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Convex Optimization

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OptimizationProbability·Captain: mikedeng1

A Block Successive Upper-Bound Minimization Method of Multipliers for Linearly Constrained Convex Optimization 2: Randomized BSUM-M Converges to Primal-Dual Optimal Solutions Almost SurelyResearch Paper

Motivation

Many large convex problems in signal processing, networking and statistics have a separable objective coupled by linear constraints: KKK blocks of variables, each with its own nonsmooth regularizer and its own feasible set, tied together by ∑kEkxk=q\sum_k E_kx_k=q∑k​Ek​xk​=q. The alternating direction method of multipliers (ADMM) is the standard tool for such problems when K=2K=2K=2. For K≥3K\ge3K≥3 the direct extension of ADMM can diverge, as shown by Chen, He, Ye and Yuan (2016), and convergence guarantees for multi-block variants typically require strong convexity or extra correction steps.

Hong, Chang, Wang, Razaviyayn, Ma and Luo propose the block successive upper-bound minimization method of multipliers (BSUM-M), which updates each primal block by minimizing a local upper bound of the augmented Lagrangian, followed by a dual gradient step, and prove that it converges for any number of blocks without strong convexity of the objective. They also analyse a randomized version, RBSUM-M, in which each iteration updates a single randomly chosen block, primal or dual. Randomized block selection matters when data or computation are distributed and not every block is available at every step. This mission formalizes the randomized half of their main theorem; the cyclic half is a separate mission.

Setting

Let x=(x1,…,xK)x=(x_1,\dots,x_K)x=(x1​,…,xK​) with xk∈Rnkx_k\in\mathbb R^{n_k}xk​∈Rnk​, and consider

min⁡x f(x)=g(x)+∑k=1Khk(xk)s.t.Ex=∑k=1KEkxk=q,xk∈Xk.(1.1)\min_x\ f(x)=g(x)+\sum_{k=1}^K h_k(x_k)\quad\text{s.t.}\quad Ex=\sum_{k=1}^K E_kx_k=q,\quad x_k\in X_k. \tag{1.1}xmin​ f(x)=g(x)+k=1∑K​hk​(xk​)s.t.Ex=k=1∑K​Ek​xk​=q,xk​∈Xk​.(1.1)

The standing assumptions (Assumption A) are: g(x)=ℓ(Ax)+⟨x,b⟩g(x)=\ell(Ax)+\langle x,b\rangleg(x)=ℓ(Ax)+⟨x,b⟩ with ℓ\ellℓ strictly convex and continuously differentiable; hk(xk)=λk∥xk∥1+∑JwJ∥xk,J∥2h_k(x_k)=\lambda_k\|x_k\|_1+\sum_J w_J\|x_{k,J}\|_2hk​(xk​)=λk​∥xk​∥1​+∑J​wJ​∥xk,J​∥2​ with nonnegative weights; each Xk={xk∣Ckxk≤ck}X_k=\{x_k\mid C_kx_k\le c_k\}Xk​={xk​∣Ck​xk​≤ck​} is a compact polyhedron; the problem is feasible and its primal and dual optimal values are attained.

For ρ>0\rho>0ρ>0 the augmented Lagrangian and augmented dual function are

L(x;y)=f(x)+⟨y,q−Ex⟩+ρ2∥q−Ex∥2,d(y)=min⁡x∈XL(x;y),L(x;y)=f(x)+\langle y,q-Ex\rangle+\frac\rho2\|q-Ex\|^2,\qquad d(y)=\min_{x\in X}L(x;y),L(x;y)=f(x)+⟨y,q−Ex⟩+2ρ​∥q−Ex∥2,d(y)=x∈Xmin​L(x;y),

and X(y)X(y)X(y) is the set of minimizers of L(⋅;y)L(\cdot;y)L(⋅;y) over X=∏kXkX=\prod_kX_kX=∏k​Xk​. The method works with approximation functions uk(vk;x)u_k(v_k;x)uk​(vk​;x) (Assumption B): uk(⋅;x)u_k(\cdot;x)uk​(⋅;x) majorizes g+ρ2∥E⋅−q∥2g+\frac\rho2\|E\cdot-q\|^2g+2ρ​∥E⋅−q∥2 in block kkk, touches it with matching gradient at xkx_kxk​, is strongly convex with modulus γk\gamma_kγk​ and has an LkL_kLk​-Lipschitz gradient.

RBSUM-M. Fix probabilities p0,…,pK>0p_0,\dots,p_K>0p0​,…,pK​>0 summing to 1. At iteration t≥1t\ge1t≥1 draw kkk with probability pkp_kpk​. If k=0k=0k=0, take a dual step yt+1=yt+αt(q−Ext)y^{t+1}=y^t+\alpha^t(q-Ex^t)yt+1=yt+αt(q−Ext); otherwise replace block kkk by

xkt+1=arg⁡min⁡xk∈Xk uk(xk;xt)−⟨yt,Ekxk⟩+hk(xk),x_k^{t+1}=\arg\min_{x_k\in X_k}\ u_k(x_k;x^t)-\langle y^t,E_kx_k\rangle+h_k(x_k),xkt+1​=argxk​∈Xk​min​ uk​(xk​;xt)−⟨yt,Ek​xk​⟩+hk​(xk​),

leaving the other blocks and yyy unchanged. The analysis uses the block steps x^kt+1\hat x_k^{t+1}x^kt+1​ (the minimizer above, computed for every kkk), the dual step y^t+1=yt+αt(q−Ext)\hat y^{t+1}=y^t+\alpha^t(q-Ex^t)y^​t+1=yt+αt(q−Ext), the gaps Δdt=d∗−d(yt)\Delta_d^t=d^*-d(y^t)Δdt​=d∗−d(yt), Δpt=L(xt;yt)−d(yt)\Delta_p^t=L(x^t;y^t)-d(y^t)Δpt​=L(xt;yt)−d(yt), and the proximal gradient ∇~xL(x;y)=x−prox⁡h+ιX(x−∇x(L(x;y)−h(x)))\tilde\nabla_xL(x;y)=x-\operatorname{prox}_{h+\iota_X}\big(x-\nabla_x(L(x;y)-h(x))\big)∇~x​L(x;y)=x−proxh+ιX​​(x−∇x​(L(x;y)−h(x))). The error bound with constant τ\tauτ is dist⁡(x,X(y))≤τ∥∇~xL(x;y)∥\operatorname{dist}(x,X(y))\le\tau\|\tilde\nabla_xL(x;y)\|dist(x,X(y))≤τ∥∇~x​L(x;y)∥ for all yyy and x∈Xx\in Xx∈X.

Formalization targets

Goal: Theorem 2.1, part 2

Under Assumptions A and B and the error bound, if the stepsizes are either constant and sufficiently small, or satisfy ∑tαt=∞\sum_t\alpha^t=\infty∑t​αt=∞, αt→0\alpha^t\to0αt→0, then with probability 1

∥Ext−q∥→0,∥xt−xt+1∥→0,∥xt−xˉt∥→0,\|Ex^t-q\|\to0,\qquad\|x^t-x^{t+1}\|\to0,\qquad\|x^t-\bar x^t\|\to0,∥Ext−q∥→0,∥xt−xt+1∥→0,∥xt−xˉt∥→0,

where xˉt\bar x^txˉt is the point of X(y^t)X(\hat y^t)X(y^​t) nearest to xtx^txt, and every limit point of (xt,yt)(x^t,y^t)(xt,yt) is a primal and dual optimal pair. The threshold for "sufficiently small" is existential and depends only on the problem data, the uku_kuk​, the error-bound constant and ppp.

Milestones

In the order of the paper: Lemma 2.1 (differentiability of ddd, ∇d(y)=q−Ex(y)\nabla d(y)=q-Ex(y)∇d(y)=q−Ex(y), the 1/ρ1/\rho1/ρ-Lipschitz bound); Lemma 2.3(2) (expected decrease of LLL); Lemma 2.4(2) (proximal gradient bounded by the block and dual steps); Lemmas 2.5(2) and 2.6(2) (expected change of the dual and primal gaps); and from the proof of Theorem 2.1, (2.24)–(2.25) (expected change of Δp+Δd\Delta_p+\Delta_dΔp​+Δd​), (2.28) (constraint violation), (2.29) (the descent estimate with explicit coefficients) and (2.40) (one-step change of ∥Exˉt−q∥\|E\bar x^t-q\|∥Exˉt−q∥).

Significance

The result shows that a randomized, single-block-per-iteration primal-dual method converges almost surely to primal-dual optimal solutions of a multi-block linearly constrained problem, under assumptions that allow a rank-deficient AAA, nonsmooth group-sparse regularizers, and inexact (majorized) block subproblems. The potential function Δp+Δd\Delta_p+\Delta_dΔp​+Δd​ and the way the error bound converts it into a supermartingale estimate are reused in later analyses of multi-block and randomized ADMM-type methods.

The result is proved in the paper; to our knowledge it has no machine-checked proof. Formalizing it produces a checked convergence proof for a randomized augmented-Lagrangian method, a reusable formal treatment of the augmented dual function of a convex program with compact polyhedral constraints, and a precise record of the conventions under which the published statements hold (see the scope section).

Difficulty

The obvious route is to show that L(xt;yt)L(x^t;y^t)L(xt;yt) decreases. It does not: a dual step increases LLL by αt∥q−Ext∥2\alpha^t\|q-Ex^t\|^2αt∥q−Ext∥2, and without strong convexity there is no direct control of the distance to the solution set. The argument has to combine the primal and dual gaps into one potential, bound the residual term ∥Ext−Exˉt+1∥\|Ex^t-E\bar x^{t+1}\|∥Ext−Exˉt+1∥ through an error bound that holds without strong convexity, and then pass from a conditional-expectation inequality to almost-sure convergence. Under diminishing stepsizes the supermartingale argument only yields lim inf⁡∥Exˉt−q∥=0\liminf\|E\bar x^t-q\|=0liminf∥Exˉt−q∥=0, and upgrading this to a limit needs a separate pathwise argument on how fast ∇d(y^t)\nabla d(\hat y^t)∇d(y^​t) can move.

Formalization scope

Blocks are EuclideanSpace ℝ (Fin (n k)) and the full vector lives in PiLp 2, so norms are Euclidean. ℓ\ellℓ is real-valued on all of Rp\mathbb R^pRp. The augmented dual function is d(y)=min⁡x∈XL(x;y)d(y)=\min_{x\in X}L(x;y)d(y)=minx∈X​L(x;y) (the page's (1.9) prints an unconstrained minimum of ggg plus penalty; the constrained reading is the one Lemma 2.1 and (2.19) use). The prox in the proximal gradient includes the constraint set XXX, which is what the proof of Lemma 2.4 needs; the error bound of Lemma 2.2 is a hypothesis of the goal, in its global form on XXX, and is not derived. Lemma 2.2 itself is not part of the mission.

Conditional expectations given zt=(xt,yt)z^t=(x^t,y^t)zt=(xt,yt) are written as the explicit average p0F(x,y^)+∑kpkF((x^k,x−k),y)p_0F(x,\hat y)+\sum_kp_kF((\hat x_k,x_{-k}),y)p0​F(x,y^​)+∑k​pk​F((x^k​,x−k​),y) over the random index, at every state; this is E[F(zt+1)∣zt]\mathbb E[F(z^{t+1})\mid z^t]E[F(zt+1)∣zt] because the index drawn at iteration ttt is independent of ztz^tzt. The goal is stated on an arbitrary probability space carrying mutually independent indices with law ppp, for every run from a deterministic start x1∈Xx^1\in Xx1∈X, y1y^1y1. Iterations are indexed from t=1t=1t=1 as on the page.

Two printed statements are corrected and labelled in their items: Lemma 2.1 asserts AxAxAx (not each AkxkA_kx_kAk​xk​) constant over X(y)X(y)X(y), and Lemma 2.6(2) uses αt\alpha^tαt where the page prints αr\alpha^rαr. Statements are not trivialized: the setting is satisfiable (for instance K=1K=1K=1, g≡0g\equiv0g≡0, h=0h=0h=0, E=0E=0E=0, X=[−1,1]X=[-1,1]X=[−1,1], u(v;x)=(v−x1)2/2u(v;x)=(v-x_1)^2/2u(v;x)=(v−x1​)2/2), the stepsize threshold precedes the probability space and the run, and the solution sets entering distances are nonempty under Assumption A. A formalization in which the error bound or the gap bounds are assumed in a form that already contains the conclusion would not count.

A complete development needs: Danskin-type differentiability of ddd and the 1/ρ1/\rho1/ρ-smoothness of the augmented dual; first-order optimality and nonexpansiveness of the prox of h+ιXh+\iota_Xh+ιX​; and the Robbins–Siegmund almost-supermartingale convergence theorem in Mathlib's conditional expectation framework, together with a bridge from the explicit index average to condExp. The last two are reusable well beyond this mission. Contributions to any of the milestones, or to these general lemmas, are welcome.

Selected references

  • M. Hong, T.-H. Chang, X. Wang, M. Razaviyayn, S. Ma, Z.-Q. Luo, A Block Successive Upper Bound Minimization Method of Multipliers for Linearly Constrained Convex Optimization, arXiv:1401.7079v1, 2014; Mathematics of Operations Research 45(3), 2020. https://arxiv.org/abs/1401.7079, https://doi.org/10.1287/moor.2019.1010
  • M. Hong, Z.-Q. Luo, On the linear convergence of the alternating direction method of multipliers, Mathematical Programming 162, 2017. https://doi.org/10.1007/s10107-016-1034-2
  • C. Chen, B. He, Y. Ye, X. Yuan, The direct extension of ADMM for multi-block convex minimization problems is not necessarily convergent, Mathematical Programming 155, 2016. https://doi.org/10.1007/s10107-014-0826-5
  • H. Robbins, D. Siegmund, A convergence theorem for non negative almost supermartingales and some applications, in Optimizing Methods in Statistics, Academic Press, 1971. https://doi.org/10.1016/B978-0-12-604550-5.50015-8
  • M. Razaviyayn, M. Hong, Z.-Q. Luo, A unified convergence analysis of block successive minimization methods for nonsmooth optimization, SIAM Journal on Optimization 23(2), 2013. https://doi.org/10.1137/120891009

Theorem numbers, equation numbers and page numbers in this mission refer to arXiv:1401.7079v1 (printed page = PDF page − 1); the journal version renumbers them.

12 thms1 active userReviewed
Optimization·Captain: mikedeng1

A Block Successive Upper-Bound Minimization Method of Multipliers for Linearly Constrained Convex Optimization 1: Cyclic BSUM-M Converges to Primal-Dual Optimal SolutionsResearch Paper

Motivation

Many problems in signal processing, machine learning and power systems have the form of a convex objective that is a sum of a smooth coupled term and nonsmooth block-separable terms, minimized subject to linear equality constraints that couple KKK blocks of variables: basis pursuit, demand response control in smart grids, and distributed estimation are the examples of Hong, Chang, Wang, Razaviyayn, Ma, Luo. The alternating direction method of multipliers (ADMM) handles two blocks well, but for K≥3K\ge3K≥3 blocks the directly extended Gauss–Seidel ADMM can diverge (Chen, He, Ye, Yuan, 2016), and convergence proofs for multi-block schemes usually need strong convexity or extra correction steps.

The block successive upper-bound minimization method of multipliers (BSUM-M) is the paper's answer: each block is updated by minimizing a local upper bound of the augmented Lagrangian, which makes the subproblems simple (for instance closed-form proximal steps), and the multiplier is updated by a dual gradient step with a small or diminishing stepsize. The main theorem shows that this scheme converges to primal and dual optimal solutions for any number of blocks without strong convexity, under an error bound.

Setting

The variable is x=(x1,…,xK)x=(x_1,\dots,x_K)x=(x1​,…,xK​), xk∈Rnkx_k\in\mathbb R^{n_k}xk​∈Rnk​, with the Euclidean norm ∥x∥2=∑k∥xk∥2\|x\|^2=\sum_k\|x_k\|^2∥x∥2=∑k​∥xk​∥2. Problem (1.1) is

min⁡x f(x)=g(x)+∑k=1Khk(xk)s.t.Ex=∑k=1KEkxk=q,xk∈Xk.\min_x\ f(x)=g(x)+\sum_{k=1}^K h_k(x_k)\quad\text{s.t.}\quad Ex=\sum_{k=1}^KE_kx_k=q,\quad x_k\in X_k .xmin​ f(x)=g(x)+k=1∑K​hk​(xk​)s.t.Ex=k=1∑K​Ek​xk​=q,xk​∈Xk​.

Under the standing Assumption A, g(x)=ℓ(Ax)+⟨x,b⟩g(x)=\ell(Ax)+\langle x,b\rangleg(x)=ℓ(Ax)+⟨x,b⟩ with ℓ\ellℓ strictly convex and continuously differentiable and AAA any matrix; hk(xk)=λk∥xk∥1+∑JwJ∥xk,J∥2h_k(x_k)=\lambda_k\|x_k\|_1+\sum_Jw_J\|x_{k,J}\|_2hk​(xk​)=λk​∥xk​∥1​+∑J​wJ​∥xk,J​∥2​ is a mixed ℓ1/ℓ2\ell_1/\ell_2ℓ1​/ℓ2​ norm with nonnegative weights; each Xk={xk∣Ckxk≤ck}X_k=\{x_k\mid C_kx_k\le c_k\}Xk​={xk​∣Ck​xk​≤ck​} is a compact polyhedron and X=∏kXkX=\prod_kX_kX=∏k​Xk​; the problem is feasible and the dual optimal value is attained.

For ρ>0\rho>0ρ>0, the augmented Lagrangian is L(x;y)=f(x)+⟨y,q−Ex⟩+ρ2∥q−Ex∥2L(x;y)=f(x)+\langle y,q-Ex\rangle+\frac\rho2\|q-Ex\|^2L(x;y)=f(x)+⟨y,q−Ex⟩+2ρ​∥q−Ex∥2, the augmented dual is d(y)=min⁡x∈XL(x;y)d(y)=\min_{x\in X}L(x;y)d(y)=minx∈X​L(x;y), and X(y)=arg⁡min⁡x∈XL(x;y)X(y)=\arg\min_{x\in X}L(x;y)X(y)=argminx∈X​L(x;y). For x∈Xx\in Xx∈X, xˉ\bar xxˉ denotes the point of X(y)X(y)X(y) nearest to xxx.

Assumption B concerns the approximation functions uk(vk;x)u_k(v_k;x)uk​(vk​;x): each upper-bounds G(x)=g(x)+ρ2∥Ex−q∥2G(x)=g(x)+\frac\rho2\|Ex-q\|^2G(x)=g(x)+2ρ​∥Ex−q∥2 along block kkk, is tight with matching gradient at vk=xkv_k=x_kvk​=xk​, is continuous, strongly convex in vkv_kvk​ with a uniform modulus γk>0\gamma_k>0γk​>0, and has an LkL_kLk​-Lipschitz gradient in vkv_kvk​.

BSUM-M (1.12). From x1∈Xx^1\in Xx1∈X and any y1y^1y1, for r≥1r\ge1r≥1:

yr+1=yr+αr(q−Exr),xkr+1=arg⁡min⁡xk∈Xkuk(xk;wkr+1)−⟨yr+1,Ekxk⟩+hk(xk),y^{r+1}=y^r+\alpha^r(q-Ex^r),\qquad x_k^{r+1}=\arg\min_{x_k\in X_k}u_k(x_k;w_k^{r+1})-\langle y^{r+1},E_kx_k\rangle+h_k(x_k),yr+1=yr+αr(q−Exr),xkr+1​=argxk​∈Xk​min​uk​(xk​;wkr+1​)−⟨yr+1,Ek​xk​⟩+hk​(xk​),

for k=1,…,Kk=1,\dots,Kk=1,…,K in order, with the Gauss–Seidel point wkr+1=(x1r+1,…,xk−1r+1,xkr,…,xKr)w_k^{r+1}=(x_1^{r+1},\dots,x_{k-1}^{r+1},x_k^r,\dots,x_K^r)wkr+1​=(x1r+1​,…,xk−1r+1​,xkr​,…,xKr​).

The proximal gradient is ∇~xL(x;y)=x−prox⁡(x−∇x(L(x;y)−h(x)))\tilde\nabla_xL(x;y)=x-\operatorname{prox}(x-\nabla_x(L(x;y)-h(x)))∇~x​L(x;y)=x−prox(x−∇x​(L(x;y)−h(x))) with prox⁡(z)=arg⁡min⁡u∈Xh(u)+12∥z−u∥2\operatorname{prox}(z)=\arg\min_{u\in X}h(u)+\frac12\|z-u\|^2prox(z)=argminu∈X​h(u)+21​∥z−u∥2. The error bound asks for τ>0\tau>0τ>0 with dist⁡(x,X(y))≤τ∥∇~xL(x;y)∥\operatorname{dist}(x,X(y))\le\tau\|\tilde\nabla_xL(x;y)\|dist(x,X(y))≤τ∥∇~x​L(x;y)∥ for all x∈Xx\in Xx∈X and all yyy.

Formalization targets

Goal: Theorem 2.1, part 1

Under Assumptions A and B and the error bound, there is αˉ>0\bar\alpha>0αˉ>0 such that for stepsizes αr>0\alpha^r>0αr>0 that are either constant with αr=α≤αˉ\alpha^r=\alpha\le\bar\alphaαr=α≤αˉ, or satisfy ∑rαr=∞\sum_r\alpha^r=\infty∑r​αr=∞ and αr→0\alpha^r\to0αr→0, every BSUM-M run satisfies

lim⁡r→∞∥Exr−q∥=0,lim⁡r→∞∥xr−xr+1∥=0,lim⁡r→∞∥xr−xˉr∥=0,\lim_{r\to\infty}\|Ex^r-q\|=0,\qquad\lim_{r\to\infty}\|x^r-x^{r+1}\|=0,\qquad\lim_{r\to\infty}\|x^r-\bar x^r\|=0,r→∞lim​∥Exr−q∥=0,r→∞lim​∥xr−xr+1∥=0,r→∞lim​∥xr−xˉr∥=0,

and every limit point of {(xr,yr)}\{(x^r,y^r)\}{(xr,yr)} is a primal and dual optimal solution. The threshold αˉ\bar\alphaαˉ is not specified; no rate is claimed.

Milestones

Lemma 2.3(1) (one sweep decreases L(⋅;yr+1)L(\cdot;y^{r+1})L(⋅;yr+1) by γ∥xr−xr+1∥2\gamma\|x^r-x^{r+1}\|^2γ∥xr−xr+1∥2), Lemma 2.5(1) (dual gap decrease), Lemma 2.6(1) (primal gap bound), Lemma 2.4(1) (the proximal gradient at xrx^rxr is O(∥xr+1−xr∥)O(\|x^{r+1}-x^r\|)O(∥xr+1−xr∥)) and Lemma 2.1 (differentiability of ddd, ∇d(y)=q−Ex(y)\nabla d(y)=q-Ex(y)∇d(y)=q−Ex(y), and Lipschitz continuity of ∇d\nabla d∇d on superlevel sets).

Significance

The theorem gives a convergent multi-block method of multipliers whose block subproblems may be replaced by any majorizer satisfying Assumption B, such as a linearized proximal step. It covers the cyclic Gauss–Seidel order, where the direct multi-block ADMM can fail, and it does not require strong convexity of fff (the matrix AAA need not have full column rank). The paper's randomized variant (part 2 of the same theorem) is a separate mission.

The result is proved in the paper (the proof of part 1 is described as following the steps written out for part 2). It has not been machine-checked. Formalization adds a verified account of the potential-function argument for a primal-dual method with inexact block updates, and checks three printed statements that need correction (see the scope section): a formal proof settles them.

Difficulty

The obvious approach is to treat BSUM-M as an inexact dual gradient ascent on ddd, but a single Gauss–Seidel sweep does not compute x(yr+1)∈X(yr+1)x(y^{r+1})\in X(y^{r+1})x(yr+1)∈X(yr+1), so the dual step uses a gradient at the wrong point. Controlling that error requires relating the primal step length to the distance from X(y)X(y)X(y), which fails without an error bound: L(⋅;y)L(\cdot;y)L(⋅;y) is not strongly convex, X(y)X(y)X(y) need not be a singleton, and the proximal gradient can be small far from X(y)X(y)X(y). The cyclic order adds a second gap: block kkk is linearized at wkr+1w_k^{r+1}wkr+1​, not at xrx^rxr. With a constant stepsize the dual ascent must not outrun the primal descent, which is where the smallness threshold enters.

Formalization scope

Citation basis: the arXiv preprint arXiv:1401.7079v1 (28 Jan 2014); every index refers to that version, not to the revised journal version (Mathematics of Operations Research, 2020).

Representation: blocks are indexed by Fin K with K≥1K\ge1K≥1; the block space is PiLp 2 of Euclidean spaces (the Euclidean norm, not the sup norm). ℓ\ellℓ is real valued and C1C^1C1 on all of Rp\mathbb R^pRp, which specializes the paper's extended-valued ℓ\ellℓ. ddd, d∗d^*d∗ and f∗f^*f∗ are real infima and suprema over nonempty compact sets, where they are attained. The algorithm is a predicate on sequences indexed from r=1r=1r=1; argmin steps are minimality conditions, the minimizer being unique. The initial point is required to lie in XXX. "Sufficiently small" is an existential threshold quantified before the stepsizes and the run. ∥xr−xˉr∥\|x^r-\bar x^r\|∥xr−xˉr∥ is the distance from xrx^rxr to X(yr)X(y^r)X(yr). Limit points are cluster points of the joint sequence; boundedness of {yr}\{y^r\}{yr} is neither assumed nor concluded.

Interpretations and corrections, each labelled in the item's statement:

  • the proximity operator in (2.3) includes the constraint set XXX, as the paper's optimality relation (2.14) requires;
  • d(y)d(y)d(y) is min⁡x∈XL(x;y)\min_{x\in X}L(x;y)minx∈X​L(x;y); (1.9) prints g(x)g(x)g(x) and an unconstrained minimum;
  • (2.17) has ExrEx^rExr where its proof (2.19) has Exr−1Ex^{r-1}Exr−1; the proved inequality is stated;
  • (2.12) evaluates the proximal gradient at yry^ryr and is false at r=1r=1r=1; it is stated at yr+1y^{r+1}yr+1;
  • Lemma 2.1's clause "AkxkA_kx_kAk​xk​ constant on X(y)X(y)X(y)" fails for non-separable ℓ\ellℓ; it is stated as "AxAxAx constant".

The error bound is a hypothesis of the goal, as in the paper, and is not derived from Assumption A: the paper's Lemma 2.2 does not hold under Assumption A alone. A formalization that makes the hypotheses unsatisfiable, drops the run's dependence on yr+1y^{r+1}yr+1, or lets αˉ\bar\alphaαˉ depend on the run is not this theorem. A sanity check that the hypotheses are satisfiable (a one-block instance with a constant run) is part of the drafting record.

Infrastructure needed: proximity operators of convex functions restricted to polyhedra and their nonexpansiveness; Danskin-type differentiability of a parametric minimum over a compact set; smoothness of the augmented dual; elementary convergence lemmas for nonnegative sequences with summable decrements. These pieces are reusable for other augmented Lagrangian and ADMM analyses. Proofs of the milestones are welcome independently of the goal.

Selected references

  • M. Hong, T.-H. Chang, X. Wang, M. Razaviyayn, S. Ma, Z.-Q. Luo, A Block Successive Upper Bound Minimization Method of Multipliers for Linearly Constrained Convex Optimization, arXiv:1401.7079v1, 2014; Mathematics of Operations Research 45(3), 2020. https://arxiv.org/abs/1401.7079 , https://doi.org/10.1287/moor.2019.1010
  • M. Hong, Z.-Q. Luo, On the linear convergence of the alternating direction method of multipliers, Mathematical Programming 162, 2017. https://doi.org/10.1007/s10107-016-1034-2
  • M. Razaviyayn, M. Hong, Z.-Q. Luo, A unified convergence analysis of block successive minimization methods for nonsmooth optimization, SIAM Journal on Optimization 23(2), 2013. https://doi.org/10.1137/120891009
  • C. Chen, B. He, Y. Ye, X. Yuan, The direct extension of ADMM for multi-block convex minimization problems is not necessarily convergent, Mathematical Programming 155, 2016. https://doi.org/10.1007/s10107-014-0826-5
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Operations ResearchOptimizationStatistics·Captain: mikedeng1

Sparse Regression at Scale: Branch-and-Bound rooted in First-Order Optimization 5: Dual Bounds from Active-Set Primal Solutions Lose Only O(kε), Independent of pResearch Paper

Motivation

Best-subset selection with ridge shrinkage, min⁡β12∥y−Xβ∥22+λ0∥β∥0+λ2∥β∥22\min_\beta \tfrac12\|y-X\beta\|_2^2+\lambda_0\|\beta\|_0+\lambda_2\|\beta\|_2^2minβ​21​∥y−Xβ∥22​+λ0​∥β∥0​+λ2​∥β∥22​, is a mixed-integer program that statisticians want to solve to certified optimality at the scale of modern data (ppp up to 10710^7107 features). Hazimeh, Mazumder and Saab (arXiv:2004.06152, Mathematical Programming 2022) built a branch-and-bound solver, L0BnB, whose node relaxations are solved in the primal space by active-set coordinate descent instead of by an interior-point method. Branch-and-bound prunes a node only with a valid dual bound, a certified lower bound on the node's relaxation value. A primal method returns an approximate minimizer, not such a bound, so the solver must turn an inexact primal point into a dual feasible point and needs to know how much is lost in doing so. This mission formalizes the paper's answer, its main theorem (Theorem 3).

Setting

Data are X∈Rn×pX\in\mathbb R^{n\times p}X∈Rn×p with columns X1,…,XpX_1,\dots,X_pX1​,…,Xp​, y∈Rny\in\mathbb R^ny∈Rn, and parameters λ0,λ2,M>0\lambda_0,\lambda_2,M>0λ0​,λ2​,M>0. The reverse Huber penalty is B(t)=∣t∣\mathcal B(t)=|t|B(t)=∣t∣ for ∣t∣≤1|t|\le1∣t∣≤1 and (t2+1)/2(t^2+1)/2(t2+1)/2 for ∣t∣≥1|t|\ge1∣t∣≥1. The penalty ψ(b)\psi(b)ψ(b) equals ψ1(b)=2λ0B(bλ2/λ0)\psi_1(b)=2\lambda_0\mathcal B(b\sqrt{\lambda_2/\lambda_0})ψ1​(b)=2λ0​B(bλ2​/λ0​​) if λ0/λ2≤M\sqrt{\lambda_0/\lambda_2}\le Mλ0​/λ2​​≤M and ψ2(b)=(λ0/M+λ2M)∣b∣\psi_2(b)=(\lambda_0/M+\lambda_2M)|b|ψ2​(b)=(λ0​/M+λ2​M)∣b∣ otherwise. The reduced relaxation (5) is

min⁡β∈Rp F(β)=12∥y−Xβ∥22+∑iψ(βi)s.t.∥β∥∞≤M.\min_{\beta\in\mathbb R^p}\ F(\beta)=\tfrac12\|y-X\beta\|_2^2+\sum_{i}\psi(\beta_i)\quad\text{s.t.}\quad \|\beta\|_\infty\le M .β∈Rpmin​ F(β)=21​∥y−Xβ∥22​+i∑​ψ(βi​)s.t.∥β∥∞​≤M.

Throughout, the columns of XXX and yyy have unit ℓ2\ell_2ℓ2​ norm (the standing assumption of Section 3 of the paper).

Algorithm 2 (active-set coordinate descent) returns a point β^\hat\betaβ^​ in the box such that the set

V={i∉Supp⁡(β^): 0≠arg min⁡∣t∣≤MF(β^1,…,t,…,β^p)}V=\{i\notin\operatorname{Supp}(\hat\beta):\ 0\ne\operatorname*{arg\,min}_{|t|\le M}F(\hat\beta_1,\dots,t,\dots,\hat\beta_p)\}V={i∈/Supp(β^​): 0=∣t∣≤Margmin​F(β^​1​,…,t,…,β^​p​)}

is empty: no coordinate outside the support wants to move. Write r^=y−Xβ^\hat r=y-X\hat\betar^=y−Xβ^​, k=∥β^∥0k=\|\hat\beta\|_0k=∥β^​∥0​, and let β∗\beta^*β∗ be an optimal solution of (5) with r∗=y−Xβ∗r^*=y-X\beta^*r∗=y−Xβ∗. The primal gap is ϵ=∥X(β∗−β^)∥2\epsilon=\|X(\beta^*-\hat\beta)\|_2ϵ=∥X(β∗−β^​)∥2​.

The two duals of (5) (Theorem 2 of the paper) are, with v(α,γi)=[(α⊤Xi−γi)2/(4λ2)−λ0]++M∣γi∣v(\alpha,\gamma_i)=[(\alpha^\top X_i-\gamma_i)^2/(4\lambda_2)-\lambda_0]_++M|\gamma_i|v(α,γi​)=[(α⊤Xi​−γi​)2/(4λ2​)−λ0​]+​+M∣γi​∣,

h1(α,γ)=−12∥α∥22−α⊤y−∑iv(α,γi),h2(ρ,μ)=−12∥ρ∥22−ρ⊤y−M∥μ∥1,h_1(\alpha,\gamma)=-\tfrac12\|\alpha\|_2^2-\alpha^\top y-\textstyle\sum_i v(\alpha,\gamma_i),\qquad h_2(\rho,\mu)=-\tfrac12\|\rho\|_2^2-\rho^\top y-M\|\mu\|_1,h1​(α,γ)=−21​∥α∥22​−α⊤y−∑i​v(α,γi​),h2​(ρ,μ)=−21​∥ρ∥22​−ρ⊤y−M∥μ∥1​,

the latter under ∣ρ⊤Xi∣−μi≤λ0/M+λ2M|\rho^\top X_i|-\mu_i\le\lambda_0/M+\lambda_2M∣ρ⊤Xi​∣−μi​≤λ0​/M+λ2​M. The dual variables built from β∗\beta^*β∗ are α∗=ρ∗=−r∗\alpha^*=\rho^*=-r^*α∗=ρ∗=−r∗, γi∗=1[∣βi∗∣=M](α∗⊤Xi−2Mλ2sign⁡(α∗⊤Xi))\gamma^*_i=\mathbb 1_{[|\beta^*_i|=M]}(\alpha^{*\top}X_i-2M\lambda_2\operatorname{sign}(\alpha^{*\top}X_i))γi∗​=1[∣βi∗​∣=M]​(α∗⊤Xi​−2Mλ2​sign(α∗⊤Xi​)) and μi∗=1[∣βi∗∣=M](∣ρ∗⊤Xi∣−λ0/M−λ2M)\mu^*_i=\mathbb 1_{[|\beta^*_i|=M]}(|\rho^{*\top}X_i|-\lambda_0/M-\lambda_2M)μi∗​=1[∣βi∗​∣=M]​(∣ρ∗⊤Xi​∣−λ0​/M−λ2​M). The dual points built from β^\hat\betaβ^​ are α^=ρ^=−r^\hat\alpha=\hat\rho=-\hat rα^=ρ^​=−r^, with γ^\hat\gammaγ^​ a maximizer of h1(α^,⋅)h_1(\hat\alpha,\cdot)h1​(α^,⋅) (25) and μ^\hat\muμ^​ a maximizer of h2(ρ^,⋅)h_2(\hat\rho,\cdot)h2​(ρ^​,⋅) under the constraints (27).

Formalization targets

Goal: Theorem 3 with the proof's constants

If λ0/λ2≤M\sqrt{\lambda_0/\lambda_2}\le Mλ0​/λ2​​≤M, with ci=(2λ2)−1c_i=(2\lambda_2)^{-1}ci​=(2λ2​)−1 when ∣βi∗∣<M|\beta^*_i|<M∣βi∗​∣<M and ci=Mc_i=Mci​=M when ∣βi∗∣=M|\beta^*_i|=M∣βi∗​∣=M,

h1(α^,γ^) ≥ h1(α∗,γ∗)−2ϵ−12ϵ2−∑i∈Supp⁡(β^)(ciϵ+(4λ2)−1ϵ2).(55)h_1(\hat\alpha,\hat\gamma)\ \ge\ h_1(\alpha^*,\gamma^*)-2\epsilon-\tfrac12\epsilon^2-\sum_{i\in\operatorname{Supp}(\hat\beta)}\big(c_i\epsilon+(4\lambda_2)^{-1}\epsilon^2\big).\qquad(55)h1​(α^,γ^​) ≥ h1​(α∗,γ∗)−2ϵ−21​ϵ2−i∈Supp(β^​)∑​(ci​ϵ+(4λ2​)−1ϵ2).(55)

If λ0/λ2>M\sqrt{\lambda_0/\lambda_2}>Mλ0​/λ2​​>M,

h2(ρ^,μ^) ≥ h2(ρ∗,μ∗)−ϵ(2+Mk)−12ϵ2.(59)h_2(\hat\rho,\hat\mu)\ \ge\ h_2(\rho^*,\mu^*)-\epsilon(2+Mk)-\tfrac12\epsilon^2.\qquad(59)h2​(ρ^​,μ^​) ≥ h2​(ρ∗,μ∗)−ϵ(2+Mk)−21​ϵ2.(59)

The paper states these as −kO(ϵ)−kO(ϵ2)-kO(\epsilon)-kO(\epsilon^2)−kO(ϵ)−kO(ϵ2) (29) and −kO(ϵ)−O(ϵ2)-kO(\epsilon)-O(\epsilon^2)−kO(ϵ)−O(ϵ2) (30); the goal states the expressions its proof establishes.

Milestones

In the order the proof uses them: the closed-form coordinate updates (14) and (15); Proposition 3, V={i∉Supp⁡(β^):∣⟨r^,Xi⟩∣>c(λ0,λ2,M)}V=\{i\notin\operatorname{Supp}(\hat\beta): |\langle\hat r,X_i\rangle|>c(\lambda_0,\lambda_2,M)\}V={i∈/Supp(β^​):∣⟨r^,Xi​⟩∣>c(λ0​,λ2​,M)}; the bound ∥α∗∥2≤1\|\alpha^*\|_2\le1∥α∗∥2​≤1; Lemma 2, which bounds v(α^,γ^i)v(\hat\alpha,\hat\gamma_i)v(α^,γ^​i​) coordinate by coordinate and makes it vanish off the support; inequality (53); the closed form (28) of μ^\hat\muμ^​; the optimality conditions (58); the bound (57) ∣μ^i∣≤ϵ+∣μi∗∣|\hat\mu_i|\le\epsilon+|\mu^*_i|∣μ^​i​∣≤ϵ+∣μi∗​∣ on the support; and inequality (56).

Significance

The result. In both regimes the loss of the dual bound is controlled by the primal gap times the sparsity kkk of the iterate, with constants depending only on MMM and λ2\lambda_2λ2​; the number of features ppp does not enter. Since L0BnB seeks solutions with k≪pk\ll pk≪p, the cheap dual bound obtained from an inexact primal solution is nearly as good as the exact one, which is what allows pruning without an interior-point solve at every node. The paper notes that with plain coordinate descent in place of Algorithm 2 the same argument gives ppp in place of kkk.

Formalizing it. The result is proved in the paper; it has no machine-checked proof. The mission produces a checked version of the main theorem with explicit constants, a formal model of what "output of an active-set method" means for the analysis, and reusable closed forms for the boxed soft-thresholding updates of an ℓ1\ell_1ℓ1​- or reverse-Huber-penalized box-constrained least squares problem.

Difficulty

The bound is not a consequence of weak duality alone: weak duality says only that each dual value is below the primal optimum, and says nothing about how far the constructed dual point is from the dual optimum. The obvious estimate, a Lipschitz bound on h1h_1h1​ or h2h_2h2​ summed over all coordinates, gives a loss proportional to ppp. Getting kkk instead requires showing that the dual contribution of every coordinate outside Supp⁡(β^)\operatorname{Supp}(\hat\beta)Supp(β^​) vanishes exactly, which uses the emptiness of VVV through Proposition 3 and the closed forms (14)–(15) of one-dimensional nonsmooth box-constrained problems. On the support, the loss must be bounded using the structure of γ∗\gamma^*γ∗ and μ∗\mu^*μ∗ at coordinates where β∗\beta^*β∗ hits the box, which is where ci=Mc_i=Mci​=M and (58) enter.

Formalization scope

Indices are Fin p; norms are explicit sums; sign⁡\operatorname{sign}sign is Real.sign with sign⁡(0)=0\operatorname{sign}(0)=0sign(0)=0; [a]+[a]_+[a]+​ is max a 0. The unit norms of the columns of XXX and of yyy are hypotheses, never built into the definitions, and each theorem assumes only the ones it uses. β∗\beta^*β∗ is any point of the box minimizing FFF over the box. The output of Algorithm 2 is modelled by its two properties used in the paper: ∥β^∥∞≤M\|\hat\beta\|_\infty\le M∥β^​∥∞​≤M and V=∅V=\emptysetV=∅ ("0≠arg⁡min⁡0\ne\arg\min0=argmin" encoded as "000 is not a minimizer"); the iterations are not formalized. γ^\hat\gammaγ^​ and μ^\hat\muμ^​ are arbitrary maximizers satisfying (25) and (27). The dual variables (23)–(24) are defined by their formulas; their optimality (Theorem 2, a separate mission) is neither assumed nor needed, and the goal is an inequality between explicit numbers.

Instantiations of O(⋅)O(\cdot)O(⋅). (29) is stated as (55): kO(ϵ)+kO(ϵ2)kO(\epsilon)+kO(\epsilon^2)kO(ϵ)+kO(ϵ2) becomes 2ϵ+12ϵ2+∑i∈Supp⁡(β^)(ciϵ+(4λ2)−1ϵ2)2\epsilon+\tfrac12\epsilon^2+\sum_{i\in\operatorname{Supp}(\hat\beta)}(c_i\epsilon+(4\lambda_2)^{-1}\epsilon^2)2ϵ+21​ϵ2+∑i∈Supp(β^​)​(ci​ϵ+(4λ2​)−1ϵ2) with ci∈{(2λ2)−1,M}c_i\in\{(2\lambda_2)^{-1},M\}ci​∈{(2λ2​)−1,M} decided by β∗\beta^*β∗. (30) is stated as (59): kO(ϵ)+O(ϵ2)kO(\epsilon)+O(\epsilon^2)kO(ϵ)+O(ϵ2) becomes ϵ(2+Mk)+12ϵ2\epsilon(2+Mk)+\tfrac12\epsilon^2ϵ(2+Mk)+21​ϵ2. The proof's final rearrangement of (29), which counts ∣β^i∣|\hat\beta_i|∣β^​i​∣ instead of ∣βi∗∣|\beta^*_i|∣βi∗​∣, is not used.

A formalization that takes β^=β∗\hat\beta=\beta^*β^​=β∗, γ^=γ∗\hat\gamma=\gamma^*γ^​=γ∗ or μ^=μ∗\hat\mu=\mu^*μ^​=μ∗, that drops the hypothesis V=∅V=\emptysetV=∅, or that replaces the constants by an existential "∃C\exists C∃C" would be trivial or a different statement; the goal quantifies over every optimal β∗\beta^*β∗, every box-feasible β^\hat\betaβ^​ with V=∅V=\emptysetV=∅ and every maximizer γ^\hat\gammaγ^​, μ^\hat\muμ^​, with the explicit constants above.

Needed infrastructure: one-dimensional convex minimization on an interval with piecewise penalties, Cauchy–Schwarz for finite sums, and first-order optimality conditions for box-constrained composite problems. Proofs of any milestone are welcome independently.

Selected references

  • H. Hazimeh, R. Mazumder, A. Saab, Sparse Regression at Scale: Branch-and-Bound rooted in First-Order Optimization, arXiv:2004.06152v2, 2021; Mathematical Programming 196 (2022). https://arxiv.org/abs/2004.06152
  • P. Tseng, Convergence of a block coordinate descent method for nondifferentiable minimization, J. Optim. Theory Appl. 109 (2001). https://doi.org/10.1023/A:1017501703105
  • J. Friedman, T. Hastie, R. Tibshirani, Regularization paths for generalized linear models via coordinate descent, J. Stat. Softw. 33 (2010). https://doi.org/10.18637/jss.v033.i01
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Dynamical SystemsFunctional AnalysisOperations Research+1·Captain: mikedeng1

Tikhonov Regularization of a Second Order Dynamical System with Hessian Driven Damping 3: If ∫ ε(t)/t dt = +∞, the Trajectory Converges Strongly in the Ergodic Sense to the Minimum-Norm MinimizerResearch Paper

Motivation

Second order dynamical systems with vanishing damping are continuous-time models of accelerated first-order methods. The system x¨+αtx˙+∇g(x)=0\ddot x + \frac{\alpha}{t}\dot x + \nabla g(x) = 0x¨+tα​x˙+∇g(x)=0 is the continuous limit of Nesterov's accelerated gradient method (Su, Boyd, Candès 2016), and its trajectories converge weakly to a minimizer of a convex ggg when α>3\alpha>3α>3 (Attouch, Chbani, Peypouquet, Redont 2018). Two modifications of this system have been studied separately. A Hessian-driven damping term β∇2g(x)x˙\beta\nabla^2 g(x)\dot xβ∇2g(x)x˙ damps oscillations and keeps the fast rates (Attouch, Peypouquet, Redont 2016). A Tikhonov regularization term ϵ(t)x\epsilon(t)xϵ(t)x with ϵ(t)→0\epsilon(t)\to0ϵ(t)→0 selects one minimizer, the one of minimum norm, and can turn weak convergence into strong convergence (Attouch, Chbani, Riahi 2018).

Boţ, Csetnek and László (arXiv:1911.12845v2, Math. Program. 2021) study the system with both terms. Their results split into two regimes according to how fast ϵ\epsilonϵ decays. This mission covers the slow-decay regime of §4.1, where ∫+∞ϵ(t)/t dt=+∞\int^{+\infty}\epsilon(t)/t\,dt=+\infty∫+∞ϵ(t)/tdt=+∞ and the trajectory approaches the minimum-norm minimizer in a weighted average sense.

Timeline. 2016: Su, Boyd and Candès derive the continuous model of Nesterov's method. 2016: Attouch, Peypouquet and Redont add Hessian-driven damping (α≥3\alpha\ge3α≥3, β>0\beta>0β>0) and prove fast rates and weak convergence. 2018: Attouch, Chbani and Riahi add Tikhonov regularization without Hessian damping and prove, among other results, strong ergodic convergence to the minimum-norm minimizer when ∫ϵ(t)/t dt=+∞\int\epsilon(t)/t\,dt=+\infty∫ϵ(t)/tdt=+∞. 2020: Boţ, Csetnek and László combine both terms and extend that ergodic result (their Theorem 4.2).

Setting

Let H\mathcal HH be a real Hilbert space, t0>0t_0>0t0​>0, α>0\alpha>0α>0, β≥0\beta\ge0β≥0, and u0,v0∈Hu_0,v_0\in\mathcal Hu0​,v0​∈H. The data satisfy the paper's General assumption:

  • g:H→Rg:\mathcal H\to\mathbb Rg:H→R is convex and twice Fréchet differentiable, its gradient ∇g\nabla g∇g is Lipschitz continuous on bounded sets, and argmin⁡g≠∅\operatorname{argmin} g\neq\emptysetargming=∅;
  • ϵ:[t0,+∞)→[0,+∞)\epsilon:[t_0,+\infty)\to[0,+\infty)ϵ:[t0​,+∞)→[0,+∞) is nonincreasing, of class C1C^1C1, and lim⁡t→+∞ϵ(t)=0\lim_{t\to+\infty}\epsilon(t)=0limt→+∞​ϵ(t)=0.

A global C2C^2C2-solution of system (5) is a twice continuously differentiable x:[t0,+∞)→Hx:[t_0,+\infty)\to\mathcal Hx:[t0​,+∞)→H with

x¨(t)+αtx˙(t)+β∇2g(x(t))x˙(t)+∇g(x(t))+ϵ(t)x(t)=0(t≥t0),x(t0)=u0, x˙(t0)=v0.\ddot x(t)+\frac{\alpha}{t}\dot x(t)+\beta\nabla^2 g(x(t))\dot x(t)+\nabla g(x(t))+\epsilon(t)x(t)=0\quad(t\ge t_0),\qquad x(t_0)=u_0,\ \dot x(t_0)=v_0 .x¨(t)+tα​x˙(t)+β∇2g(x(t))x˙(t)+∇g(x(t))+ϵ(t)x(t)=0(t≥t0​),x(t0​)=u0​, x˙(t0​)=v0​.

The set argmin⁡g\operatorname{argmin} gargming is nonempty, closed and convex, so it has a unique element of minimum norm, the minimum-norm minimizer x∗=argmin⁡{∥x∥:x∈argmin⁡g}x^*=\operatorname{argmin}\{\|x\|:x\in\operatorname{argmin} g\}x∗=argmin{∥x∥:x∈argming}. For ϵ>0\epsilon>0ϵ>0 the Tikhonov approximation curve is

xϵ=argmin⁡x∈H(g(x)+ϵ2∥x∥2),x_\epsilon=\operatorname*{argmin}_{x\in\mathcal H}\Big(g(x)+\frac{\epsilon}{2}\|x\|^2\Big),xϵ​=x∈Hargmin​(g(x)+2ϵ​∥x∥2),

the unique minimizer of a strongly convex function. Finally, hx∗(t)=12∥x(t)−x∗∥2h_{x^*}(t)=\tfrac12\|x(t)-x^*\|^2hx∗​(t)=21​∥x(t)−x∗∥2 measures the distance of the trajectory to x∗x^*x∗, with derivative h˙x∗(t)=⟨x˙(t),x(t)−x∗⟩\dot h_{x^*}(t)=\langle\dot x(t),x(t)-x^*\rangleh˙x∗​(t)=⟨x˙(t),x(t)−x∗⟩.

Formalization targets

Goal: Theorem 4.2 (p. 18)

If ∫t0+∞ϵ(t)t dt=+∞\int_{t_0}^{+\infty}\frac{\epsilon(t)}{t}\,dt=+\infty∫t0​+∞​tϵ(t)​dt=+∞ and α>0\alpha>0α>0, then every global C2C^2C2-solution satisfies

lim⁡t→+∞1∫t0tϵ(s)s ds∫t0tϵ(s)s∥x(s)−x∗∥2 ds=0andlim inf⁡t→+∞∥x(t)−x∗∥=0.\lim_{t\to+\infty}\frac{1}{\int_{t_0}^{t}\frac{\epsilon(s)}{s}\,ds}\int_{t_0}^{t}\frac{\epsilon(s)}{s}\|x(s)-x^*\|^2\,ds=0 \qquad\text{and}\qquad \liminf_{t\to+\infty}\|x(t)-x^*\|=0 .t→+∞lim​∫t0​t​sϵ(s)​ds1​∫t0​t​sϵ(s)​∥x(s)−x∗∥2ds=0andt→+∞liminf​∥x(t)−x∗∥=0.

No rate and no constant is asserted, so the goal does not depend on any particular choice of ϵ\epsilonϵ.

Milestones

  1. Lemma 4.1 (p. 16): for α>0\alpha>0α>0, β≥0\beta\ge0β≥0, the velocity is bounded, 1t∥x˙(t)∥2∈L1([t0,+∞))\frac1t\|\dot x(t)\|^2\in L^1([t_0,+\infty))t1​∥x˙(t)∥2∈L1([t0​,+∞)), and sup⁡t≥t01t∣h˙x∗(t)∣<+∞\sup_{t\ge t_0}\frac1t|\dot h_{x^*}(t)|<+\inftysupt≥t0​​t1​∣h˙x∗​(t)∣<+∞ for every x∗∈argmin⁡gx^*\in\operatorname{argmin} gx∗∈argming.
  2. §4, p. 18: ∥xϵ∥≤∥x∗∥\|x_\epsilon\|\le\|x^*\|∥xϵ​∥≤∥x∗∥ for every ϵ>0\epsilon>0ϵ>0.
  3. §4, p. 18: lim⁡ϵ→0+xϵ=x∗\lim_{\epsilon\to0^+}x_\epsilon=x^*limϵ→0+​xϵ​=x∗ (stated in the paper as well known).
  4. (46) (p. 20): under the hypotheses of Theorem 4.2 there is C>0C>0C>0 with
∫t0tϵ(s)s(hx∗(s)−12(∥x∗∥2−∥xϵ(s)∥2))ds≤Cfor every t≥t0.\int_{t_0}^{t}\frac{\epsilon(s)}{s}\Big(h_{x^*}(s)-\frac12\big(\|x^*\|^2-\|x_{\epsilon(s)}\|^2\big)\Big)ds\le C\quad\text{for every }t\ge t_0 .∫t0​t​sϵ(s)​(hx∗​(s)−21​(∥x∗∥2−∥xϵ(s)​∥2))ds≤Cfor every t≥t0​.

Significance

The result shows that slow Tikhonov regularization still selects the minimum-norm minimizer when Hessian damping is added: the weighted time average of ∥x(t)−x∗∥2\|x(t)-x^*\|^2∥x(t)−x∗∥2 tends to zero and the trajectory comes arbitrarily close to x∗x^*x∗ infinitely often. The hypothesis is only α>0\alpha>0α>0, well below the threshold α≥3\alpha\ge3α≥3 that the paper needs for its fast rates, and no growth condition on ϵ\epsilonϵ beyond the divergence of ∫ϵ(t)/t dt\int\epsilon(t)/t\,dt∫ϵ(t)/tdt is imposed. It complements Theorem 4.4 of the same paper (a separate mission), which reaches full strong convergence under fast decay, ∫ϵ(t)/t dt<+∞\int\epsilon(t)/t\,dt<+\infty∫ϵ(t)/tdt<+∞, plus further conditions.

On the formal side, the theorem and its milestones are proved in the paper and in the cited literature, but none of them has a machine-checked proof. The work splits into an energy estimate for a nonautonomous second order ODE in a Hilbert space (Lemma 4.1), two facts about the Tikhonov curve that underlie the whole theory of Tikhonov regularization of convex problems (milestones 2 and 3), an integrated differential inequality (46), and a l'Hospital-type averaging step. The Tikhonov-curve facts are reusable for any formal treatment of viscosity selection and minimum-norm solutions.

Difficulty

The obvious attempt, a Lyapunov function that decreases along the trajectory and controls ∥x(t)−x∗∥\|x(t)-x^*\|∥x(t)−x∗∥, fails because x∗x^*x∗ is not a stationary point of the perturbed system: ∇g(x∗)+ϵ(t)x∗=ϵ(t)x∗≠0\nabla g(x^*)+\epsilon(t)x^*=\epsilon(t)x^*\neq0∇g(x∗)+ϵ(t)x∗=ϵ(t)x∗=0 in general. The distance to x∗x^*x∗ therefore need not decrease, and pointwise convergence is not available under the slow-decay hypothesis alone. The comparison point has to move along the Tikhonov curve xϵ(t)x_{\epsilon(t)}xϵ(t)​, whose convergence to x∗x^*x∗ comes without a rate. The available bound controls only a weighted integral of hx∗h_{x^*}hx∗​ corrected by ∥x∗∥2−∥xϵ(s)∥2\|x^*\|^2-\|x_{\epsilon(s)}\|^2∥x∗∥2−∥xϵ(s)​∥2, so the passage from (46) to the goal needs both xϵ(t)→x∗x_{\epsilon(t)}\to x^*xϵ(t)​→x∗ and the divergence of the weight. In the formal setting the Tikhonov-curve limit is itself a nontrivial weak-compactness argument in a Hilbert space, which the paper does not spell out.

Formalization scope

  • H\mathcal HH is a real Hilbert space (InnerProductSpace ℝ H, CompleteSpace H). ∇g\nabla g∇g is gradient g, and ∇2g(x)v\nabla^2 g(x)v∇2g(x)v is the Fréchet derivative of gradient g at xxx applied to vvv. "Twice Fréchet differentiable" means ggg and ∇g\nabla g∇g are differentiable; Lipschitz continuity on bounded sets is stated on every closed ball around the origin.
  • Trajectories are maps R→H\mathbb R\to\mathcal HR→H with explicit velocity and acceleration maps; derivatives are taken within [t0,+∞)[t_0,+\infty)[t0​,+∞) (one-sided at t0t_0t0​), the acceleration is continuous there, and values before t0t_0t0​ are irrelevant. The same holds for ϵ\epsilonϵ and its derivative.
  • Every theorem is stated for every global C2C^2C2-solution of (5). Existence and uniqueness of the solution is Theorem 2.1 of the paper, a milestone of the first mission of this series, so the hypothesis is not vacuous. The paper's standing α≥3\alpha\ge3α≥3 is replaced by each statement's own hypothesis α>0\alpha>0α>0.
  • The minimum-norm minimizer and the Tikhonov points are predicates on a candidate point; where the curve ϵ↦xϵ\epsilon\mapsto x_\epsilonϵ↦xϵ​ is needed, a selection that minimizes g+ϵ2∥⋅∥2g+\frac\epsilon2\|\cdot\|^2g+2ϵ​∥⋅∥2 for every ϵ>0\epsilon>0ϵ>0 is a hypothesis.
  • ∫t0+∞ϵ(t)/t dt=+∞\int_{t_0}^{+\infty}\epsilon(t)/t\,dt=+\infty∫t0​+∞​ϵ(t)/tdt=+∞ is stated as divergence of T↦∫t0Tϵ(t)/t dtT\mapsto\int_{t_0}^T\epsilon(t)/t\,dtT↦∫t0​T​ϵ(t)/tdt, never as an equation for a Bochner integral, which would take the value 000 on a non-integrable function. Likewise, lim inf⁡∥x(t)−x∗∥=0\liminf\|x(t)-x^*\|=0liminf∥x(t)−x∗∥=0 is stated as "for every δ>0\delta>0δ>0, ∥x(t)−x∗∥<δ\|x(t)-x^*\|<\delta∥x(t)−x∗∥<δ for arbitrarily large ttt", not through Filter.liminf, whose value on an unbounded function is a default. sup⁡<+∞\sup<+\inftysup<+∞ is boundedness from above of the image of [t0,+∞)[t_0,+\infty)[t0​,+∞), and L1L^1L1 membership is integrability on [t0,+∞)[t_0,+\infty)[t0​,+∞).
  • Definitions needed: argmin, the minimum-norm minimizer, Tikhonov points, the General assumption, the solution predicate for (5), and hx∗h_{x^*}hx∗​, h˙x∗\dot h_{x^*}h˙x∗​. These duplicate objects of the other two missions of the series, which are drafted independently.
  • Contributions welcome: proofs of the Tikhonov-curve facts in Mathlib generality, the energy estimate of Lemma 4.1, a continuous l'Hospital/Cesàro lemma for weighted averages, and the goal itself.

Selected references

  • R.I. Boţ, E.R. Csetnek, S.C. László, Tikhonov regularization of a second order dynamical system with Hessian driven damping, Mathematical Programming, 2021, https://doi.org/10.1007/s10107-020-01528-8 (cited from arXiv:1911.12845v2). https://arxiv.org/abs/1911.12845
  • H. Attouch, Z. Chbani, H. Riahi, Combining fast inertial dynamics for convex optimization with Tikhonov regularization, Journal of Mathematical Analysis and Applications 457(2), 1065–1094, 2018. https://arxiv.org/abs/1602.01973
  • H. Attouch, J. Peypouquet, P. Redont, Fast convex optimization via inertial dynamics with Hessian driven damping, Journal of Differential Equations 261(10), 5734–5783, 2016. https://arxiv.org/abs/1601.07113
  • H. Attouch, Z. Chbani, J. Peypouquet, P. Redont, Fast convergence of inertial dynamics and algorithms with asymptotic vanishing viscosity, Mathematical Programming 168, 123–175, 2018. https://arxiv.org/abs/1507.04782
  • W. Su, S. Boyd, E.J. Candès, A differential equation for modeling Nesterov's accelerated gradient method: theory and insights, Journal of Machine Learning Research 17(153), 1–43, 2016. https://arxiv.org/abs/1503.01243
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Optimization·Captain: mikedeng1

Faster Convergence Rates of Relaxed Peaceman-Rachford and ADMM Under Regularity Assumptions IV: Lipschitz ∇g and Strongly Convex f (or Vice Versa) Make Relaxed PRS Contract LinearlyResearch Paper

Motivation

Peaceman–Rachford splitting separates the minimization of a sum into two proximal computations. That matters when each summand has a tractable proximal map but the sum does not. Douglas–Rachford splitting is its half-relaxed instance, and related iterations appear in the analysis of ADMM. Davis and Yin study how regularity of the two summands changes the rate at which a relaxed Peaceman–Rachford iteration approaches a fixed point. Their Section 4 distinguishes two arrangements: one summand may carry both strong convexity and a Lipschitz gradient, or the two properties may be shared between summands. The mixed case of Theorem 4.3 is the target of this mission. The authors describe it as a new result in the preprint version used here. Davis and Yin, §4, pp. 13–16.

Setting

Let HHH be a real Hilbert space and let f,g:H→(−∞,+∞]f,g:H\to(-\infty,+\infty]f,g:H→(−∞,+∞] be proper, closed, convex functions. For a step size γ>0\gamma>0γ>0, the proximal map Pf=prox⁡γfP_f=\operatorname{prox}_{\gamma f}Pf​=proxγf​ takes a point zzz to the minimizer of f(x)+∥x−z∥2/(2γ)f(x)+\|x-z\|^2/(2\gamma)f(x)+∥x−z∥2/(2γ); define PgP_gPg​ similarly. The reflection associated with a proximal map PPP is RP=2P−IR_P=2P-IRP​=2P−I. The Peaceman–Rachford operator is TPRS=RPf∘RPgT_{\rm PRS}=R_{P_f}\circ R_{P_g}TPRS​=RPf​​∘RPg​​. Its relaxed iteration, Algorithm 1 of the paper, is

zk+1=(1−λk)zk+λkTPRS(zk),0<λk≤1.z^{k+1}=(1-\lambda_k)z^k+\lambda_k T_{\rm PRS}(z^k), \qquad 0<\lambda_k\le1.zk+1=(1−λk​)zk+λk​TPRS​(zk),0<λk​≤1.

The analysis fixes a point z∗z^*z∗ satisfying TPRS(z∗)=z∗T_{\rm PRS}(z^*)=z^*TPRS​(z∗)=z∗ and writes x∗=Pg(z∗)x^*=P_g(z^*)x∗=Pg​(z∗). It also uses the two proximal points xgk=Pg(zk)x_g^k=P_g(z^k)xgk​=Pg​(zk) and xfk=Pf(RPg(zk))x_f^k=P_f(R_{P_g}(z^k))xfk​=Pf​(RPg​​(zk)). Their selected proximal subgradients are ∇~g(xgk)=(zk−xgk)/γ\widetilde\nabla g(x_g^k)=(z^k-x_g^k)/\gamma∇g(xgk​)=(zk−xgk​)/γ and ∇~f(xfk)=(RPg(zk)−xfk)/γ\widetilde\nabla f(x_f^k)=(R_{P_g}(z^k)-x_f^k)/\gamma∇f(xfk​)=(RPg​​(zk)−xfk​)/γ. Lemma 1.1 states that they belong to the respective convex subdifferentials and relates them to the iteration. These are selected subgradients, rather than arbitrary members of a set-valued subdifferential. Davis and Yin, §1.2 and Lemma 1.1, pp. 4–7.

A function is μ\muμ-strongly convex when its convexity inequality improves by the quadratic term μt(1−t)∥x−y∥2/2\mu t(1-t)\|x-y\|^2/2μt(1−t)∥x−y∥2/2. A (1/β)(1/\beta)(1/β)-Lipschitz gradient means the function is real valued, differentiable, and ∥∇h(x)−∇h(y)∥≤∥x−y∥/β\|\nabla h(x)-\nabla h(y)\|\le\|x-y\|/\beta∥∇h(x)−∇h(y)∥≤∥x−y∥/β, with β>0\beta>0β>0. Section 1.10 also permits the parameters μ\muμ and β\betaβ to be zero when a property is unavailable. Its auxiliary term Sf(x,y)S_f(x,y)Sf​(x,y) is the maximum of a squared-point-distance term weighted by μf/2\mu_f/2μf​/2 and a squared-selected-subgradient-distance term weighted by βf/2\beta_f/2βf​/2. The one-step bound (2.1) controls the sum of the corresponding terms for fff and ggg. Davis and Yin, (1.13)–(1.14) and (2.1), pp. 7–8.

Formalization targets

Mixed regularity: Theorem 4.3

Suppose μ,β>0\mu,\beta>0μ,β>0. The goal covers both arrangements: fff is μ\muμ-strongly convex while ggg has a (1/β)(1/\beta)(1/β)-Lipschitz gradient, and the arrangement with fff and ggg exchanged. In either case the target is

∥zk+1−z∗∥≤C(λk)∥zk−z∗∥,C(t)=(1−4t3min⁡{γμ,βγ,1−t})1/2.\|z^{k+1}-z^*\|\le C(\lambda_k)\|z^k-z^*\|, \qquad C(t)=\left(1-\frac{4t}{3}\min\left\{\gamma\mu,\frac{\beta}{\gamma},1-t\right\}\right)^{1/2}.∥zk+1−z∗∥≤C(λk​)∥zk−z∗∥,C(t)=(1−34t​min{γμ,γβ​,1−t})1/2.

The factor is the paper's explicit factor, for 0≤t≤10\le t\le10≤t≤1. It is strictly below one for 0<t<10<t<10<t<1 with fixed positive regularity parameters; at t=1t=1t=1 it equals one. A uniform geometric rate therefore requires relaxation parameters to remain in a range where these factors have a uniform upper bound below one. Davis and Yin, Theorem 4.3, p. 16.

Companion rates

Theorems 4.1 and 4.2 give the explicit factors when ggg, or respectively fff, supplies both properties. Proposition 4.1 translates a fixed-point contraction sequence into bounds on the proximal points, selected subgradients, fixed-point residual, and objective error. These are companion items in the proposal. The milestone list follows Lemma 1.1, the auxiliary bound (2.1), and the displayed estimates (4.6) and (4.7) from the proof of the mixed case. Davis and Yin, Proposition 4.1 and Theorems 4.1–4.3, pp. 13–16.

Significance

Theorem 4.3 identifies a rate available when neither summand alone carries both regularity properties. The explicit dependence on γ\gammaγ, μ\muμ, β\betaβ, and λk\lambda_kλk​ lets a reader compare choices of step size and relaxation without hiding them in an unspecified constant. Proposition 4.1 explains what a contraction in the auxiliary fixed-point variable says about the quantities used to judge an optimization method: proximal point error, residual, and objective error. The distinction between a per-step bound and a uniform geometric rate is part of the mathematical result.

The inequalities are proved in the source paper; the remaining work here is to give their statements and eventual proofs a machine-checked account. The shared setting makes the proximal operator, selected subgradients, and regularity terms explicit, so the same formal definitions can be used across this mission's estimates. The two external platform definitions cited by this development already provide the closed proper convex class, proximal-map predicate, smooth convex class, and subdifferential. The results in this proposal are open Lean statements until solvers supply proofs.

Difficulty

Strong convexity and Lipschitz smoothness control different quantities in the mixed case. The decrease inequality directly bounds distances between proximal points and between gradients, whereas the desired conclusion concerns zk−z∗z^k-z^*zk−z∗. Treating TPRST_{\rm PRS}TPRS​ merely as a nonexpansive operator yields no factor below one. The displayed estimate (4.7) expresses the fixed-point distance through the quantities controlled by (4.6). The proof must also identify the proximal subgradient of the smooth summand with its ordinary gradient, rather than assume that identity as part of the goal. Davis and Yin, proof of Theorem 4.3, p. 16.

Formalization scope

The Lean carrier is a complete real inner-product space, including the zero space. The functions take values in EReal to represent +∞+\infty+∞ outside their effective domains. The published IsProperClosedConvex, IsProx, IsSmoothConvex, and subgrad definitions supply the common function and operator conventions. A proximal map is passed as a function together with a proof that it minimizes the defining objective; under the standing assumptions it is uniquely determined. Every result involving a proximal map assumes γ>0\gamma>0γ>0. Run statements require 0<λk≤10<\lambda_k\le10<λk​≤1, and the mixed theorem requires μ,β>0\mu,\beta>0μ,β>0. The goal has no hypothesis asserting any of its decrease estimates or a contraction; those are results to establish.

The contraction factors use Real.sqrt. For the mixed and fff-regular factors, the radicands are positive throughout the relaxation range. For the ggg-regular factor, its nonnegativity follows from the compatibility of positive strong convexity and gradient Lipschitz parameters on a nonzero space; the zero space makes the contraction statement trivial even if that radicand is negative. Objective errors use real values only at proximal points where both summands are finite. The milestone (2.1) uses the paper's selected proximal subgradients. Proving the link between smooth gradients and those subgradients, and reusable proximal-map inequalities, are welcome contributions beyond the four named milestones.

Selected references

  • Damek Davis and Wotao Yin, Faster convergence rates of relaxed Peaceman–Rachford and ADMM under regularity assumptions, arXiv:1407.5210v3, 2015; published in Mathematics of Operations Research 42(3), 2017. Preprint, journal DOI.
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Optimization·Captain: mikedeng1

Faster Convergence Rates of Relaxed Peaceman-Rachford and ADMM Under Regularity Assumptions V: Relaxed PRS on Squared Distances Converges Linearly Under Bounded Linear RegularityResearch Paper

Motivation

The convex feasibility problem asks for a point in the intersection of closed convex sets. It underlies signal and image reconstruction, phase retrieval relaxations, and the constraint handling inside larger optimization methods. The workhorse algorithms are projection methods: the method of alternating projections (MAP), going back to von Neumann for subspaces, and the Douglas–Rachford and Peaceman–Rachford splitting schemes, which can be applied to the indicator, distance or squared-distance functions of the sets.

Without a regularity condition on how the sets meet, projection methods can converge arbitrarily slowly. Bounded linear regularity, an error bound saying that a point close to every set is close to their intersection, is the standard condition under which linear rates are obtained (Bauschke and Borwein, SIAM Review, 1996, doi:10.1137/S0036144593251710). Section 5 of D. Davis and W. Yin, Faster convergence rates of relaxed Peaceman–Rachford and ADMM under regularity assumptions (arXiv:1407.5210v3, Math. Oper. Res. 42(3), 2017) applies relaxed Peaceman–Rachford splitting (PRS) to the squared distance functions of two sets and proves that, under bounded linear regularity, the distance of the iterates to the intersection contracts by an explicit factor at every step, with step sizes and relaxation parameters allowed to vary between iterations. MAP is the special case of step size 1/21/21/2 and relaxation 111.

Setting

Let H\mathcal HH be a real Hilbert space and Cf,Cg⊆HC_f, C_g \subseteq \mathcal HCf​,Cg​⊆H closed convex sets with Cf∩Cg≠∅C_f\cap C_g\neq\emptysetCf​∩Cg​=∅. For C⊆HC\subseteq\mathcal HC⊆H the distance function is dC(x)=inf⁡y∈C∥x−y∥d_C(x)=\inf_{y\in C}\|x-y\|dC​(x)=infy∈C​∥x−y∥, and PCP_CPC​ is the metric projection, the nearest point of CCC. The problem is modelled with

f(x)=dCf2(x),g(x)=dCg2(x).f(x)=d^2_{C_f}(x),\qquad g(x)=d^2_{C_g}(x).f(x)=dCf​2​(x),g(x)=dCg​2​(x).

For γ>0\gamma>0γ>0 the proximal map proxγh(x)\mathbf{prox}_{\gamma h}(x)proxγh​(x) is the minimiser of h(y)+12γ∥y−x∥2h(y)+\frac1{2\gamma}\|y-x\|^2h(y)+2γ1​∥y−x∥2, and the reflection is reflγh=2 proxγh−I\mathbf{refl}_{\gamma h}=2\,\mathbf{prox}_{\gamma h}-Ireflγh​=2proxγh​−I. With two step sizes, TPRSγf,γg=reflγff∘reflγggT^{\gamma_f,\gamma_g}_{\mathrm{PRS}}=\mathbf{refl}_{\gamma_f f}\circ\mathbf{refl}_{\gamma_g g}TPRSγf​,γg​​=reflγf​f​∘reflγg​g​, and (T)λ=(1−λ)I+λT(T)_\lambda=(1-\lambda)I+\lambda T(T)λ​=(1−λ)I+λT.

Given z0z^0z0, step sizes γf,k,γg,k>0\gamma_{f,k},\gamma_{g,k}>0γf,k​,γg,k​>0 and relaxation parameters λk∈(0,1]\lambda_k\in(0,1]λk​∈(0,1], iteration (5.1) is

xgk=proxγg,kdCg2(zk),xfk=proxγf,kdCf2(2xgk−zk),zk+1=zk+2λk(xfk−xgk).x_g^k=\mathbf{prox}_{\gamma_{g,k}d^2_{C_g}}(z^k),\quad x_f^k=\mathbf{prox}_{\gamma_{f,k}d^2_{C_f}}(2x_g^k-z^k),\quad z^{k+1}=z^k+2\lambda_k(x_f^k-x_g^k).xgk​=proxγg,k​dCg​2​​(zk),xfk​=proxγf,k​dCf​2​​(2xgk​−zk),zk+1=zk+2λk​(xfk​−xgk​).

The pair {Cf,Cg}\{C_f,C_g\}{Cf​,Cg​} is boundedly linearly regular (Definition 5.1) if for every ρ>0\rho>0ρ>0 there is μρ>0\mu_\rho>0μρ​>0 such that

dCf∩Cg(x)≤μρmax⁡{dCf(x),dCg(x)}for all x∈B(0,ρ),d_{C_f\cap C_g}(x)\le\mu_\rho\max\{d_{C_f}(x),d_{C_g}(x)\}\qquad\text{for all }x\in B(0,\rho),dCf​∩Cg​​(x)≤μρ​max{dCf​​(x),dCg​​(x)}for all x∈B(0,ρ),

where B(0,ρ)B(0,\rho)B(0,ρ) is the open ball. The rate function is

C(γf,γg,λ,μ)=(1−4λmin⁡{γg/(2γg+1)2, γf/(2γf+1)2}μ2max⁡{16γg2/(2γg+1)2, 1})1/2.C(\gamma_f,\gamma_g,\lambda,\mu)=\left(1-\frac{4\lambda\min\{\gamma_g/(2\gamma_g+1)^2,\ \gamma_f/(2\gamma_f+1)^2\}}{\mu^2\max\{16\gamma_g^2/(2\gamma_g+1)^2,\ 1\}}\right)^{1/2}.C(γf​,γg​,λ,μ)=(1−μ2max{16γg2​/(2γg​+1)2, 1}4λmin{γg​/(2γg​+1)2, γf​/(2γf​+1)2}​)1/2.

Formalization targets

Goal: Theorem 5.1

Suppose {Cf,Cg}\{C_f,C_g\}{Cf​,Cg​} is boundedly linearly regular, (zk)(z^k)(zk) is generated by (5.1), every zjz^jzj lies in B(0,ρ)B(0,\rho)B(0,ρ), and dCf∩Cg≤μρmax⁡{dCf,dCg}d_{C_f\cap C_g}\le\mu_\rho\max\{d_{C_f},d_{C_g}\}dCf​∩Cg​​≤μρ​max{dCf​​,dCg​​} on B(0,ρ)B(0,\rho)B(0,ρ). Then for all k≥0k\ge0k≥0

dCf∩Cg(zk+1)≤C(γf,k,γg,k,λk,μρ) dCf∩Cg(zk),(5.3)d_{C_f\cap C_g}(z^{k+1})\le C(\gamma_{f,k},\gamma_{g,k},\lambda_k,\mu_\rho)\,d_{C_f\cap C_g}(z^k), \tag{5.3}dCf​∩Cg​​(zk+1)≤C(γf,k​,γg,k​,λk​,μρ​)dCf​∩Cg​​(zk),(5.3)

and if C‾=sup⁡jC(γf,j,γg,j,λj,μρ)<1\overline C=\sup_j C(\gamma_{f,j},\gamma_{g,j},\lambda_j,\mu_\rho)<1C=supj​C(γf,j​,γg,j​,λj​,μρ​)<1, the iterates converge to a point x∈Cf∩Cgx\in C_f\cap C_gx∈Cf​∩Cg​ with

∥zk−x∥≤2 dCf∩Cg(z0)∏i=0k−1C(γf,i,γg,i,λi,μρ).(5.4)\|z^k-x\|\le 2\,d_{C_f\cap C_g}(z^0)\prod_{i=0}^{k-1}C(\gamma_{f,i},\gamma_{g,i},\lambda_i,\mu_\rho). \tag{5.4}∥zk−x∥≤2dCf​∩Cg​​(z0)i=0∏k−1​C(γf,i​,γg,i​,λi​,μρ​).(5.4)

Milestones

The milestones follow the paper's own argument: Proposition 5.1 Parts 2 and 3 (the gradient of dC2d_C^2dC2​ and the closed form proxγdC2=12γ+1I+2γ2γ+1PC\mathbf{prox}_{\gamma d_C^2}=\frac1{2\gamma+1}I+\frac{2\gamma}{2\gamma+1}P_CproxγdC2​​=2γ+11​I+2γ+12γ​PC​); Proposition 5.2, the fundamental inequality specialised to squared distances; Propositions C.1 and C.2 (the fixed-point set of TPRSγf,γgT^{\gamma_f,\gamma_g}_{\mathrm{PRS}}TPRSγf​,γg​​ is Cf∩CgC_f\cap C_gCf​∩Cg​, and the iterates are Fejér monotone for λk∈(0,1]\lambda_k\in(0,1]λk​∈(0,1]); and the displays (5.5)–(5.7), (5.8), (5.10) and (5.11) of the proof of Theorem 5.1, ending with the one-step contraction at a single point.

Companion: Corollary 5.1

With γf,k≡γg,k≡12\gamma_{f,k}\equiv\gamma_{g,k}\equiv\frac12γf,k​≡γg,k​≡21​ and λk≡1\lambda_k\equiv1λk​≡1, iteration (5.1) is MAP, zk+1=PCfPCgzkz^{k+1}=P_{C_f}P_{C_g}z^kzk+1=PCf​​PCg​​zk, and under the assumptions of Theorem 5.1 it contracts the distance to Cf∩CgC_f\cap C_gCf​∩Cg​ by (1−1/μρ2)1/2(1-1/\mu_\rho^2)^{1/2}(1−1/μρ2​)1/2 from the second iterate on, converging linearly to a point of the intersection.

Significance

Theorem 5.1 gives an explicit, iteration-wise linear rate for relaxed PRS on the two-set feasibility problem with step sizes and relaxation parameters that may change from step to step. Its specialisation, Corollary 5.1, recovers linear convergence of MAP under bounded linear regularity with rate (1−1/μρ2)1/2(1-1/\mu_\rho^2)^{1/2}(1−1/μρ2​)1/2, better than the (1−1/(8μ2))1/2(1-1/(8\mu^2))^{1/2}(1−1/(8μ2))1/2 derived in earlier work on cyclic projections. Remark 5.1 of the paper notes that Douglas–Rachford on indicator functions is a limiting case of the scheme as the step sizes grow, though the rate degenerates in that limit.

The results are proved in the paper; the proof of the convergence statement cites Bauschke–Combettes, Convex Analysis and Monotone Operator Theory in Hilbert Spaces, Theorem 5.12 (Fejér monotone sequences whose distance to a closed convex set decays converge strongly). No machine-checked proof of these statements was found on Prove2Me (search of 2026-10-07). A formalization produces a checked chain from the closed form of the prox of dC2d_C^2dC2​ through the fundamental inequality to the linear rate, and with it reusable facts about squared distance functions, metric projections onto closed convex sets in Hilbert space, and Fejér monotone sequences.

Difficulty

The obvious argument would contract the distance to Cf∩CgC_f\cap C_gCf​∩Cg​ directly, but one PRS step measures only dCgd_{C_g}dCg​​ at zzz and dCfd_{C_f}dCf​​ at the reflected point reflγgg(z)\mathbf{refl}_{\gamma_g g}(z)reflγg​g​(z), never dCf(z)d_{C_f}(z)dCf​​(z). Transferring the second distance back to zzz costs a factor max⁡{c12,1}\max\{c_1^2,1\}max{c12​,1} with c1=4γg/(2γg+1)c_1=4\gamma_g/(2\gamma_g+1)c1​=4γg​/(2γg​+1), and only after that does the regularity inequality turn max⁡{dCf(z),dCg(z)}\max\{d_{C_f}(z),d_{C_g}(z)\}max{dCf​​(z),dCg​​(z)} into dCf∩Cg(z)d_{C_f\cap C_g}(z)dCf​∩Cg​​(z). The fundamental inequality (5.2) itself rests on the prox-gradient calculus of the earlier sections, specialised to functions whose gradients 2(I−PC)2(I-P_C)2(I−PC​) are Lipschitz. Passing from a contracting distance to convergence of the iterates to one point needs Fejér monotonicity and a completeness argument; a contracting distance alone does not give a limit.

Formalization scope

Everything lives in a real Hilbert space (InnerProductSpace ℝ H with CompleteSpace H); dCd_CdC​ is Mathlib's Metric.infDist. The squared distance is viewed as an extended-real function so that the published proximal predicate ThreeOpSplitting.ConvexRates.IsProx applies, and prox maps are arbitrary maps satisfying it (unique here). Metric projections are maps satisfying the published RandomGradFree.Nonsmooth.IsMetricProjection. Step sizes and prox maps are indexed by the iteration. The hypotheses of the goal are: Cf,CgC_f,C_gCf​,Cg​ closed and convex with nonempty intersection; bounded linear regularity of the pair; γf,k,γg,k>0\gamma_{f,k},\gamma_{g,k}>0γf,k​,γg,k​>0; λk∈(0,1]\lambda_k\in(0,1]λk​∈(0,1]; iterates in an open ball B(0,ρ)B(0,\rho)B(0,ρ) on which the regularity inequality holds with μρ>0\mu_\rho>0μρ​>0. The range λk∈(0,1]\lambda_k\in(0,1]λk​∈(0,1] is Algorithm 1's standing assumption, used in the proof but not restated in (5.1). The condition C‾<1\overline C<1C<1 is stated as a uniform bound c<1c<1c<1 on all rate factors. The product in (5.4) runs over i=0,…,k−1i=0,\dots,k-1i=0,…,k−1; the page prints the upper index kkk, which claims an extra factor that the proof does not give. In the proof's (5.9)–(5.10) the page swaps γf\gamma_fγf​ and γg\gamma_gγg​ relative to (5.2); the milestone states the pairing that (5.2) produces. Corollary 5.1's improved rate is stated for k≥1k\ge1k≥1, since it uses zk∈Cfz^k\in C_fzk∈Cf​.

A trivializing formalization is ruled out: the goal mentions none of the proof's intermediate quantities, takes the prox maps as genuine minimisers of the squared-distance objective rather than chosen points, and measures distances to a nonempty intersection, so the junk value of infDist on the empty set never arises.

A complete development needs the closed form of proxγdC2\mathbf{prox}_{\gamma d^2_C}proxγdC2​​, differentiability of dC2d_C^2dC2​, the fundamental inequality of the paper's §1 specialised to these functions, and the convergence theorem for Fejér monotone sequences. The last three are reusable well beyond this mission. Proofs of any milestone, and of Mathlib-level lemmas on metric projections, are welcome.

Selected references

  • D. Davis, W. Yin, Faster convergence rates of relaxed Peaceman–Rachford and ADMM under regularity assumptions, Mathematics of Operations Research 42(3), 2017; arXiv version used here: arXiv:1407.5210v3.
  • H. H. Bauschke, J. M. Borwein, On projection algorithms for solving convex feasibility problems, SIAM Review 38(3), 1996. doi:10.1137/S0036144593251710
  • H. H. Bauschke, P. L. Combettes, Convex Analysis and Monotone Operator Theory in Hilbert Spaces, Springer, 2011. doi:10.1007/978-1-4419-9467-7
  • P.-L. Lions, B. Mercier, Splitting algorithms for the sum of two nonlinear operators, SIAM Journal on Numerical Analysis 16(6), 1979. doi:10.1137/0716071
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Optimization·Captain: mikedeng1

Faster Convergence Rates of Relaxed Peaceman-Rachford and ADMM Under Regularity Assumptions III: With Lipschitz ∇g and Small Stepsize, the DRS Objective Error Is O(1/(k+1)) and o(1/(k+1))Research Paper

Why this rate matters

Douglas–Rachford splitting is a method for minimizing a sum of two convex functions when each function has an accessible proximal operator. Its iterates are easy to state, but the speed of convergence of the objective at an individual proximal point is less immediate than convergence of an averaged point or of a residual. For optimization models in which one summand has a Lipschitz continuous gradient, Davis and Yin give explicit objective-error bounds that depend on the proximal stepsize. Their paper compares these bounds with forward–backward splitting and shows that DRS has an objective rate at least as fast when the stepsize is sufficiently small.

The present mission formalizes the rate in Theorem 3.2 and the Appendix B estimates that state the relevant contraction, monotonicity and summability properties. The companion Theorem 3.3 concerns the squared fixed-point residual. Both results are proved in the 2015 arXiv version of the paper, which fixes the numbering and constants used here; the journal article appeared in Mathematics of Operations Research in 2017.

The DRS setting

Let HHH be a real Hilbert space. Let f:H→(−∞,+∞]f:H\to(-\infty,+\infty]f:H→(−∞,+∞] be proper, lower semicontinuous and convex, and let g:H→Rg:H\to\mathbb Rg:H→R be convex and differentiable with a (1/β)(1/\beta)(1/β)-Lipschitz gradient for some β>0\beta>0β>0. The proximal map of a function hhh at stepsize γ>0\gamma>0γ>0 sends zzz to the minimizer of h(x)+∥x−z∥2/(2γ)h(x)+\|x-z\|^2/(2\gamma)h(x)+∥x−z∥2/(2γ). Write Pf=prox⁡γfP_f=\operatorname{prox}_{\gamma f}Pf​=proxγf​ and Pg=prox⁡γgP_g=\operatorname{prox}_{\gamma g}Pg​=proxγg​, and let RP=2P−IR_P=2P-IRP​=2P−I be the reflection associated with a proximal map PPP.

The Peaceman–Rachford map is TPRS=RPf∘RPgT_{\mathrm{PRS}}=R_{P_f}\circ R_{P_g}TPRS​=RPf​​∘RPg​​. The DRS run is the relaxed PRS run with relaxation parameter 1/21/21/2 at every step:

zk+1=12zk+12TPRS(zk),xgk=Pg(zk),xfk=Pf(RPg(zk)).z^{k+1}=\tfrac12z^k+\tfrac12T_{\mathrm{PRS}}(z^k),\qquad x_g^k=P_g(z^k),\qquad x_f^k=P_f(R_{P_g}(z^k)).zk+1=21​zk+21​TPRS​(zk),xgk​=Pg​(zk),xfk​=Pf​(RPg​​(zk)).

Equivalently, zk+1=zk+xfk−xgkz^{k+1}=z^k+x_f^k-x_g^kzk+1=zk+xfk​−xgk​. The initial z0∈Hz^0\in Hz0∈H is arbitrary. Let z∗z^*z∗ be a fixed point of TPRST_{\mathrm{PRS}}TPRS​, and put x∗=Pg(z∗)x^*=P_g(z^*)x∗=Pg​(z∗). The objective value compared in this mission is at xfkx_f^kxfk​ for both summands: ek=f(xfk)+g(xfk)−f(x∗)−g(x∗)e_k=f(x_f^k)+g(x_f^k)-f(x^*)-g(x^*)ek​=f(xfk​)+g(xfk​)−f(x∗)−g(x∗). These values are finite under the standing assumptions. The section's Assumption 5 requires the smoothness of ggg and constant relaxation 1/21/21/2; it applies to Theorems 3.2 and 3.3 even though their own sentences do not repeat it.

Formalization targets

Objective error: Theorem 3.2

Let ρ=(1+5)/2\rho=(1+\sqrt5)/2ρ=(1+5​)/2 be the positive root of r3−2r−1=0r^3-2r-1=0r3−2r−1=0, and κ≈1.24698\kappa\approx1.24698κ≈1.24698 the positive root of r3+r2−2r−1=0r^3+r^2-2r-1=0r3+r2−2r−1=0. The first target bounds the best objective error at every k≥0k\ge0k≥0:

min⁡0≤i≤kei≤12γ(k+1){∥xg0−x∗∥2,γ<ρβ,∥xg0−x∗∥2+γ3/β−2γβ−β2β2+γ2∥z0−z∗∥2,γ≥ρβ.\min_{0\le i\le k}e_i\le\frac{1}{2\gamma(k+1)}\begin{cases}\|x_g^0-x^*\|^2,&\gamma<\rho\beta,\\\|x_g^0-x^*\|^2+\dfrac{\gamma^3/\beta-2\gamma\beta-\beta^2}{\beta^2+\gamma^2}\|z^0-z^*\|^2,&\gamma\ge\rho\beta.\end{cases}0≤i≤kmin​ei​≤2γ(k+1)1​⎩⎨⎧​∥xg0​−x∗∥2,∥xg0​−x∗∥2+β2+γ2γ3/β−2γβ−β2​∥z0−z∗∥2,​γ<ρβ,γ≥ρβ.​

For every γ>0\gamma>0γ>0, this best error is o(1/(k+1))o(1/(k+1))o(1/(k+1)). When γ<κβ\gamma<\kappa\betaγ<κβ, the same first-case upper bound holds for each eke_kek​, and ek=o(1/(k+1))e_k=o(1/(k+1))ek​=o(1/(k+1)). The goal states all four clauses together. The paper prints ρ≈2.2056\rho\approx2.2056ρ≈2.2056, the positive root of r3−2r2−1r^3-2r^2-1r3−2r2−1. That threshold does not match the coefficient γ3/β−2γβ−β2\gamma^3/\beta-2\gamma\beta-\beta^2γ3/β−2γβ−β2 the proof needs to be nonpositive, and with it the first case fails: for f=0f=0f=0, g(x)=x2/(2β)g(x)=x^2/(2\beta)g(x)=x2/(2β) on R\mathbb RR, γ=2β\gamma=2\betaγ=2β and k=0k=0k=0 the error is twice the bound. The mission states the theorem with the threshold the proof supports, the positive root of r3−2r−1r^3-2r-1r3−2r−1.

Fixed-point residual: Theorem 3.3

For γ<κβ\gamma<\kappa\betaγ<κβ and k≥1k\ge1k≥1, the companion target is

∥zk−zk+1∥2≤β2∥xg0−x∗∥2k2(1+γ/β)2(β2−γ2/κ2),∥zk−zk+1∥2=o(1/k2).\|z^k-z^{k+1}\|^2\le\frac{\beta^2\|x_g^0-x^*\|^2}{k^2(1+\gamma/\beta)^2(\beta^2-\gamma^2/\kappa^2)},\qquad \|z^k-z^{k+1}\|^2=o(1/k^2).∥zk−zk+1∥2≤k2(1+γ/β)2(β2−γ2/κ2)β2∥xg0​−x∗∥2​,∥zk−zk+1∥2=o(1/k2).

The Appendix B milestones give the contraction of the smooth gradient at proximal points, a fundamental one-step inequality, monotonicity, the extremal admissible stepsize ratio, and two summability bounds. Their constants and indices match the printed displays (B.1), (B.4), (B.7), (B.8), (B.10) and (B.12).

What the result supplies

The objective theorem gives a rate directly at the proximal point xfkx_f^kxfk​ when the stepsize is below the smaller threshold. Outside that regime, it still gives a best-iterate rate for every positive stepsize, including the explicit correction term for larger γ\gammaγ. The residual theorem controls the change in the DRS state at the faster squared rate. These statements let later work compare DRS against other splitting methods using the same objective and residual quantities, rather than changing the point at which the objective is measured.

The paper proves these results (Theorem 3.2 with the corrected threshold ρ\rhoρ); their statements are not new conjectures. The formalization work is to connect extended-real convex functions, actual proximal minimizers, smooth gradients, infinite sums, finite minima, and little-o assertions in a single Lean development. The seven Appendix B milestones are also useful as separately importable facts about proximal splitting. A machine-checked proof is still needed for the draft theorems of this mission.

Where the analysis is delicate

The familiar convergence of the DRS fixed-point residual does not by itself give the objective error at xfkx_f^kxfk​. An objective comparison involves the two different proximal points and the smooth gradient evaluated at successive xgkx_g^kxgk​. The large-stepsize regime changes the coefficient of the gradient increment and therefore changes the explicit bound. For the per-iterate conclusion, one must establish a monotone, summable quantity that dominates the objective error; a best-iterate estimate alone does not yield the stated nonergodic little-o claim. This explains why the mission retains the Appendix B estimates rather than replacing the goal with a generic O(1/k)O(1/k)O(1/k) statement.

Formalization scope

The Lean carrier is a complete real inner-product space. The proper, closed, convex predicate for fff and the proximal-map predicate are imported from the published ThreeOpSplitting.ConvexRates.Problem definition; the published MoreauProx.Characterization.GammaZero supplies the subgradient notion used by the paper's surrounding analysis. The smooth ggg is a real-valued function, with its actual gradient supplied by Mathlib's gradient and constrained by the imported smoothness predicate. Each proximal map is a function with the defining minimization property; the theorems do not assume an arbitrary map can stand in for a prox.

The fixed point z∗z^*z∗ is an explicit hypothesis, as in the paper. The two root constants are positive real numbers satisfying their defining cubics, never decimal approximations. A finite minimum ranges over i=0,…,ki=0,\ldots,ki=0,…,k; infinite sums come with summability; asymptotic claims use genuine little-o. The k≥1k\ge1k≥1 condition protects the k2k^2k2 denominator in Theorem 3.3. The objective error is taken at xfkx_f^kxfk​, never at xgkx_g^kxgk​, and the goal contains no auxiliary monotonicity or summability assumption that would assert part of its proof. Further contributions that establish proximal finiteness, the Appendix B inequalities, and the rates themselves fit within this scope.

Selected references

  • Damek Davis and Wotao Yin, Faster convergence rates of relaxed Peaceman-Rachford and ADMM under regularity assumptions, Mathematics of Operations Research 42(3), 2017. arXiv:1407.5210v3; DOI:10.1287/moor.2016.0827.
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Optimization·Captain: mikedeng1

Faster Convergence Rates of Relaxed Peaceman-Rachford and ADMM Under Regularity Assumptions II: With One Lipschitz Gradient, the Best Relaxed PRS Objective Error Is o(1/(k+1))Research Paper

Motivation

Many problems in signal processing, statistics and machine learning ask to minimise a sum f+gf + gf+g of two convex functions, each of which is easy to handle on its own through its proximal operator but not jointly. Operator-splitting methods exploit exactly that structure. The Douglas–Rachford (DRS) and Peaceman–Rachford (PRS) splitting schemes, introduced for linear equations in the 1950s and extended to maximal monotone operators by Lions and Mercier (1979), are the classical examples; applied to the dual of a linearly constrained problem, DRS is the alternating direction method of multipliers (ADMM) of Gabay and Mercier (1976).

Convergence of these methods has been known for decades, but convergence rates in terms of the objective value were established only recently. Davis and Yin (arXiv:1406.4834) showed that for general convex f,gf, gf,g the objective error of relaxed PRS converges at the nonergodic rate o(1/k+1)o(1/\sqrt{k+1})o(1/k+1​), and that this is sharp. The paper behind this mission (arXiv:1407.5210v3) asks how much faster the method becomes when fff or ggg is more regular. Its Theorem 3.1 answers the question for the case of one smooth function: the best objective error found in the first kkk iterations is o(1/(k+1))o(1/(k+1))o(1/(k+1)), for any stepsize. This matches the rate of forward–backward splitting (FBS), the method one would otherwise use when one of the two functions is smooth, without FBS's stepsize restriction.

Setting

Let H\mathcal HH be a real Hilbert space and let f,g:H→(−∞,∞]f, g : \mathcal H \to (-\infty, \infty]f,g:H→(−∞,∞] be closed, proper and convex. For γ>0\gamma > 0γ>0 the proximal operator is

proxγf(x)=arg⁡min⁡y∈H f(y)+12γ∥y−x∥2,\mathbf{prox}_{\gamma f}(x) = \arg\min_{y \in \mathcal H}\ f(y) + \tfrac{1}{2\gamma}\|y - x\|^2,proxγf​(x)=argy∈Hmin​ f(y)+2γ1​∥y−x∥2,

the reflection is reflγf=2 proxγf−IH\mathbf{refl}_{\gamma f} = 2\,\mathbf{prox}_{\gamma f} - I_{\mathcal H}reflγf​=2proxγf​−IH​, and the PRS operator is TPRS=reflγf∘reflγgT_{\mathrm{PRS}} = \mathbf{refl}_{\gamma f}\circ\mathbf{refl}_{\gamma g}TPRS​=reflγf​∘reflγg​. For λ>0\lambda > 0λ>0 write (TPRS)λ=(1−λ)IH+λTPRS(T_{\mathrm{PRS}})_\lambda = (1-\lambda) I_{\mathcal H} + \lambda T_{\mathrm{PRS}}(TPRS​)λ​=(1−λ)IH​+λTPRS​.

Relaxed PRS (Algorithm 1) starts from any z0∈Hz^0 \in \mathcal Hz0∈H and iterates

zk+1=(1−λk)zk+λk reflγf∘reflγg(zk),λk∈(0,1].z^{k+1} = (1 - \lambda_k) z^k + \lambda_k\, \mathbf{refl}_{\gamma f}\circ\mathbf{refl}_{\gamma g}(z^k), \qquad \lambda_k \in (0,1].zk+1=(1−λk​)zk+λk​reflγf​∘reflγg​(zk),λk​∈(0,1].

The choice λk≡1/2\lambda_k \equiv 1/2λk​≡1/2 is DRS and λk≡1\lambda_k \equiv 1λk​≡1 is PRS. Each step computes two auxiliary points,

xgk=proxγg(zk),xfk=proxγf(2xgk−zk),x_g^k = \mathbf{prox}_{\gamma g}(z^k), \qquad x_f^k = \mathbf{prox}_{\gamma f}(2x_g^k - z^k),xgk​=proxγg​(zk),xfk​=proxγf​(2xgk​−zk),

which are the method's candidate solutions. If z∗z^*z∗ is a fixed point of TPRST_{\mathrm{PRS}}TPRS​, then x∗=proxγg(z∗)x^* = \mathbf{prox}_{\gamma g}(z^*)x∗=proxγg​(z∗) minimises f+gf + gf+g. The objective error at a point xxx is f(x)+g(x)−f(x∗)−g(x∗)f(x) + g(x) - f(x^*) - g(x^*)f(x)+g(x)−f(x∗)−g(x∗).

A function has a (1/β)(1/\beta)(1/β)-Lipschitz gradient (β>0\beta > 0β>0) if it is real-valued and differentiable and ∥∇f(x)−∇f(y)∥≤1β∥x−y∥\|\nabla f(x) - \nabla f(y)\| \le \frac1\beta\|x - y\|∥∇f(x)−∇f(y)∥≤β1​∥x−y∥ for all x,yx, yx,y.

Formalization targets

Goal: Theorem 3.1 (p. 10)

Suppose τ‾=inf⁡j≥0λj(1−λj)>0\underline\tau = \inf_{j\ge0}\lambda_j(1-\lambda_j) > 0τ​=infj≥0​λj​(1−λj​)>0. If ∇f\nabla f∇f is (1/β)(1/\beta)(1/β)-Lipschitz and xk=xgkx^k = x_g^kxk=xgk​, or if ∇g\nabla g∇g is (1/β)(1/\beta)(1/β)-Lipschitz and xk=xfkx^k = x_f^kxk=xfk​, then

min⁡i=0,…,k{f(xi)+g(xi)−f(x∗)−g(x∗)}=o(1k+1).\min_{i=0,\dots,k}\big\{f(x^i) + g(x^i) - f(x^*) - g(x^*)\big\} = o\Big(\frac{1}{k+1}\Big).i=0,…,kmin​{f(xi)+g(xi)−f(x∗)−g(x∗)}=o(k+11​).

Both cases are part of the goal. The statement fixes no constants: it asserts only the order of the best-iterate error, so it holds for every stepsize γ>0\gamma > 0γ>0.

Milestones

  • Theorem A.1 (p. 31): the descent inequality and the Baillon–Haddad cocoercivity inequality for a convex function with a (1/β)(1/\beta)(1/β)-Lipschitz gradient.
  • Lemma 1.1 (p. 7): the relaxed PRS step written through the prox subgradients ∇~g(xg)=(z−xg)/γ∈∂g(xg)\widetilde\nabla g(x_g) = (z - x_g)/\gamma \in \partial g(x_g)∇g(xg​)=(z−xg​)/γ∈∂g(xg​) and ∇~f(xf)∈∂f(xf)\widetilde\nabla f(x_f) \in \partial f(x_f)∇f(xf​)∈∂f(xf​).
  • Lemma C.1 (p. 35): the optimality conditions of TPRST_{\mathrm{PRS}}TPRS​, (C.1)–(C.2).
  • Inequality (1.16) (p. 8), the upper fundamental inequality at x∗x^*x∗, in the form with one Lipschitz gradient.
  • Proposition 3.1 (p. 10): 4γλ4\gamma\lambda4γλ times the objective error is bounded by a telescoping term plus a multiple of ∥z−z+∥2\|z - z^+\|^2∥z−z+∥2, with the constant depending on whether γ≤β\gamma \le \betaγ≤β.
  • Fact 1.2 Part 5 (p. 7): ∑iλi(1−λi)∥TPRSzi−zi∥2≤∥z0−z∗∥2\sum_i \lambda_i(1-\lambda_i)\|T_{\mathrm{PRS}}z^i - z^i\|^2 \le \|z^0 - z^*\|^2∑i​λi​(1−λi​)∥TPRS​zi−zi∥2≤∥z0−z∗∥2.
  • Fact 1.1 Part 3 (p. 6): the best entry of a sequence with ∑iλiai<∞\sum_i\lambda_i a_i < \infty∑i​λi​ai​<∞ is nonincreasing and is o(1/(Λk−Λ⌈k/2⌉))o(1/(\Lambda_k - \Lambda_{\lceil k/2\rceil}))o(1/(Λk​−Λ⌈k/2⌉​)).

A companion item states the explicit bounds of the proof of Theorem 3.1 (p. 11), of the form ∥z0−z∗∥2/(4γλ‾(k+1))\|z^0 - z^*\|^2/(4\gamma\underline\lambda(k+1))∥z0−z∗∥2/(4γλ​(k+1)) times a case-dependent factor.

Significance

The result separates relaxed PRS from FBS. FBS needs γ<2β\gamma < 2\betaγ<2β to converge, so it needs the Lipschitz constant of the gradient, or a line search to estimate it. Theorem 3.1 says relaxed PRS reaches the same o(1/(k+1))o(1/(k+1))o(1/(k+1)) best-iterate order for every γ>0\gamma > 0γ>0, and the companion bounds show how the constant depends on γ/β\gamma/\betaγ/β. The theorem and its explicit bounds are part of the paper's catalogue of rates (its Tables 1.1–1.2), which records how the rates of relaxed PRS and ADMM improve under regularity.

The result is proved in the paper. As far as is known, none of these statements is machine-checked. Formalizing it means building the prox calculus for extended-valued convex functions on a Hilbert space (Lemma 1.1, Lemma C.1), the descent and cocoercivity inequalities for smooth convex functions (Theorem A.1), the Fejér-type summability of the fixed-point residual of averaged nonexpansive maps (Fact 1.2), and the summable-sequence rate lemma (Fact 1.1). Each of these is reused across operator-splitting analyses.

Difficulty

The objective errors f(xk)+g(xk)−f(x∗)−g(x∗)f(x^k) + g(x^k) - f(x^*) - g(x^*)f(xk)+g(xk)−f(x∗)−g(x∗) are nonnegative and, by Proposition 3.1 and Fact 1.2, weighted-summable. They are not monotone, however. A summable nonnegative sequence need not be o(1/k)o(1/k)o(1/k) term by term, which is why only the best iterate gets the little-o rate. A summability argument that ignores this, or that claims the rate for the last iterate, proves something false.

Proposition 3.1 is the substantive step. The upper fundamental inequality contains an inner-product term 2⟨z−z+,z∗−x∗⟩2\langle z - z^+, z^* - x^*\rangle2⟨z−z+,z∗−x∗⟩ that does not telescope, and it must be absorbed through the optimality condition (C.2) and the smoothness inequalities (A.1)–(A.2). When γ>β\gamma > \betaγ>β the residual term that remains has the wrong sign. It is controlled only by a second use of the Lipschitz gradient, through the regularity term Sf(xf,x∗)S_f(x_f, x^*)Sf​(xf​,x∗), which costs the factor 1+(γ−β)/(2β)1 + (\gamma-\beta)/(2\beta)1+(γ−β)/(2β).

Formalization scope

  • Space and functions. H\mathcal HH is a real InnerProductSpace with CompleteSpace. f,gf, gf,g are H → EReal, closed, proper and convex in the sense of the published IsProperClosedConvex. A prox map is a map PPP with the published IsProx γ f P, which for γ>0\gamma > 0γ>0 determines it uniquely. The subdifferential is the published subgrad.
  • Smoothness. "∇f\nabla f∇f is (1/β)(1/\beta)(1/β)-Lipschitz" means: f=hf = hf=h for a real function hhh with the published IsSmoothConvex β h (convex, Fréchet differentiable, (1/β)(1/\beta)(1/β)-Lipschitz gradient), β>0\beta > 0β>0.
  • Standing assumptions. Assumption 1 (closed, proper, convex), γ>0\gamma > 0γ>0, and λk∈(0,1]\lambda_k \in (0,1]λk​∈(0,1] (Algorithm 1) are hypotheses of every item about the method. Assumption 4 (one Lipschitz gradient) appears as the hypothesis of each case.
  • Rates. τ‾>0\underline\tau > 0τ​>0 is encoded by a positive lower bound τ≤λj(1−λj)\tau \le \lambda_j(1-\lambda_j)τ≤λj​(1−λj​), which is equivalent. "ak=o(1/(k+1))a_k = o(1/(k+1))ak​=o(1/(k+1))" is Asymptotics.IsLittleO along atTop. The best iterate is Finset.inf' over {0,…,k}\{0,\dots,k\}{0,…,k}.
  • Objective error. It is a real number computed with EReal.toReal, evaluated only where all four values are finite. These points are prox outputs of a proper function, and values of the real-valued smooth function.
  • Disclosed choices. The page's stray "Let z∈Hz \in \mathcal Hz∈H" in Theorem 3.1 is dropped. (1.16) is stated with μf=μg=0\mu_f = \mu_g = 0μf​=μg​=0 and one β\betaβ vanishing, as the paper's §1.10 convention allows. The little-o of Fact 1.1 is stated under a positive lower bound on λj\lambda_jλj​; without one, its denominator can vanish identically.
  • No trivialization. Neither "respectively" case may be dropped, and the error must sit at xgkx_g^kxgk​ (smooth fff) or xfkx_f^kxfk​ (smooth ggg). Swapping the points, adding Proposition 3.1's bound or Fact 1.1 as a hypothesis, or bounding a weaker quantity than the minimum objective error would change the theorem.

Contributions are welcome at every level: the prox calculus of Lemma 1.1 and Lemma C.1, Theorem A.1, the summability results, and the final assembly.

Selected references

  • D. Davis, W. Yin, Faster convergence rates of relaxed Peaceman-Rachford and ADMM under regularity assumptions, Math. Oper. Res. 42(3), 2017; read as arXiv:1407.5210v3. https://arxiv.org/abs/1407.5210
  • D. Davis, W. Yin, Convergence rate analysis of several splitting schemes, arXiv:1406.4834, 2014. https://arxiv.org/abs/1406.4834
  • P.-L. Lions, B. Mercier, Splitting algorithms for the sum of two nonlinear operators, SIAM J. Numer. Anal. 16(6), 964–979, 1979. https://doi.org/10.1137/0716071
  • D. Gabay, B. Mercier, A dual algorithm for the solution of nonlinear variational problems via finite element approximation, Comput. Math. Appl. 2(1), 17–40, 1976. https://doi.org/10.1016/0898-1221(76)90003-1
  • H. H. Bauschke, P. L. Combettes, Convex Analysis and Monotone Operator Theory in Hilbert Spaces, Springer, 2011. https://doi.org/10.1007/978-1-4419-9467-7
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Operations ResearchOptimizationStatistics·Captain: mikedeng1

Sparse Regression at Scale: Branch-and-Bound rooted in First-Order Optimization 4: Lagrangian Duals of the Reduced Relaxation and Their Closed-Form Optimal Dual VariablesResearch Paper

Motivation

Best subset selection with ridge shrinkage, the ℓ0ℓ2\ell_0\ell_2ℓ0​ℓ2​-regularized least squares problem

min⁡β∈Rp 12∥y−Xβ∥22+λ0∥β∥0+λ2∥β∥22,\min_{\beta\in\mathbb R^p}\ \tfrac12\|y-X\beta\|_2^2+\lambda_0\|\beta\|_0+\lambda_2\|\beta\|_2^2,β∈Rpmin​ 21​∥y−Xβ∥22​+λ0​∥β∥0​+λ2​∥β∥22​,

is a mixed integer program. Exact solvers for it rely on branch-and-bound: at every node of the search tree a convex relaxation is solved, and the node is discarded if a lower bound on that relaxation already exceeds the best objective value found so far. Hazimeh, Mazumder and Saab (arXiv:2004.06152v2, Mathematical Programming 2022) build such a solver, L0BnB, for instances with ppp in the millions. Its relaxations are solved only approximately, by first-order methods, and an approximate primal solution does not by itself certify a lower bound. The bound has to come from a dual feasible point. Theorem 2 of the paper supplies the duals of the node relaxation in closed form, together with explicit formulas for the optimal dual variables as functions of the primal optimum. Everything the paper later proves about the quality of its dual bounds (Section 3.2, Theorem 3) starts from these formulas.

Setting

Data are a matrix X∈Rn×pX\in\mathbb R^{n\times p}X∈Rn×p with columns X1,…,XpX_1,\dots,X_pX1​,…,Xp​, a response y∈Rny\in\mathbb R^ny∈Rn, and parameters λ0,λ2,M>0\lambda_0,\lambda_2,M>0λ0​,λ2​,M>0, where MMM bounds the coefficients. Write [p]={1,…,p}[p]=\{1,\dots,p\}[p]={1,…,p} and [a]+=max⁡{a,0}[a]_+=\max\{a,0\}[a]+​=max{a,0}. The reverse Huber penalty is B(t)=∣t∣\mathcal B(t)=|t|B(t)=∣t∣ for ∣t∣≤1|t|\le1∣t∣≤1 and B(t)=(t2+1)/2\mathcal B(t)=(t^2+1)/2B(t)=(t2+1)/2 for ∣t∣≥1|t|\ge1∣t∣≥1. Define

ψ1(b)=2λ0 B(bλ2/λ0),ψ2(b)=(λ0M+λ2M)∣b∣,\psi_1(b)=2\lambda_0\,\mathcal B\big(b\sqrt{\lambda_2/\lambda_0}\big),\qquad \psi_2(b)=\Big(\frac{\lambda_0}{M}+\lambda_2M\Big)|b|,ψ1​(b)=2λ0​B(bλ2​/λ0​​),ψ2​(b)=(Mλ0​​+λ2​M)∣b∣,

and let ψ=ψ1\psi=\psi_1ψ=ψ1​ if λ0/λ2≤M\sqrt{\lambda_0/\lambda_2}\le Mλ0​/λ2​​≤M and ψ=ψ2\psi=\psi_2ψ=ψ2​ if λ0/λ2>M\sqrt{\lambda_0/\lambda_2}>Mλ0​/λ2​​>M. The reduced relaxation (5) is

min⁡β∈Rp F(β)=12∥y−Xβ∥22+∑i∈[p]ψ(βi)s.t.∥β∥∞≤M.\min_{\beta\in\mathbb R^p}\ F(\beta)=\tfrac12\|y-X\beta\|_2^2+\sum_{i\in[p]}\psi(\beta_i)\quad\text{s.t.}\quad\|\beta\|_\infty\le M.β∈Rpmin​ F(β)=21​∥y−Xβ∥22​+i∈[p]∑​ψ(βi​)s.t.∥β∥∞​≤M.

By Theorem 1 of the paper it is the interval relaxation of the perspective formulation, projected onto β\betaβ.

The two dual objectives of Theorem 2 are, for α,ρ∈Rn\alpha,\rho\in\mathbb R^nα,ρ∈Rn and γ,μ∈Rp\gamma,\mu\in\mathbb R^pγ,μ∈Rp,

h1(α,γ)=−12∥α∥22−αTy−∑i∈[p]v(α,γi),v(α,γi)=[(αTXi−γi)24λ2−λ0]++M∣γi∣,h_1(\alpha,\gamma)=-\tfrac12\|\alpha\|_2^2-\alpha^Ty-\sum_{i\in[p]}v(\alpha,\gamma_i),\qquad v(\alpha,\gamma_i)=\Big[\frac{(\alpha^TX_i-\gamma_i)^2}{4\lambda_2}-\lambda_0\Big]_++M|\gamma_i|,h1​(α,γ)=−21​∥α∥22​−αTy−i∈[p]∑​v(α,γi​),v(α,γi​)=[4λ2​(αTXi​−γi​)2​−λ0​]+​+M∣γi​∣, h2(ρ,μ)=−12∥ρ∥22−ρTy−M∥μ∥1,h_2(\rho,\mu)=-\tfrac12\|\rho\|_2^2-\rho^Ty-M\|\mu\|_1,h2​(ρ,μ)=−21​∥ρ∥22​−ρTy−M∥μ∥1​,

where h1h_1h1​ is maximized over all of Rn×Rp\mathbb R^n\times\mathbb R^pRn×Rp (problem (20)) and h2h_2h2​ subject to ∣ρTXi∣−μi≤λ0/M+λ2M|\rho^TX_i|-\mu_i\le\lambda_0/M+\lambda_2M∣ρTXi​∣−μi​≤λ0​/M+λ2​M for i∈[p]i\in[p]i∈[p] (problem (22)). For an optimal β∗\beta^*β∗ of (5), with residual r∗=y−Xβ∗r^*=y-X\beta^*r∗=y−Xβ∗, the candidate dual variables are

α∗=ρ∗=−r∗,γi∗=1[∣βi∗∣=M](α∗TXi−2Mλ2 sign(α∗TXi)),μi∗=1[∣βi∗∣=M](∣ρ∗TXi∣−λ0/M−λ2M).\alpha^*=\rho^*=-r^*,\qquad \gamma^*_i=\mathbb 1_{[|\beta^*_i|=M]}\big(\alpha^{*T}X_i-2M\lambda_2\,\mathrm{sign}(\alpha^{*T}X_i)\big),\qquad \mu^*_i=\mathbb 1_{[|\beta^*_i|=M]}\big(|\rho^{*T}X_i|-\lambda_0/M-\lambda_2M\big).α∗=ρ∗=−r∗,γi∗​=1[∣βi∗​∣=M]​(α∗TXi​−2Mλ2​sign(α∗TXi​)),μi∗​=1[∣βi∗​∣=M]​(∣ρ∗TXi​∣−λ0​/M−λ2​M).

In the Lean development these objects are F, box, h1, v, h2, Feas22, alphaStar, gammaStar, rhoStar, muStar in the namespace L0BnB.Duality.

Formalization targets

Goal: Theorem 2 (pp. 13–14)

Let β∗\beta^*β∗ minimize FFF over ∥β∥∞≤M\|\beta\|_\infty\le M∥β∥∞​≤M.

  • If λ0/λ2≤M\sqrt{\lambda_0/\lambda_2}\le Mλ0​/λ2​​≤M:  h1(α,γ)≤F(β)\ h_1(\alpha,\gamma)\le F(\beta) h1​(α,γ)≤F(β) for all α,γ\alpha,\gammaα,γ and all feasible β\betaβ, and h1(α∗,γ∗)=F(β∗)h_1(\alpha^*,\gamma^*)=F(\beta^*)h1​(α∗,γ∗)=F(β∗).
  • If λ0/λ2>M\sqrt{\lambda_0/\lambda_2}>Mλ0​/λ2​​>M:  h2(ρ,μ)≤F(β)\ h_2(\rho,\mu)\le F(\beta) h2​(ρ,μ)≤F(β) for all (ρ,μ)(\rho,\mu)(ρ,μ) feasible for (22) and all feasible β\betaβ; (ρ∗,μ∗)(\rho^*,\mu^*)(ρ∗,μ∗) is feasible for (22) and h2(ρ∗,μ∗)=F(β∗)h_2(\rho^*,\mu^*)=F(\beta^*)h2​(ρ∗,μ∗)=F(β∗).

This is "(20), respectively (22), is a dual of (5), and (23), respectively (24), are optimal dual variables", with the paper's remark that strong duality holds.

Milestones

  1. (45) For a∈Ra\in\mathbb Ra∈R, η≥0\eta\ge0η≥0 and D(b)=ψ1(b)+ab+η∣b∣D(b)=\psi_1(b)+ab+\eta|b|D(b)=ψ1​(b)+ab+η∣b∣, the point 000 (if 2λ0λ2+η−∣a∣≥02\sqrt{\lambda_0\lambda_2}+\eta-|a|\ge02λ0​λ2​​+η−∣a∣≥0) or −λ0/λ2 sign(a)-\sqrt{\lambda_0/\lambda_2}\,\mathrm{sign}(a)−λ0​/λ2​​sign(a) (otherwise) minimizes DDD on ∣b∣≤λ0/λ2|b|\le\sqrt{\lambda_0/\lambda_2}∣b∣≤λ0​/λ2​​.
  2. (47) If ∣a∣−η≥2λ0λ2|a|-\eta\ge2\sqrt{\lambda_0\lambda_2}∣a∣−η≥2λ0​λ2​​, then min⁡b∈RD(b)=−14λ2(∣a∣−η)2+λ0\min_{b\in\mathbb R}D(b)=-\frac{1}{4\lambda_2}(|a|-\eta)^2+\lambda_0minb∈R​D(b)=−4λ2​1​(∣a∣−η)2+λ0​.
  3. Weak duality, the first halves of both bullets of the goal.
  4. (23) h1(α∗,γ∗)=F(β∗)h_1(\alpha^*,\gamma^*)=F(\beta^*)h1​(α∗,γ∗)=F(β∗) when λ0/λ2≤M\sqrt{\lambda_0/\lambda_2}\le Mλ0​/λ2​​≤M.
  5. (24) (ρ∗,μ∗)(\rho^*,\mu^*)(ρ∗,μ∗) feasible for (22) and h2(ρ∗,μ∗)=F(β∗)h_2(\rho^*,\mu^*)=F(\beta^*)h2​(ρ∗,μ∗)=F(β∗) when λ0/λ2>M\sqrt{\lambda_0/\lambda_2}>Mλ0​/λ2​​>M.

Significance

The result. Theorem 2 turns the node relaxation of L0BnB into a pair of explicit concave maximization problems, one per regime of λ0/λ2\sqrt{\lambda_0/\lambda_2}λ0​/λ2​​ versus MMM. The dual (20) is unconstrained, so any (α,γ)(\alpha,\gamma)(α,γ) gives a valid lower bound; the paper's dual bounds (25)–(28) evaluate h1h_1h1​ or h2h_2h2​ at α^=−r^\hat\alpha=-\hat rα^=−r^ built from an inexact primal solution β^\hat\betaβ^​, with the remaining variable chosen in closed form. The formulas (23)–(24) explain why this choice is right: at the exact optimum it recovers the primal value. Theorem 3 of the paper, which bounds the loss of this dual bound by a quantity depending on the support size rather than on ppp, compares v(α^,γ^i)v(\hat\alpha,\hat\gamma_i)v(α^,γ^​i​) to v(α∗,γi∗)v(\alpha^*,\gamma^*_i)v(α∗,γi∗​) term by term and therefore depends on (23).

Formalizing it. The paper proves the case λ0/λ2≤M\sqrt{\lambda_0/\lambda_2}\le Mλ0​/λ2​​≤M in Appendix A and omits the proof of the case λ0/λ2>M\sqrt{\lambda_0/\lambda_2}>Mλ0​/λ2​​>M ("follows along the lines similar to what was shown above"). The appendix also contains an intermediate formula for the coordinate minimum, −[(∣αTXi∣−ηi)2/(4λ2)−λ0]+-[(|\alpha^TX_i|-\eta_i)^2/(4\lambda_2)-\lambda_0]_+−[(∣αTXi​∣−ηi​)2/(4λ2​)−λ0​]+​, that is incorrect when ηi\eta_iηi​ is large; the final dual (49) = (20) is nevertheless correct. A machine-checked proof supplies the omitted case and settles the correct statement. To our knowledge neither half has been formalized.

Difficulty

The dual objective (20) hides the box constraint inside the term M∣γi∣M|\gamma_i|M∣γi​∣ and the penalty inside [ ⋅ ]+[\,\cdot\,]_+[⋅]+​, and the reverse Huber penalty is piecewise, so even the weak-duality half has to handle both pieces of ψ1\psi_1ψ1​ and the junction ∣b∣=λ0/λ2|b|=\sqrt{\lambda_0/\lambda_2}∣b∣=λ0​/λ2​​. The attainment half is where the work lies: it needs the optimality conditions of a nonsmooth convex problem over a box, at coordinates where βi∗=0\beta^*_i=0βi∗​=0 (where ψ\psiψ is not differentiable), where ∣βi∗∣=M|\beta^*_i|=M∣βi∗​∣=M (where the box is active), and where both may interact with the regime boundary λ0/λ2=M\sqrt{\lambda_0/\lambda_2}=Mλ0​/λ2​​=M. The natural first idea, to read (23) off the Lagrangian derivation in the paper, does not yield a proof: that derivation assumes a dual optimum (α∗,η∗)(\alpha^*,\eta^*)(α∗,η∗) exists and relates it to β∗\beta^*β∗ by complementary slackness, whereas the theorem asserts an identity for the explicit (α∗,γ∗)(\alpha^*,\gamma^*)(α∗,γ∗) built from β∗\beta^*β∗ alone.

Formalization scope

Data are X : Matrix (Fin n) (Fin p) ℝ, y : Fin n → ℝ and reals lam0 lam2 M with 0 < lam0, 0 < lam2, 0 < M as hypotheses; [p][p][p] is Fin p. Norms and inner products are explicit sums: αTXi=∑rαrXri\alpha^TX_i=\sum_r\alpha_rX_{ri}αTXi​=∑r​αr​Xri​, ∥α∥22=∑rαr2\|\alpha\|_2^2=\sum_r\alpha_r^2∥α∥22​=∑r​αr2​, ∥μ∥1=∑i∣μi∣\|\mu\|_1=\sum_i|\mu_i|∥μ∥1​=∑i​∣μi​∣, [a]+=max⁡{a,0}[a]_+=\max\{a,0\}[a]+​=max{a,0}, and ∥β∥∞≤M\|\beta\|_\infty\le M∥β∥∞​≤M is ∣βi∣≤M|\beta_i|\le M∣βi​∣≤M for every iii. The regime split is written λ0/λ2≤M\sqrt{\lambda_0/\lambda_2}\le Mλ0​/λ2​​≤M versus M<λ0/λ2M<\sqrt{\lambda_0/\lambda_2}M<λ0​/λ2​​. sign is Real.sign, with sign(0)=0\mathrm{sign}(0)=0sign(0)=0; where it is evaluated in (23) the argument is nonzero at an optimum. The optimal solution β∗\beta^*β∗ is a hypothesis (feasible and minimizing FFF over the box); its existence is not part of the statements. The coordinate milestones (45) and (47) are stated for a scalar aaa standing for αTXi\alpha^TX_iαTXi​ and a multiplier η≥0\eta\ge0η≥0. No normalization of XXX or yyy is assumed: the unit-norm convention that opens Section 3 is not used by Theorem 2. The paper writes no O(⋅)O(\cdot)O(⋅) in these results, so no constants are instantiated.

"A dual is given by" is formalized as weak duality over all dual-feasible points together with equality at the explicit dual variables. Weak duality alone would not be Theorem 2, and neither would the equality alone; the goal requires both in both regimes. Uniqueness of the dual optimum is not claimed.

A complete development needs elementary convex analysis of the scalar penalty ψ1\psi_1ψ1​ (its conjugate and subdifferential), first-order optimality conditions for a convex function over a box in Rp\mathbb R^pRp, and finite-sum bookkeeping. The scalar facts about the reverse Huber penalty are reusable in the companion missions on the reduced relaxation and on dual-bound quality. Contributions to any milestone, or a direct proof of the goal, are welcome.

Selected references

  • H. Hazimeh, R. Mazumder, A. Saab, Sparse Regression at Scale: Branch-and-Bound rooted in First-Order Optimization, arXiv:2004.06152v2 (2021); Mathematical Programming (2022). https://arxiv.org/abs/2004.06152v2
  • S. Boyd, L. Vandenberghe, Convex Optimization, Cambridge University Press, 2004. https://web.stanford.edu/~boyd/cvxbook/
  • A. B. Owen, A robust hybrid of lasso and ridge regression, Contemporary Mathematics 443, 59–72, 2007. https://doi.org/10.1090/conm/443/08555
  • D. Bertsimas, A. King, R. Mazumder, Best subset selection via a modern optimization lens, Annals of Statistics 44(2), 813–852, 2016. https://doi.org/10.1214/15-AOS1388
  • H. Hazimeh, R. Mazumder, Fast best subset selection: coordinate descent and local combinatorial optimization algorithms, Operations Research 68(5), 1517–1537, 2020. https://arxiv.org/abs/1803.01454
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Dynamical SystemsFunctional AnalysisOperations Research+1·Captain: mikedeng1

Tikhonov Regularization of a Second Order Dynamical System with Hessian Driven Damping 1: For α > 3 and ∫ tε(t) dt < +∞ the Trajectory Converges Weakly to a Minimizer of gResearch Paper

Motivation

Minimizing a convex function ggg on a real Hilbert space H\mathcal HH by first-order methods has a continuous-time counterpart: second-order differential equations whose trajectories descend ggg. Su, Boyd and Candès (20) showed that Nesterov's accelerated gradient method is a discretization of x¨+αtx˙+∇g(x)=0\ddot x+\frac{\alpha}{t}\dot x+\nabla g(x)=0x¨+tα​x˙+∇g(x)=0 with α=3\alpha=3α=3, along which g(x(t))−min⁡g=O(1/t2)g(x(t))-\min g=O(1/t^2)g(x(t))−ming=O(1/t2). Two modifications of this equation have been studied separately because each adds a property the plain system lacks.

  • A Hessian-driven damping term β∇2g(x(t))x˙(t)\beta\nabla^2g(x(t))\dot x(t)β∇2g(x(t))x˙(t) (Attouch, Peypouquet, Redont, J. Differential Equations 2016) damps oscillations and, for β>0\beta>0β>0, makes t2∥∇g(x(t))∥2t^2\|\nabla g(x(t))\|^2t2∥∇g(x(t))∥2 integrable, while keeping fast values and weak convergence of trajectories.
  • A Tikhonov regularization term ϵ(t)x(t)\epsilon(t)x(t)ϵ(t)x(t) with ϵ(t)↓0\epsilon(t)\downarrow0ϵ(t)↓0 (Attouch, Chbani, Riahi, J. Math. Anal. Appl. 2018) can steer trajectories to the minimum-norm minimizer.

Boţ, Csetnek and László (arXiv:1911.12845v2, 2020) combine both terms and ask which properties of the two parent systems survive. This mission covers the first of their answers: when ϵ\epsilonϵ decays fast enough, the fast rates and the weak convergence of trajectories are preserved.

Timeline. 2016 (published 2018): weak convergence of trajectories of x¨+αtx˙+∇g(x)=0\ddot x+\frac\alpha t\dot x+\nabla g(x)=0x¨+tα​x˙+∇g(x)=0 for α>3\alpha>3α>3 (Attouch, Chbani, Peypouquet, Redont, Math. Program. 168). 2016: the same with Hessian-driven damping, β>0\beta>0β>0 (Attouch, Peypouquet, Redont). 2018: Tikhonov regularization of that system, with the O(1/t2)O(1/t^2)O(1/t2) rate kept and strong convergence to the minimum-norm minimizer under slow decay of ϵ\epsilonϵ (Attouch, Chbani, Riahi). 2020: both terms together (Boţ, Csetnek, László, this paper).

Setting

Fix a real Hilbert space H\mathcal HH, a starting time t0>0t_0>0t0​>0, parameters α≥3\alpha\ge3α≥3 and β≥0\beta\ge0β≥0, and initial data u0,v0∈Hu_0,v_0\in\mathcal Hu0​,v0​∈H. The General assumption of the paper is:

  • g:H→Rg:\mathcal H\to\mathbb Rg:H→R is convex and twice Fréchet differentiable, ∇g\nabla g∇g is Lipschitz continuous on bounded sets, and argmin⁡g≠∅\operatorname{argmin} g\ne\emptysetargming=∅; min⁡g\min gming denotes its minimal value;
  • ϵ:[t0,+∞)→[0,+∞)\epsilon:[t_0,+\infty)\to[0,+\infty)ϵ:[t0​,+∞)→[0,+∞) is nonincreasing, of class C1C^1C1, and ϵ(t)→0\epsilon(t)\to0ϵ(t)→0 as t→+∞t\to+\inftyt→+∞.

The dynamical system is

x¨(t)+αtx˙(t)+β∇2g(x(t))x˙(t)+∇g(x(t))+ϵ(t)x(t)=0,t≥t0,x(t0)=u0, x˙(t0)=v0.(5)\ddot x(t)+\frac{\alpha}{t}\dot x(t)+\beta\nabla^2g(x(t))\dot x(t)+\nabla g(x(t))+\epsilon(t)x(t)=0,\quad t\ge t_0,\quad x(t_0)=u_0,\ \dot x(t_0)=v_0. \tag{5}x¨(t)+tα​x˙(t)+β∇2g(x(t))x˙(t)+∇g(x(t))+ϵ(t)x(t)=0,t≥t0​,x(t0​)=u0​, x˙(t0​)=v0​.(5)

A global C2C^2C2-solution is a twice continuously differentiable x:[t0,+∞)→Hx:[t_0,+\infty)\to\mathcal Hx:[t0​,+∞)→H satisfying (5) for every t≥t0t\ge t_0t≥t0​. The decay of ϵ\epsilonϵ is controlled by ∫t0+∞tϵ(t) dt<+∞\int_{t_0}^{+\infty}t\epsilon(t)\,dt<+\infty∫t0​+∞​tϵ(t)dt<+∞ together with one of two conditions:

  • (a) there exist a>1a>1a>1 and t1≥t0t_1\ge t_0t1​≥t0​ with ϵ˙(t)≤−aβ2ϵ2(t)\dot\epsilon(t)\le-\frac{a\beta}{2}\epsilon^2(t)ϵ˙(t)≤−2aβ​ϵ2(t) for all t≥t1t\ge t_1t≥t1​;
  • (b) there exist a>0a>0a>0 and t1≥t0t_1\ge t_0t1​≥t0​ with ϵ(t)≤at\epsilon(t)\le\frac atϵ(t)≤ta​ for all t≥t1t\ge t_1t≥t1​.

A curve x(t)x(t)x(t) converges weakly to xˉ\bar xxˉ if ⟨x(t),v⟩→⟨xˉ,v⟩\langle x(t),v\rangle\to\langle\bar x,v\rangle⟨x(t),v⟩→⟨xˉ,v⟩ for every v∈Hv\in\mathcal Hv∈H. The Lean development lives in the namespace TikhonovHDD.Weak, with IsSolution, GenAssumptionG, GenAssumptionEps, CondA, CondB, argmin, minVal and WeakTendstoAtTop for these objects.

Formalization targets

Goal: Theorem 3.5 (p. 15)

Under the General assumption, ∫t0+∞tϵ(t) dt<+∞\int_{t_0}^{+\infty}t\epsilon(t)\,dt<+\infty∫t0​+∞​tϵ(t)dt<+∞ and (a) or (b), if α>3\alpha>3α>3 then every global C2C^2C2-solution of (5) satisfies

∃ xˉ∈argmin⁡g:x(t)⇀xˉ(t→+∞).\exists\,\bar x\in\operatorname{argmin} g:\qquad x(t)\rightharpoonup\bar x\quad(t\to+\infty).∃xˉ∈argming:x(t)⇀xˉ(t→+∞).

Milestones

In the order the argument uses them:

  1. Theorem 2.1 (p. 4): existence and uniqueness of a global C2C^2C2-solution of (5).
  2. Lemma A.2 (p. 29): a bounded-below, locally absolutely continuous FFF with F˙≤G∈L1\dot F\le G\in L^1F˙≤G∈L1 a.e. has a finite limit.
  3. Theorem 3.3 (p. 11), split three ways: for α≥3\alpha\ge3α≥3, g(x(t))−min⁡g=O(1/t2)g(x(t))-\min g=O(1/t^2)g(x(t))−ming=O(1/t2); for α>3\alpha>3α>3, xxx is bounded and t(g(x(t))−min⁡g)t(g(x(t))-\min g)t(g(x(t))−ming), t∥x˙∥2t\|\dot x\|^2t∥x˙∥2, tϵ∥x−x∗∥2t\epsilon\|x-x^*\|^2tϵ∥x−x∗∥2, tϵ∥x∥2∈L1t\epsilon\|x\|^2\in L^1tϵ∥x∥2∈L1; and separately t2∥∇g(x(t))∥2∈L1t^2\|\nabla g(x(t))\|^2\in L^1t2∥∇g(x(t))∥2∈L1.
  4. Lemma A.3 (p. 30): u(t)+tαu˙(t)→uˉu(t)+\frac t\alpha\dot u(t)\to\bar uu(t)+αt​u˙(t)→uˉ with α>0\alpha>0α>0 implies u(t)→uˉu(t)\to\bar uu(t)→uˉ.
  5. Theorem 3.4 (p. 12): for α>3\alpha>3α>3 and every x∗∈argmin⁡gx^*\in\operatorname{argmin} gx∗∈argming, t⟨∇g(x),x−x∗⟩∈L1t\langle\nabla g(x),x-x^*\rangle\in L^1t⟨∇g(x),x−x∗⟩∈L1, lim⁡∥x(t)−x∗∥\lim\|x(t)-x^*\|lim∥x(t)−x∗∥ and lim⁡t⟨x˙+β∇g(x),x−x∗⟩\lim t\langle\dot x+\beta\nabla g(x),x-x^*\ranglelimt⟨x˙+β∇g(x),x−x∗⟩ exist, g(x(t))−min⁡g=o(1/t2)g(x(t))-\min g=o(1/t^2)g(x(t))−ming=o(1/t2), ∥x˙+β∇g(x)∥=o(1/t)\|\dot x+\beta\nabla g(x)\|=o(1/t)∥x˙+β∇g(x)∥=o(1/t), and t2ϵ(t)∥x(t)∥2→0t^2\epsilon(t)\|x(t)\|^2\to0t2ϵ(t)∥x(t)∥2→0.

Significance

The result. Theorem 3.5 shows that the Tikhonov term, when it decays at least as fast as ∫tϵ<∞\int t\epsilon<\infty∫tϵ<∞ requires, does not disturb the asymptotics of the Hessian-damped system: values converge at rate o(1/t2)o(1/t^2)o(1/t2) and trajectories converge weakly to a minimizer. With β=0\beta=0β=0 it recovers the corresponding results for the regularized system without Hessian damping, and with ϵ≡0\epsilon\equiv0ϵ≡0 those for the Hessian-damped system. It is also the boundary case of the paper's second half, where slower decay of ϵ\epsilonϵ is shown to give strong convergence to the minimum-norm minimizer instead.

Formalizing it. The results are proved in the paper; none of them is machine-checked. A formal development would produce reusable pieces: a Lyapunov-energy analysis of second-order systems with time-dependent coefficients, the asymptotic Lemmas A.2 and A.3, and the bridge from "the distance to every minimizer converges and weak cluster points are minimizers" to weak convergence of a curve (the continuous Opial lemma).

Difficulty

The obvious approach, a single Lyapunov function that decreases along trajectories, fails here: the Tikhonov term makes the natural energy Eb\mathcal E_bEb​ only almost nonincreasing, with an error ∝tϵ(t)∥x∗∥2\propto t\epsilon(t)\|x^*\|^2∝tϵ(t)∥x∗∥2 that must be integrated, and the Hessian term produces a cross term −βϵ(t)t2⟨∇g(x),x⟩-\beta\epsilon(t)t^2\langle\nabla g(x),x\rangle−βϵ(t)t2⟨∇g(x),x⟩ that is controlled only by condition (a) or (b). The step from O(1/t2)O(1/t^2)O(1/t2) to o(1/t2)o(1/t^2)o(1/t2) and to the existence of lim⁡∥x(t)−x∗∥\lim\|x(t)-x^*\|lim∥x(t)−x∗∥ cannot be read off a single bounded energy: boundedness of Eb\mathcal E_bEb​ gives rates in OOO, not in ooo, and says nothing directly about ∥x(t)−x∗∥\|x(t)-x^*\|∥x(t)−x∗∥. Weak convergence then requires Opial's lemma, which is not in Mathlib in continuous form. Existence of solutions is itself nontrivial in infinite dimension: the right-hand side involves ∇2g\nabla^2g∇2g, so the system has to be rewritten as a first-order system before the Cauchy–Lipschitz theorem applies.

Formalization scope

  • H\mathcal HH is any real Hilbert space (InnerProductSpace ℝ H, CompleteSpace H); nothing is finite-dimensional, so weak convergence is genuinely weaker than norm convergence. It is stated through inner products with every v∈Hv\in\mathcal Hv∈H; stating it as norm convergence, or testing only some vvv, would change the theorem.
  • Trajectories are maps R→H\mathbb R\to\mathcal HR→H with velocity and acceleration maps; derivatives are one-sided at t0t_0t0​ and values before t0t_0t0​ play no role. Every theorem is stated for every C2C^2C2-solution; Theorem 2.1 shows this class is a singleton, so the hypothesis is not vacuous. A sorry-free check that the hypotheses of the goal can be met (g=0g=0g=0, ϵ=0\epsilon=0ϵ=0, x=0x=0x=0) accompanies the drafts.
  • ∇2g(x)v\nabla^2g(x)v∇2g(x)v is the derivative of ∇g\nabla g∇g at xxx applied to vvv; ϵ˙\dot\epsilonϵ˙ is a derivative map tied to ϵ\epsilonϵ on [t0,+∞)[t_0,+\infty)[t0​,+∞); min⁡g=inf⁡g\min g=\inf gming=infg, attained since argmin⁡g≠∅\operatorname{argmin} g\ne\emptysetargming=∅; L1L^1L1 membership is Lebesgue integrability on [t0,+∞)[t_0,+\infty)[t0​,+∞) (never a comparison of a Bochner integral with a number); OOO, ooo are Asymptotics relations at +∞+\infty+∞.
  • Repair. Theorem 2.1 carries the extra hypothesis "β=0\beta=0β=0 or g∈C2g\in C^2g∈C2". As printed (only twice differentiable ggg) it is false for β>0\beta>0β>0: on R\mathbb RR, g′(x)=2x+x2sin⁡(1/x)g'(x)=2x+x^2\sin(1/x)g′(x)=2x+x2sin(1/x) gives a strongly convex ggg with bounded but discontinuous g′′g''g′′, and the solution from u0=0u_0=0u0​=0, v0=1v_0=1v0​=1 is not C2C^2C2. The paper's own proof uses continuity of ∇2g\nabla^2 g∇2g.
  • Flagged, not repaired. The last claim of Theorem 3.3, t2∥∇g(x(t))∥2∈L1t^2\|\nabla g(x(t))\|^2\in L^1t2∥∇g(x(t))∥2∈L1, is its own item: the paper's argument for it uses a term proportional to β\betaβ, so for β=0\beta=0β=0 the paper gives no proof. No counterexample is known, and the statement is drafted as printed.
  • Referenced, not re-posed. Lemma A.4 (continuous Opial lemma, p. 30), the last step of the goal's proof, is the published InertialAVD.Traj.lemma_A_2 (same hypotheses: SSS nonempty, lim⁡∥x(t)−z∥\lim\|x(t)-z\|lim∥x(t)−z∥ exists for every z∈Sz\in Sz∈S, every weak sequential limit point lies in SSS; same conclusion). It is a reference milestone of this mission; its weak convergence InertialAVD.Traj.WeakTendstoAtTop has the same body as TikhonovHDD.Weak.WeakTendstoAtTop.
  • The model is defined from scratch: the published HessianDamping.DINAVD.Setting concerns a different equation (no ϵx\epsilon xϵx term) and is not reused.
  • Welcome contributions: a general Cauchy–Lipschitz existence theorem for locally Lipschitz first-order systems in Banach spaces on [t0,+∞)[t_0,+\infty)[t0​,+∞) with a blow-up alternative, the continuous Opial lemma, and Lemma A.2 for absolutely continuous functions.

Selected references

  • R.I. Boţ, E.R. Csetnek, S.C. László, Tikhonov regularization of a second order dynamical system with Hessian driven damping, arXiv:1911.12845v2, 2020; published in Math. Program., https://doi.org/10.1007/s10107-020-01528-8. https://arxiv.org/abs/1911.12845v2
  • H. Attouch, J. Peypouquet, P. Redont, Fast convex optimization via inertial dynamics with Hessian driven damping, J. Differential Equations 261(10), 5734–5783, 2016. https://doi.org/10.1016/j.jde.2016.08.020
  • H. Attouch, Z. Chbani, H. Riahi, Combining fast inertial dynamics for convex optimization with Tikhonov regularization, J. Math. Anal. Appl. 457(2), 1065–1094, 2018. https://doi.org/10.1016/j.jmaa.2016.12.017
  • H. Attouch, Z. Chbani, J. Peypouquet, P. Redont, Fast convergence of inertial dynamics and algorithms with asymptotic vanishing viscosity, Math. Program. 168, 123–175, 2018. https://doi.org/10.1007/s10107-016-0992-8
  • W. Su, S. Boyd, E.J. Candès, A differential equation for modeling Nesterov's accelerated gradient method: theory and insights, J. Mach. Learn. Res. 17(153), 1–43, 2016. https://jmlr.org/papers/v17/15-084.html
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Tikhonov Regularization of a Second Order Dynamical System with Hessian Driven Damping 2: lim inf ‖x(t) − x*‖ = 0 at the Minimum-Norm Minimizer, and x(t) → x* If x(t) Ends In or Out of B(0, ‖x*‖)Research Paper

Motivation

Many methods for minimizing a smooth convex function ggg on a Hilbert space can be read as discretizations of second order ordinary differential equations, and the asymptotic behaviour of the continuous trajectories predicts the behaviour of the iterates. The inertial system with vanishing damping x¨+αtx˙+∇g(x)=0\ddot x+\frac{\alpha}{t}\dot x+\nabla g(x)=0x¨+tα​x˙+∇g(x)=0 is the continuous counterpart of Nesterov's accelerated gradient method (Su, Boyd, Candès 2016); for α>3\alpha>3α>3 its trajectories converge weakly to some minimizer of ggg (Attouch, Chbani, Peypouquet, Redont 2018). Two modifications of this system have been studied separately. A Hessian driven damping term β∇2g(x)x˙\beta\nabla^2g(x)\dot xβ∇2g(x)x˙ reduces oscillations while keeping the fast rate of the values (Attouch, Peypouquet, Redont 2016). A Tikhonov regularization term ϵ(t)x\epsilon(t)xϵ(t)x with ϵ(t)→0\epsilon(t)\to 0ϵ(t)→0 selects a particular minimizer: under suitable decay of ϵ\epsilonϵ, trajectories approach the minimizer of minimum norm in the strong (norm) topology (Attouch, Chbani, Riahi 2018).

Boţ, Csetnek and László (arXiv:1911.12845v2, published in Mathematical Programming 2021) combine both terms and ask which properties of the two separate systems survive. This mission formalizes their strong convergence result, Theorem 4.4.

Setting

Let H\mathcal HH be a real Hilbert space, t0>0t_0>0t0​>0, α≥3\alpha\ge 3α≥3, β≥0\beta\ge0β≥0, and u0,v0∈Hu_0,v_0\in\mathcal Hu0​,v0​∈H. The General assumption of the paper (p. 2) is:

  • g:H→Rg:\mathcal H\to\mathbb Rg:H→R is convex and twice Fréchet differentiable, ∇g\nabla g∇g is Lipschitz continuous on bounded sets, and argmin⁡g≠∅\operatorname{argmin} g\neq\emptysetargming=∅;
  • ϵ:[t0,+∞)→[0,+∞)\epsilon:[t_0,+\infty)\to[0,+\infty)ϵ:[t0​,+∞)→[0,+∞) is nonincreasing, of class C1C^1C1, and lim⁡t→+∞ϵ(t)=0\lim_{t\to+\infty}\epsilon(t)=0limt→+∞​ϵ(t)=0.

A global C2C^2C2-solution of the system

x¨(t)+αtx˙(t)+β∇2g(x(t))x˙(t)+∇g(x(t))+ϵ(t)x(t)=0,t≥t0,x(t0)=u0, x˙(t0)=v0,(5)\ddot x(t)+\frac{\alpha}{t}\dot x(t)+\beta\nabla^2g(x(t))\dot x(t)+\nabla g(x(t))+\epsilon(t)x(t)=0,\quad t\ge t_0,\qquad x(t_0)=u_0,\ \dot x(t_0)=v_0, \tag{5}x¨(t)+tα​x˙(t)+β∇2g(x(t))x˙(t)+∇g(x(t))+ϵ(t)x(t)=0,t≥t0​,x(t0​)=u0​, x˙(t0​)=v0​,(5)

is a twice continuously differentiable curve x:[t0,+∞)→Hx:[t_0,+\infty)\to\mathcal Hx:[t0​,+∞)→H satisfying (5) at every t≥t0t\ge t_0t≥t0​. The set argmin⁡g\operatorname{argmin} gargming is nonempty, closed and convex, so it has a unique element of minimum norm, denoted x∗x^*x∗. The open ball B(0,∥x∗∥)B(0,\|x^*\|)B(0,∥x∗∥) is {y:∥y∥<∥x∗∥}\{y:\|y\|<\|x^*\|\}{y:∥y∥<∥x∗∥}. In the Lean development these objects are GeneralAssumption g t₀ ε ε', IsSolution g α β t₀ ε u₀ v₀ x xd xdd and IsMinNormMinimizer g xstar in the namespace TikhonovHDD.Strong, with min⁡g\min gming written minValue g.

Formalization targets

Goal: Theorem 4.4 (p. 21)

Assume, in addition to the above,

∫t0+∞ϵ(t)t dt<+∞,lim⁡t→+∞βϵ(t)tα3+1∫t0tϵ2(s)sα3+1 ds=0,\int_{t_0}^{+\infty}\frac{\epsilon(t)}{t}\,dt<+\infty,\qquad \lim_{t\to+\infty}\frac{\beta}{\epsilon(t)t^{\frac{\alpha}{3}+1}}\int_{t_0}^{t}\epsilon^2(s)s^{\frac{\alpha}{3}+1}\,ds=0,∫t0​+∞​tϵ(t)​dt<+∞,t→+∞lim​ϵ(t)t3α​+1β​∫t0​t​ϵ2(s)s3α​+1ds=0,

that ϵ˙(t)≤−aβ2ϵ2(t)\dot\epsilon(t)\le-\frac{a\beta}{2}\epsilon^2(t)ϵ˙(t)≤−2aβ​ϵ2(t) for all t≥t1t\ge t_1t≥t1​, for some a>1a>1a>1 and t1≥t0t_1\ge t_0t1​≥t0​, and that lim⁡t→+∞t2ϵ(t)=+∞\lim_{t\to+\infty}t^2\epsilon(t)=+\inftylimt→+∞​t2ϵ(t)=+∞ if α=3\alpha=3α=3, while t2ϵ(t)≥23α(13α−1+βc2)t^2\epsilon(t)\ge\frac23\alpha\left(\frac13\alpha-1+\beta c^2\right)t2ϵ(t)≥32​α(31​α−1+βc2) for large ttt, for some c>0c>0c>0, if α>3\alpha>3α>3. Then

lim inf⁡t→+∞∥x(t)−x∗∥=0,\liminf_{t\to+\infty}\|x(t)-x^*\|=0,t→+∞liminf​∥x(t)−x∗∥=0,

and

lim⁡t→+∞∥x(t)−x∗∥=0\lim_{t\to+\infty}\|x(t)-x^*\|=0t→+∞lim​∥x(t)−x∗∥=0

if there exists T≥t0T\ge t_0T≥t0​ such that {x(t):t≥T}\{x(t):t\ge T\}{x(t):t≥T} stays either in B(0,∥x∗∥)B(0,\|x^*\|)B(0,∥x∗∥) or in its complement.

Milestones

  1. Lemma A.1 (p. 29): for nonnegative continuous integrable fff on (δ,+∞)(\delta,+\infty)(δ,+∞) and nondecreasing φ≥0\varphi\ge 0φ≥0 with φ(t)→+∞\varphi(t)\to+\inftyφ(t)→+∞, 1φ(t)∫δtφ(s)f(s) ds→0\frac1{\varphi(t)}\int_\delta^t\varphi(s)f(s)\,ds\to0φ(t)1​∫δt​φ(s)f(s)ds→0.
  2. Theorem 3.1 (pp. 5–6): for α≥3\alpha\ge3α≥3, g(x(t))→min⁡gg(x(t))\to\min gg(x(t))→ming under either (a) ∫t0+∞ϵ(t)/t dt<+∞\int_{t_0}^{+\infty}\epsilon(t)/t\,dt<+\infty∫t0​+∞​ϵ(t)/tdt<+∞ together with ϵ˙≤−aβ2ϵ2\dot\epsilon\le-\frac{a\beta}{2}\epsilon^2ϵ˙≤−2aβ​ϵ2 eventually, or (b) ϵ(t)≤a/t\epsilon(t)\le a/tϵ(t)≤a/t eventually.
  3. Case I of the proof of Theorem 4.4 (pp. 21–25): the trajectory eventually stays outside the open ball, and x(t)→x∗x(t)\to x^*x(t)→x∗.
  4. Case II (pp. 25–26): the trajectory eventually stays inside the open ball, and x(t)→x∗x(t)\to x^*x(t)→x∗.
  5. Case III (p. 26): the trajectory is inside and outside the ball for arbitrarily large times, and lim inf⁡∥x(t)−x∗∥=0\liminf\|x(t)-x^*\|=0liminf∥x(t)−x∗∥=0.

The three cases are exhaustive, so Cases I–III together give the goal.

Significance

Theorem 4.4 shows that adding Hessian driven damping does not destroy the selection property of Tikhonov regularization: the trajectory comes arbitrarily close to the minimum-norm minimizer, and converges to it in norm whenever it does not oscillate across the sphere ∥y∥=∥x∗∥\|y\|=\|x^*\|∥y∥=∥x∗∥ forever. Since ϵ(t)→0\epsilon(t)\to 0ϵ(t)→0, the system still approaches argmin⁡g\operatorname{argmin} gargming, but the limit is a canonical minimizer determined by ggg alone, not by the initial data. In infinite dimensions this is the difference between weak and strong convergence, a distinction that matters for ill-posed problems and inverse problems, where the minimum-norm solution is the one usually sought. Remark 4.5 of the paper compares the hypotheses with those of Attouch, Chbani and Riahi for the system without Hessian damping: for β=0\beta=0β=0 the lower bound required of t2ϵ(t)t^2\epsilon(t)t2ϵ(t) when α>3\alpha>3α>3 is, in the authors' words, "less tight" than theirs.

The result is proved in the paper; no part of it has a machine-checked proof. Formalizing it requires a Lyapunov-energy argument for a second order ODE in a Hilbert space, the weak lower semicontinuity of convex functions and of the norm, and the passage from weak to strong convergence via convergence of norms. Theorem 3.1 and Lemma A.1 are standalone results reusable for other Tikhonov-regularized inertial systems.

Difficulty

The weak convergence argument for the unregularized system (Opial's lemma) does not identify the limit, and it does not give strong convergence. Tikhonov regularization supplies the identification only through the Tikhonov curve xϵx_{\epsilon}xϵ​, the minimizer of g+ϵ2∥⋅∥2g+\frac{\epsilon}{2}\|\cdot\|^2g+2ϵ​∥⋅∥2, and comparing x(t)x(t)x(t) with xϵ(t)x_{\epsilon(t)}xϵ(t)​ requires an energy whose derivative is controlled with weights tuned to α\alphaα. The Hessian term produces cross terms of the form βϵ(t)t2⟨∇g(x(t)),x(t)⟩\beta\epsilon(t)t^2\langle\nabla g(x(t)),x(t)\rangleβϵ(t)t2⟨∇g(x(t)),x(t)⟩ that are absent from the system without Hessian damping; the integral hypothesis on ϵ2(s)sα/3+1\epsilon^2(s)s^{\alpha/3+1}ϵ2(s)sα/3+1 and the slow-decay condition ϵ˙≤−aβ2ϵ2\dot\epsilon\le-\frac{a\beta}{2}\epsilon^2ϵ˙≤−2aβ​ϵ2 exist to absorb them. A direct energy estimate only works when ∥x(t)∥≥∥x∗∥\|x(t)\|\ge\|x^*\|∥x(t)∥≥∥x∗∥; inside the ball a different argument is required, and when the trajectory crosses the sphere infinitely often neither argument yields convergence of the whole trajectory, only a liminf statement.

Formalization scope

Conventions committed to in Lean:

  • Curves are maps R→H\mathbb R\to\mathcal HR→H; only their values on [t0,+∞)[t_0,+\infty)[t0​,+∞) matter. Derivatives of xxx, x˙\dot xx˙ and ϵ\epsilonϵ are taken within [t0,+∞)[t_0,+\infty)[t0​,+∞) (one-sided at t0t_0t0​) and passed as explicit maps xd, xdd, ε'; x¨\ddot xx¨ and ϵ˙\dot\epsilonϵ˙ are continuous there.
  • ∇g\nabla g∇g is gradient g; ∇2g(x)v\nabla^2g(x)v∇2g(x)v is the Fréchet derivative of gradient g at xxx applied to vvv. "Lipschitz on bounded sets" means Lipschitz on every closed ball centred at 000.
  • min⁡g\min gming is the infimum of the range of ggg, attained because argmin⁡g≠∅\operatorname{argmin} g\neq\emptysetargming=∅.
  • ∫t0+∞ϵ(t)/t dt<+∞\int_{t_0}^{+\infty}\epsilon(t)/t\,dt<+\infty∫t0​+∞​ϵ(t)/tdt<+∞ is Lebesgue integrability of ϵ(t)/t\epsilon(t)/tϵ(t)/t on [t0,+∞)[t_0,+\infty)[t0​,+∞), never a comparison of a Bochner integral with a number. tα/3+1t^{\alpha/3+1}tα/3+1 is the real power.
  • lim inf⁡t→+∞∥x(t)−x∗∥=0\liminf_{t\to+\infty}\|x(t)-x^*\|=0liminft→+∞​∥x(t)−x∗∥=0 is written as: for every δ>0\delta>0δ>0, ∥x(t)−x∗∥<δ\|x(t)-x^*\|<\delta∥x(t)−x∗∥<δ for arbitrarily large ttt. Lean's Filter.liminf is not used, since it returns 000 for a function tending to +∞+\infty+∞.
  • The alternative "in the ball or in its complement" uses one TTT for both branches, with the disjunction outside the universal quantifier. Placing the disjunction inside (∀t≥T\forall t\ge T∀t≥T, ∥x(t)∥<∥x∗∥\|x(t)\|<\|x^*\|∥x(t)∥<∥x∗∥ or ∥x(t)∥≥∥x∗∥\|x(t)\|\ge\|x^*\|∥x(t)∥≥∥x∗∥) would make the hypothesis always true and the strong convergence claim unconditional, which the paper does not prove.
  • Every statement is made for every global C2C^2C2-solution of (5). Existence and uniqueness of that solution (Theorem 2.1 of the paper) is a separate result, formalized in the companion mission on weak convergence; the hypothesis is not vacuous.
  • No positivity of ϵ\epsilonϵ is assumed: it follows from the conditions for α=3\alpha=3α=3 and α>3\alpha>3α>3.
  • Cases I–III carry the full hypothesis list of Theorem 4.4, although Case II uses only part of it.

No statement of the mission has been repaired against the printed text.

A complete development needs: weak lower semicontinuity of convex continuous functions and of the norm on Hilbert spaces; weak sequential compactness of bounded sets; existence of the minimum-norm element of a closed convex set (Mathlib's projection onto closed convex sets); the strongly convex Tikhonov curve and its convergence to x∗x^*x∗; and calculus for energy functionals along C2C^2C2 curves on half-lines. Lemma A.1 and the Tikhonov-curve facts are reusable for every Tikhonov-regularized dynamics. Contributions of proofs of individual milestones, of supporting lemmas, and of alternative arguments are welcome.

Selected references

  • R.I. Boţ, E.R. Csetnek, S.C. László, Tikhonov regularization of a second order dynamical system with Hessian driven damping, arXiv:1911.12845v2, 2020; Mathematical Programming 189, 151–186, 2021. https://arxiv.org/abs/1911.12845v2, https://doi.org/10.1007/s10107-020-01528-8
  • H. Attouch, Z. Chbani, H. Riahi, Combining fast inertial dynamics for convex optimization with Tikhonov regularization, Journal of Mathematical Analysis and Applications 457, 1065–1094, 2018. https://doi.org/10.1016/j.jmaa.2016.12.017
  • H. Attouch, J. Peypouquet, P. Redont, Fast convex optimization via inertial dynamics with Hessian driven damping, Journal of Differential Equations 261(10), 5734–5783, 2016. https://doi.org/10.1016/j.jde.2016.08.020
  • H. Attouch, Z. Chbani, J. Peypouquet, P. Redont, Fast convergence of inertial dynamics and algorithms with asymptotic vanishing viscosity, Mathematical Programming 168, 123–175, 2018. https://doi.org/10.1007/s10107-016-0992-8
  • W. Su, S. Boyd, E.J. Candès, A differential equation for modeling Nesterov's accelerated gradient method: theory and insights, Journal of Machine Learning Research 17(153), 1–43, 2016. https://jmlr.org/papers/v17/15-084.html
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Sparse Regression at Scale: Branch-and-Bound rooted in First-Order Optimization 1: The Perspective Interval Relaxation Is a Least Squares Problem with a Separable Reverse-Huber or ℓ1 PenaltyResearch Paper

Motivation

Best subset selection with ridge shrinkage asks for a sparse linear model: given a design matrix X∈Rn×pX\in\mathbb R^{n\times p}X∈Rn×p and responses y∈Rny\in\mathbb R^ny∈Rn, minimize

12∥y−Xβ∥22+λ0∥β∥0+λ2∥β∥22,\tfrac12\|y-X\beta\|_2^2+\lambda_0\|\beta\|_0+\lambda_2\|\beta\|_2^2 ,21​∥y−Xβ∥22​+λ0​∥β∥0​+λ2​∥β∥22​,

where ∥β∥0\|\beta\|_0∥β∥0​ counts nonzero coefficients. The problem is NP-hard, and exact methods solve it as a mixed integer program by branch-and-bound (Bertsimas, King, Mazumder 2016). The speed of branch-and-bound is governed by two things: how tight the continuous relaxation at each node is, and how cheaply that relaxation can be solved.

Hazimeh, Mazumder and Saab (arXiv:2004.06152v2; Mathematical Programming 2022) build a branch-and-bound solver whose node relaxations are solved by first-order methods rather than by a conic interior-point solver. Their starting point is the perspective formulation, a standard device for strengthening relaxations of mixed integer programs with indicator variables (Frangioni, Gentile 2006; Günlük, Linderoth 2010). Theorem 1 of the paper shows that the interval relaxation of this formulation is a box-constrained least squares problem with a separable penalty in β\betaβ alone. This mission formalizes Theorem 1.

Timeline. Owen (2007) introduced the reverse Huber penalty as a hybrid of lasso and ridge. Dong, Chen, Linderoth (2015) showed that the interval relaxation of the perspective formulation without a Big-M bound reduces to least squares with a reverse Huber penalty. Hazimeh, Mazumder and Saab (2020–2021) added the Big-M constraint and obtained Theorem 1, with a second regime in which the penalty becomes ℓ1\ell_1ℓ1​.

Setting

Fix X∈Rn×pX\in\mathbb R^{n\times p}X∈Rn×p, y∈Rny\in\mathbb R^ny∈Rn, λ0>0\lambda_0>0λ0​>0, λ2>0\lambda_2>0λ2​>0 and M>0M>0M>0, and write [p]={1,…,p}[p]=\{1,\dots,p\}[p]={1,…,p}. The perspective formulation PR(M)\mathrm{PR}(M)PR(M) is problem (3) of the paper:

min⁡β,z,s 12∥y−Xβ∥22+λ0∑i∈[p]zi+λ2∑i∈[p]sis.t.βi2≤sizi,  −Mzi≤βi≤Mzi,  zi∈{0,1},  si≥0.\min_{\beta,z,s}\ \tfrac12\|y-X\beta\|_2^2+\lambda_0\sum_{i\in[p]}z_i+\lambda_2\sum_{i\in[p]}s_i \quad\text{s.t.}\quad \beta_i^2\le s_iz_i,\ \ -Mz_i\le\beta_i\le Mz_i,\ \ z_i\in\{0,1\},\ \ s_i\ge0 .β,z,smin​ 21​∥y−Xβ∥22​+λ0​i∈[p]∑​zi​+λ2​i∈[p]∑​si​s.t.βi2​≤si​zi​,  −Mzi​≤βi​≤Mzi​,  zi​∈{0,1},  si​≥0.

Here ziz_izi​ indicates whether βi\beta_iβi​ may be nonzero, sis_isi​ stands in for βi2\beta_i^2βi2​ through the rotated second-order cone constraint βi2≤sizi\beta_i^2\le s_iz_iβi2​≤si​zi​, and MMM bounds ∣βi∣|\beta_i|∣βi​∣. The interval relaxation replaces zi∈{0,1}z_i\in\{0,1\}zi​∈{0,1} with zi∈[0,1]z_i\in[0,1]zi​∈[0,1].

The reverse Huber penalty (4) is B(t)=∣t∣\mathcal B(t)=|t|B(t)=∣t∣ for ∣t∣≤1|t|\le1∣t∣≤1 and B(t)=(t2+1)/2\mathcal B(t)=(t^2+1)/2B(t)=(t2+1)/2 for ∣t∣≥1|t|\ge1∣t∣≥1. Put

ψ1(b;λ0,λ2)=2λ0 B(bλ2/λ0),ψ2(b;λ0,λ2,M)=(λ0M+λ2M)∣b∣,\psi_1(b;\lambda_0,\lambda_2)=2\lambda_0\,\mathcal B\big(b\sqrt{\lambda_2/\lambda_0}\big),\qquad \psi_2(b;\lambda_0,\lambda_2,M)=\Big(\frac{\lambda_0}{M}+\lambda_2M\Big)|b|,ψ1​(b;λ0​,λ2​)=2λ0​B(bλ2​/λ0​​),ψ2​(b;λ0​,λ2​,M)=(Mλ0​​+λ2​M)∣b∣,

and let ψ=ψ1\psi=\psi_1ψ=ψ1​ if λ0/λ2≤M\sqrt{\lambda_0/\lambda_2}\le Mλ0​/λ2​​≤M and ψ=ψ2\psi=\psi_2ψ=ψ2​ if λ0/λ2>M\sqrt{\lambda_0/\lambda_2}>Mλ0​/λ2​​>M. The reduced relaxation (5) is

min⁡β∈Rp F(β):=12∥y−Xβ∥22+∑i∈[p]ψ(βi;λ0,λ2,M)s.t.∥β∥∞≤M,\min_{\beta\in\mathbb R^p}\ F(\beta):=\tfrac12\|y-X\beta\|_2^2+\sum_{i\in[p]}\psi(\beta_i;\lambda_0,\lambda_2,M)\quad\text{s.t.}\quad\|\beta\|_\infty\le M ,β∈Rpmin​ F(β):=21​∥y−Xβ∥22​+i∈[p]∑​ψ(βi​;λ0​,λ2​,M)s.t.∥β∥∞​≤M,

with optimal value VPR(M)V_{\mathrm{PR}(M)}VPR(M)​. For one coordinate bbb, ω(b;λ0,λ2,M)\omega(b;\lambda_0,\lambda_2,M)ω(b;λ0​,λ2​,M) is the minimum of λ0z+λ2s\lambda_0z+\lambda_2sλ0​z+λ2​s over b2≤szb^2\le szb2≤sz, −Mz≤b≤Mz-Mz\le b\le Mz−Mz≤b≤Mz, z∈[0,1]z\in[0,1]z∈[0,1], s≥0s\ge0s≥0.

Formalization targets

Goal: Theorem 1 (Reduced Relaxation), p. 6

The interval relaxation of (3) is equivalent to (5):

∃ (z,s): (β,z,s) feasible  ⟺  ∥β∥∞≤M,min⁡z,s{12∥y−Xβ∥22+λ0∑izi+λ2∑isi}=F(β)  (∥β∥∞≤M),\exists\,(z,s):\ (\beta,z,s)\ \text{feasible}\iff\|\beta\|_\infty\le M,\qquad \min_{z,s}\Big\{\tfrac12\|y-X\beta\|_2^2+\lambda_0\textstyle\sum_i z_i+\lambda_2\sum_i s_i\Big\}=F(\beta)\ \ (\|\beta\|_\infty\le M),∃(z,s): (β,z,s) feasible⟺∥β∥∞​≤M,z,smin​{21​∥y−Xβ∥22​+λ0​∑i​zi​+λ2​∑i​si​}=F(β)  (∥β∥∞​≤M),

and both problems attain the common optimal value VPR(M)V_{\mathrm{PR}(M)}VPR(M)​.

Milestones (proof of Theorem 1, p. 28)

  1. Reduction to (36). For ∣b∣≤M|b|\le M∣b∣≤M, the smallest feasible zzz is z^=max⁡{b2/s,∣b∣/M}\hat z=\max\{b^2/s,|b|/M\}z^=max{b2/s,∣b∣/M}, so
ω(b;λ0,λ2,M)=min⁡s≥b2max⁡{λ0b2s+λ2s, λ0∣b∣M+λ2s}.\omega(b;\lambda_0,\lambda_2,M)=\min_{s\ge b^2}\max\Big\{\lambda_0\tfrac{b^2}{s}+\lambda_2s,\ \lambda_0\tfrac{|b|}{M}+\lambda_2s\Big\}.ω(b;λ0​,λ2​,M)=s≥b2min​max{λ0​sb2​+λ2​s, λ0​M∣b∣​+λ2​s}.
  1. Case I. If λ0/λ2≤M\sqrt{\lambda_0/\lambda_2}\le Mλ0​/λ2​​≤M and ∣b∣≤M|b|\le M∣b∣≤M, then ω(b;λ0,λ2,M)=2λ0B(bλ2/λ0)\omega(b;\lambda_0,\lambda_2,M)=2\lambda_0\mathcal B(b\sqrt{\lambda_2/\lambda_0})ω(b;λ0​,λ2​,M)=2λ0​B(bλ2​/λ0​​).
  2. Case II. If λ0/λ2>M\sqrt{\lambda_0/\lambda_2}>Mλ0​/λ2​​>M and ∣b∣≤M|b|\le M∣b∣≤M, then ω(b;λ0,λ2,M)=(λ0/M+λ2M)∣b∣\omega(b;\lambda_0,\lambda_2,M)=(\lambda_0/M+\lambda_2M)|b|ω(b;λ0​,λ2​,M)=(λ0​/M+λ2​M)∣b∣.

Significance

The result. Theorem 1 removes the 2p2p2p auxiliary variables z,sz,sz,s and all conic constraints from the node relaxation. What remains is a composite problem, a smooth least squares loss plus a separable, convex penalty under a box constraint, to which coordinate descent and proximal methods apply directly. The paper's solver, its active-set strategy, and the dual bounds of its Section 3 are all built on (5). The theorem also exposes a regime change: when λ0/λ2>M\sqrt{\lambda_0/\lambda_2}>Mλ0​/λ2​​>M, the ridge term of the perspective formulation disappears from the relaxation and the penalty is pure ℓ1\ell_1ℓ1​. Propositions 1 and 2 of the paper, which compare the strengths of the perspective, Big-M and PR(∞)\mathrm{PR}(\infty)PR(∞) relaxations, use this reduced form.

Formalizing it. The result is proved in the paper (Appendix A) by a coordinatewise argument. To our knowledge it has no machine-checked proof. Formalizing it gives a verified bridge from the conic mixed integer formulation to the penalized form that later results of the paper use, and a checked case analysis at the regime boundary λ0/λ2=M\sqrt{\lambda_0/\lambda_2}=Mλ0​/λ2​​=M, where the two formulas must agree with the stated tie-breaking.

Difficulty

The obvious approach, "minimize over zzz and sss coordinate by coordinate", is correct in outline, but each step hides a boundary case. The rotated cone constraint βi2≤sizi\beta_i^2\le s_iz_iβi2​≤si​zi​ degenerates at si=0s_i=0si​=0 or zi=0z_i=0zi​=0, where βi2/si\beta_i^2/s_iβi2​/si​ is undefined, and the paper's convention for βi=si=0\beta_i=s_i=0βi​=si​=0 must be handled. The one-variable problem (36) is a minimum of a pointwise maximum of two functions of sss, one convex and decreasing then increasing, the other increasing. Its minimizer lies either in the interior of the region where the first term dominates or on the crossover s=∣b∣Ms=|b|Ms=∣b∣M, depending on the regime. The paper's proof describes the cases loosely: it optimizes the Case I term without imposing the side condition that Case I attains the maximum. A complete argument must prove the lower bound over all feasible sss, not just evaluate at a candidate. Finally, the minimum over (z,s)∈R2p(z,s)\in\mathbb R^{2p}(z,s)∈R2p must be shown to split into a sum of coordinate minima, each attained.

Formalization scope

Data are X : Matrix (Fin n) (Fin p) ℝ, y : Fin n → ℝ, and reals lam0 lam2 M with 0 < lam0, 0 < lam2, 0 < M; the paper's [p][p][p] is Fin p. The squared norm ∥y−Xβ∥22\|y-X\beta\|_2^2∥y−Xβ∥22​ is the explicit sum ∑r(yr−(Xβ)r)2\sum_r(y_r-(X\beta)_r)^2∑r​(yr​−(Xβ)r​)2, and ∥β∥∞≤M\|\beta\|_\infty\le M∥β∥∞​≤M is ∣βi∣≤M|\beta_i|\le M∣βi​∣≤M for all iii. The cone constraint is kept in product form βi2≤sizi\beta_i^2\le s_iz_iβi2​≤si​zi​. In z^\hat zz^ and (36), Lean's b2/0=0b^2/0=0b2/0=0 coincides with the paper's convention βi2/si=0\beta_i^2/s_i=0βi2​/si​=0 for βi=si=0\beta_i=s_i=0βi​=si​=0. Every "min" is stated with IsLeast (membership plus lower bound), so attainment is part of each statement. VPR(M)V_{\mathrm{PR}(M)}VPR(M)​ is defined as a real infimum over the box, and Theorem 1 asserts that this infimum is attained by both problems. No normalization of XXX or yyy is assumed; the paper's unit-norm assumption starts in Section 3. The paper writes no O(⋅)O(\cdot)O(⋅) in these results, so there are no constants to instantiate.

A goal stating only one inequality (that F(β)F(\beta)F(β) is achieved by some (z,s)(z,s)(z,s), or that it bounds the relaxation from below), or a goal over zi∈{0,1}z_i\in\{0,1\}zi​∈{0,1}, would not be Theorem 1. The IsLeast form rules out both. The goal uses ψ\psiψ with both regimes.

A complete development needs: a two-variable convexity argument for λ0b2/s+λ2s\lambda_0b^2/s+\lambda_2sλ0​b2/s+λ2​s on s>0s>0s>0; a lemma that the infimum of a separable objective over a product of feasible sets is the sum of the coordinate infima; and continuity of FFF with compactness of the box to obtain an optimal β\betaβ. The coordinate lemmas and the definition of the reverse Huber penalty are reusable in the companion missions on relaxation strength and Lagrangian duality. Contributions to any milestone, or an alternative proof of the goal, are welcome.

Selected references

  • H. Hazimeh, R. Mazumder, A. Saab, Sparse Regression at Scale: Branch-and-Bound rooted in First-Order Optimization, arXiv:2004.06152v2 (2021); Mathematical Programming (2022). https://arxiv.org/abs/2004.06152v2
  • A. Frangioni, C. Gentile, Perspective cuts for a class of convex 0–1 mixed integer programs, Mathematical Programming 106(2), 225–236, 2006. https://doi.org/10.1007/s10107-005-0594-3
  • O. Günlük, J. Linderoth, Perspective reformulations of mixed integer nonlinear programs with indicator variables, Mathematical Programming 124(1–2), 183–205, 2010. https://doi.org/10.1007/s10107-010-0360-z
  • H. Dong, K. Chen, J. Linderoth, Regularization vs. Relaxation: A conic optimization perspective of statistical variable selection, arXiv:1510.06083, 2015. https://arxiv.org/abs/1510.06083
  • A. B. Owen, A robust hybrid of lasso and ridge regression, Contemporary Mathematics 443, 59–72, 2007. https://doi.org/10.1090/conm/443/08555
  • D. Bertsimas, A. King, R. Mazumder, Best subset selection via a modern optimization lens, Annals of Statistics 44(2), 813–852, 2016. https://doi.org/10.1214/15-AOS1388
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Optimization·Captain: mikedeng1

The Direct Extension of ADMM for Multi-block Convex Minimization Problems is Not Necessarily Convergent III: With a Strongly Convex Objective and β = 1 the Extended ADMM Can Still DivergeResearch Paper

Motivation

The alternating direction method of multipliers (ADMM) is a standard method for convex problems whose objective splits into two blocks coupled by a linear constraint (Gabay & Mercier 1976; Boyd et al. 2011). Many models in imaging, statistics and sparse or low-rank recovery have three or more blocks, and the scheme practitioners reach for first is the direct extension of ADMM: minimize the augmented Lagrangian over each block in turn, then update the multiplier. For years it was unknown whether this scheme converges in general.

Chen, He, Ye and Yuan (Math. Program., 2016) settled the question negatively: on a three-variable linear system with zero objective, the direct extension diverges for every penalty parameter (their Theorem 3.1). Their Section 4.1 then asks whether strong convexity of the objective rescues convergence. Han and Yuan (J. Optim. Theory Appl., 2012) had proved convergence for strongly convex objectives under a restriction on the penalty parameter determined by the strong convexity moduli. Theorem 4.1 shows that this restriction cannot simply be removed. This mission formalizes Theorem 4.1 and the three facts on p. 14 that support it.

Timeline:

  • 1975–1976: Glowinski–Marrocco and Gabay–Mercier introduce two-block ADMM and prove its convergence.
  • 2012: Han and Yuan prove convergence of the multi-block direct extension when every θi\theta_iθi​ is strongly convex and β\betaβ is small enough.
  • 2014 (authors' version), published 2016: Chen, He, Ye and Yuan give the first divergent example (Theorem 3.1) and its strongly convex variant (Theorem 4.1).

Setting

The three-block problem (1.1) is

min⁡ θ1(x1)+θ2(x2)+θ3(x3)s.t.A1x1+A2x2+A3x3=b,xi∈Xi,\min\ \theta_1(x_1)+\theta_2(x_2)+\theta_3(x_3)\quad\text{s.t.}\quad A_1x_1+A_2x_2+A_3x_3=b,\quad x_i\in\mathcal X_i,min θ1​(x1​)+θ2​(x2​)+θ3​(x3​)s.t.A1​x1​+A2​x2​+A3​x3​=b,xi​∈Xi​,

with Ai∈Rp×niA_i\in\mathbb R^{p\times n_i}Ai​∈Rp×ni​, b∈Rpb\in\mathbb R^pb∈Rp, closed convex sets Xi⊆Rni\mathcal X_i\subseteq\mathbb R^{n_i}Xi​⊆Rni​ and convex functions θi:Rni→R\theta_i:\mathbb R^{n_i}\to\mathbb Rθi​:Rni​→R; the solution set is assumed nonempty.

For a penalty parameter β>0\beta>0β>0 and a multiplier λ∈Rp\lambda\in\mathbb R^pλ∈Rp, the augmented Lagrangian (1.6) is

LA(x1,x2,x3,λ)=∑i=13θi(xi)−λT(A1x1+A2x2+A3x3−b)+β2∥A1x1+A2x2+A3x3−b∥2.\mathcal L_{\mathcal A}(x_1,x_2,x_3,\lambda)=\sum_{i=1}^3\theta_i(x_i)-\lambda^T(A_1x_1+A_2x_2+A_3x_3-b)+\frac\beta2\|A_1x_1+A_2x_2+A_3x_3-b\|^2 .LA​(x1​,x2​,x3​,λ)=i=1∑3​θi​(xi​)−λT(A1​x1​+A2​x2​+A3​x3​−b)+2β​∥A1​x1​+A2​x2​+A3​x3​−b∥2.

The direct extension of ADMM (1.5) starts from (x20,x30,λ0)(x_2^0,x_3^0,\lambda^0)(x20​,x30​,λ0) and, for k≥0k\ge0k≥0, sets x1k+1x_1^{k+1}x1k+1​, x2k+1x_2^{k+1}x2k+1​, x3k+1x_3^{k+1}x3k+1​ to minimizers of LA\mathcal L_{\mathcal A}LA​ over X1,X2,X3\mathcal X_1,\mathcal X_2,\mathcal X_3X1​,X2​,X3​ in that order, each with the newest values of the other blocks, and then sets λk+1=λk−β(A1x1k+1+A2x2k+1+A3x3k+1−b)\lambda^{k+1}=\lambda^k-\beta(A_1x_1^{k+1}+A_2x_2^{k+1}+A_3x_3^{k+1}-b)λk+1=λk−β(A1​x1k+1​+A2​x2k+1​+A3​x3k+1​−b).

A function fff is mmm-strongly convex if f−m2∥⋅∥2f-\frac m2\|\cdot\|^2f−2m​∥⋅∥2 is convex.

The instance (4.1) is

min⁡ 0.05x12+0.05x22+0.05x32s.t.(111112122)(x1x2x3)=0,\min\ 0.05x_1^2+0.05x_2^2+0.05x_3^2\quad\text{s.t.}\quad\begin{pmatrix}1&1&1\\1&1&2\\1&2&2\end{pmatrix}\begin{pmatrix}x_1\\x_2\\x_3\end{pmatrix}=0,min 0.05x12​+0.05x22​+0.05x32​s.t.​111​112​122​​​x1​x2​x3​​​=0,

with scalar xix_ixi​, Xi=R\mathcal X_i=\mathbb RXi​=R and b=0b=0b=0. Its unique solution is x=0x=0x=0. For β=1\beta=1β=1 the state after an iteration is z=(x2,x3,λ1,λ2,λ3)∈R5z=(x_2,x_3,\lambda_1,\lambda_2,\lambda_3)\in\mathbb R^5z=(x2​,x3​,λ1​,λ2​,λ3​)∈R5, and M41M_{41}M41​ denotes the 5×55\times55×5 iteration matrix that maps zkz^kzk to zk+1z^{k+1}zk+1.

Formalization targets

Goal: Theorem 4.1

For the model (1.1) with strongly convex objective, (1.5) is not necessarily convergent for all β>0\beta>0β>0. Formally, (4.1) satisfies the standing assumptions, each θi\theta_iθi​ is 110\tfrac1{10}101​-strongly convex, and at β=1\beta=1β=1 there is a starting point (x20,x30,λ0)(x_2^0,x_3^0,\lambda^0)(x20​,x30​,λ0) from which a run of (1.5) exists and

no run (x1k,x2k,x3k,λk)k≥0 of (1.5) from it converges.\text{no run }(x_1^k,x_2^k,x_3^k,\lambda^k)_{k\ge0}\text{ of (1.5) from it converges.}no run (x1k​,x2k​,x3k​,λk)k≥0​ of (1.5) from it converges.

The goal fixes the witness instance and β=1\beta=1β=1, because those are what the paper computes. It does not fix the starting point.

Milestones

  1. Fixed matrix mapping. Every run of (1.5) on (4.1) with β=1\beta=1β=1 satisfies zk+1=M41zkz^{k+1}=M_{41}z^kzk+1=M41​zk for all kkk, with the explicit rational matrix M41M_{41}M41​.
  2. Spectral radius. ρ(M41)\rho(M_{41})ρ(M41​), the largest modulus of a complex eigenvalue, lies in [1.00865,1.00875)[1.00865,1.00875)[1.00865,1.00875), i.e. equals 1.00871.00871.0087 to the four decimals of the page.
  3. Diverging powers. Some real z∈R5z\in\mathbb R^5z∈R5 has ∥M41kz∥→∞\|M_{41}^kz\|\to\infty∥M41k​z∥→∞.

Significance

Theorem 4.1 says that strong convexity of each θi\theta_iθi​, on its own, does not make the three-block direct extension of ADMM converge. Convergence results for strongly convex models therefore have to restrict β\betaβ, as Han and Yuan do, or modify the scheme. Examples of modified schemes are a shrunken multiplier step (discussed in §4.2 of the paper) and Gaussian back substitution (He, Tao & Yuan 2012). The example is also a concrete test case: any proposed sufficient condition for convergence has to exclude (4.1) at β=1\beta=1β=1.

The theorem is proved in the paper, but only in outline: the iteration matrix is not printed, the spectral radius is reported as the outcome of "a simple calculation", and the construction of a divergent starting point is "omitted for succinctness". A formalization makes each step explicit and machine-checked. That means the exact iteration matrix, a certified enclosure of its spectral radius, and a real starting point whose iterates are unbounded. As far as is known, none of these results has been machine-checked.

Difficulty

There are three separate difficulties.

  • Reduction to a matrix. The method is defined by three minimizations, not by a formula, so the matrix recursion has to be derived from those minimizations.
  • Certifying the spectral radius. The spectral radius is a property of a degree-5 characteristic polynomial with large rational coefficients. Its dominant roots are a non-real conjugate pair of modulus about 1.008741.008741.00874, so the margin above 111 is under one percent, and the rounding interval requested is narrow.
  • From eigenvalue to divergence. A spectral radius above 111 does not by itself give a divergent real trajectory. The dominant eigenvectors are complex, and the starting vector must be real yet have a nonzero component along the expanding pair.

A natural first idea is to argue that strong convexity of the objective forces the iterates toward the unique solution. This fails because the multiplier and the coupling between blocks are not controlled by the objective's curvature once β\betaβ is large relative to the moduli.

Formalization scope

Vectors in Rn\mathbb R^nRn are Fin n → ℝ and matrices are Matrix (Fin p) (Fin n) ℝ. The Euclidean square norm in (1.6) is written r⋅rr\cdot rr⋅r (⬝ᵥ), never Mathlib's sup norm. Norms appear otherwise only in "∥⋅∥→∞\|\cdot\|\to\infty∥⋅∥→∞", where every norm on R5\mathbb R^5R5 gives the same meaning. Blocks are separate fields, and multiplier components are 0-based. A run is a predicate on sequences: "xk+1=Argmin⁡x^{k+1}=\operatorname{Argmin}xk+1=Argmin" means "xk+1x^{k+1}xk+1 is a minimizer", and x10x_1^0x10​ is never read. "Converges" means convergence of (x1k,x2k,x3k,λk)(x_1^k,x_2^k,x_3^k,\lambda^k)(x1k​,x2k​,x3k​,λk) in the product topology.

Strong convexity is Mathlib's StrongConvexOn Set.univ (1/10). The paper's "closed convex" θi\theta_iθi​ are real-valued on all of Rni\mathbb R^{n_i}Rni​, hence continuous, so only convexity is stated.

The quantifier "for all β>0\beta>0β>0" is read as "not for every β>0\beta>0β>0", witnessed at β=1\beta=1β=1. The stronger reading, divergence for every β\betaβ, is false for (4.1), where the spectral radius is below 111 for small β\betaβ.

Trivializations ruled out. The goal asserts the existence of a run, so non-convergence cannot hold vacuously. Runs are characterized by minimizer conditions rather than an argmin choice function with junk values. Spectral statements are over C\mathbb CC rather than over real eigenvalues only; the only real eigenvalue of M41M_{41}M41​ is 000.

What a complete development needs: first-order optimality for strictly convex scalar quadratics; existence and uniqueness of the subproblem minimizers; a certified root enclosure for a quartic with rational coefficients (via Rouché-type bounds, interval arithmetic or an explicit factorization over R\mathbb RR); and the passage from a dominant complex eigenpair to a real unbounded orbit. The last two are reusable for any linear-iteration divergence argument, including Theorem 3.1 of the same paper. Contributions of any of these lemmas, as separate theorems, are welcome.

Selected references

  • C. Chen, B. He, Y. Ye, X. Yuan, The direct extension of ADMM for multi-block convex minimization problems is not necessarily convergent, Math. Program. 155 (2016) 57–79. https://doi.org/10.1007/s10107-014-0826-5
  • D. Han, X. Yuan, A note on the alternating direction method of multipliers, J. Optim. Theory Appl. 155 (2012) 227–238. https://doi.org/10.1007/s10957-012-0003-z
  • D. Gabay, B. Mercier, A dual algorithm for the solution of nonlinear variational problems via finite element approximation, Comput. Math. Appl. 2 (1976) 17–40. https://doi.org/10.1016/0898-1221(76)90003-1
  • S. Boyd, N. Parikh, E. Chu, B. Peleato, J. Eckstein, Distributed optimization and statistical learning via the alternating direction method of multipliers, Found. Trends Mach. Learn. 3 (2011) 1–122. https://doi.org/10.1561/2200000016
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Optimization·Captain: mikedeng1

Error Bounds, Quadratic Growth, and Linear Convergence of Proximal Methods I: For the Proximal Gradient Method, the Error Bound Condition Is Equivalent to Quadratic GrowthResearch Paper

Motivation

A large share of the optimization problems solved in statistics, signal processing and machine learning have the composite form

min⁡x φ(x):=f(x)+g(x),\min_x\ \varphi(x) := f(x) + g(x),xmin​ φ(x):=f(x)+g(x),

where fff is smooth and ggg is convex but possibly nonsmooth or extended-valued (a norm penalty, the indicator of a constraint set). The workhorse algorithm for such problems is the proximal gradient method, which takes a gradient step on fff followed by a proximal step on ggg. Its worst-case rate on convex problems is sublinear, yet in practice it often converges linearly. The classical explanation, going back to Luo and Tseng (1993) Ann. Oper. Res. 46, is an error bound condition: near the solution set, the distance to the minimizers is controlled by the length of the algorithm's own step. Under such a condition the method converges linearly.

The difficulty is that the error bound is stated in terms of the algorithm, not the problem. Drusvyatskiy and Lewis (arXiv:1602.06661, Math. Oper. Res. 43(3), 2018) showed that, for convex problems, it is equivalent to a purely geometric property of φ\varphiφ: quadratic growth away from the set of minimizers. This mission formalizes that equivalence (§3 of the paper) together with the three comparison results that build it.

Setting

Write Rn\mathbb R^nRn for Euclidean space with norm ∥⋅∥\|\cdot\|∥⋅∥, R‾=R∪{±∞}\overline{\mathbb R} = \mathbb R\cup\{\pm\infty\}R=R∪{±∞}, and dist⁡(x;Q)=inf⁡z∈Q∥z−x∥\operatorname{dist}(x;Q) = \inf_{z\in Q}\|z-x\|dist(x;Q)=infz∈Q​∥z−x∥. A function g:Rn→R‾g:\mathbb R^n\to\overline{\mathbb R}g:Rn→R is closed if it is lower semicontinuous. For real rrr, the sublevel set is [φ≤r]={x:φ(x)≤r}[\varphi\le r] = \{x:\varphi(x)\le r\}[φ≤r]={x:φ(x)≤r}.

The problem is (3.1): ggg is a closed convex function, and f:Rn→Rf:\mathbb R^n\to\mathbb Rf:Rn→R is convex, C1C^1C1-smooth, with β\betaβ-Lipschitz gradient, ∥∇f(x)−∇f(y)∥≤β∥x−y∥\|\nabla f(x)-\nabla f(y)\|\le\beta\|x-y\|∥∇f(x)−∇f(y)∥≤β∥x−y∥. Let SSS be the (nonempty) set of minimizers of φ=f+g\varphi = f+gφ=f+g and φ∗\varphi^*φ∗ its minimal value. For t>0t>0t>0 the proximal map is

prox⁡tg(z)=argmin⁡y{g(y)+12t∥y−z∥2},\operatorname{prox}_{tg}(z) = \operatorname*{argmin}_y\Big\{g(y)+\tfrac1{2t}\|y-z\|^2\Big\},proxtg​(z)=yargmin​{g(y)+2t1​∥y−z∥2},

the proximal gradient method iterates xk+1=prox⁡tg(xk−t∇f(xk))x_{k+1} = \operatorname{prox}_{tg}(x_k - t\nabla f(x_k))xk+1​=proxtg​(xk​−t∇f(xk​)), and the prox-gradient mapping is

Gt(x)=t−1(x−prox⁡tg(x−t∇f(x))),\mathcal G_t(x) = t^{-1}\big(x - \operatorname{prox}_{tg}(x - t\nabla f(x))\big),Gt​(x)=t−1(x−proxtg​(x−t∇f(x))),

so that xk+1=xk−t Gt(xk)x_{k+1} = x_k - t\,\mathcal G_t(x_k)xk+1​=xk​−tGt​(xk​) and Gt(x)=0\mathcal G_t(x) = 0Gt​(x)=0 exactly at minimizers.

For ν>0\nu>0ν>0, φ\varphiφ has quadratic growth with constant α>0\alpha>0α>0 if φ(x)≥φ∗+α2dist⁡2(x;S)\varphi(x)\ge\varphi^*+\frac\alpha2\operatorname{dist}^2(x;S)φ(x)≥φ∗+2α​dist2(x;S) on [φ≤φ∗+ν][\varphi\le\varphi^*+\nu][φ≤φ∗+ν] (3.12), and the error bound condition with parameters (γ,ν)(\gamma,\nu)(γ,ν) holds if dist⁡(x;S)≤γ∥Gt(x)∥\operatorname{dist}(x;S)\le\gamma\|\mathcal G_t(x)\|dist(x;S)≤γ∥Gt​(x)∥ on the same sublevel set (Definition 3.1, (3.13)).

Formalization targets

Goal: Corollary 3.6 (p. 9)

(3.12) with α ⟹ (3.13) with γ=(2α−1+t)(1+βt),(3.13) with γ ⟹ (3.12) for every α∈(0,γ−1),\text{(3.12) with }\alpha\ \Longrightarrow\ \text{(3.13) with }\gamma = (2\alpha^{-1}+t)(1+\beta t),\qquad \text{(3.13) with }\gamma\ \Longrightarrow\ \text{(3.12) for every }\alpha\in(0,\gamma^{-1}),(3.12) with α ⟹ (3.13) with γ=(2α−1+t)(1+βt),(3.13) with γ ⟹ (3.12) for every α∈(0,γ−1),

for every step size t>0t>0t>0 and every ν>0\nu>0ν>0.

Milestones

For a closed convex hhh with minimizers S≠∅S\neq\emptysetS=∅ and minimal value h∗h^*h∗:

  • Theorem 3.3 (pp. 6–7): quadratic growth on [h≤h∗+ν][h\le h^*+\nu][h≤h∗+ν] with constant α\alphaα implies dist⁡(x;S)≤Ldist⁡(0;∂h(x))\operatorname{dist}(x;S)\le L\operatorname{dist}(0;\partial h(x))dist(x;S)≤Ldist(0;∂h(x)) there with L=2α−1L = 2\alpha^{-1}L=2α−1; conversely the latter implies quadratic growth with any α∈(0,1/L]\alpha\in(0,1/L]α∈(0,1/L].
  • Theorem 3.4 (p. 7): the subdifferential bound with LLL implies dist⁡(x;S)≤L^ t−1∥x−prox⁡th(x)∥\operatorname{dist}(x;S)\le\widehat L\,t^{-1}\|x-\operatorname{prox}_{th}(x)\|dist(x;S)≤Lt−1∥x−proxth​(x)∥ with L^=L+t\widehat L = L+tL=L+t; conversely the latter implies the former with L=L^L = \widehat LL=L.
  • Theorem 3.5 (p. 8): for maximal monotone G,ΦG,\PhiG,Φ with Φ=F+G\Phi = F + GΦ=F+G and FFF single-valued, the forward-backward step satisfies ∥Gt(x)∥≤dist⁡(0;Φ(x))\|\mathcal G_t(x)\|\le\operatorname{dist}(0;\Phi(x))∥Gt​(x)∥≤dist(0;Φ(x)) (3.10), and if FFF is β\betaβ-Lipschitz,
(1−βt)∥Gt(x)∥ ≤ ∥t−1(x−prox⁡tΦ(x))∥ ≤ (1+βt)∥Gt(x)∥.(3.11)(1-\beta t)\|\mathcal G_t(x)\|\ \le\ \|t^{-1}(x-\operatorname{prox}_{t\Phi}(x))\|\ \le\ (1+\beta t)\|\mathcal G_t(x)\|.\qquad(3.11)(1−βt)∥Gt​(x)∥ ≤ ∥t−1(x−proxtΦ​(x))∥ ≤ (1+βt)∥Gt​(x)∥.(3.11)
  • Theorem 3.2, second claim (p. 5, at t=β−1t=\beta^{-1}t=β−1): under the error bound, the iterates converge R-linearly to any limit point x∗x^*x∗, ∥xr+k−x∗∥2≤(1−12βγ)kC(φ(xr)−φ∗)\|x_{r+k}-x^*\|^2\le(1-\frac1{2\beta\gamma})^kC(\varphi(x_r)-\varphi^*)∥xr+k​−x∗∥2≤(1−2βγ1​)kC(φ(xr​)−φ∗).

Significance

The result. Corollary 3.6 converts a condition on an algorithm into a condition on the objective. Quadratic growth can be checked by hand in many models (strongly convex losses, polyhedral problems, problems with a sharp minimum), and once it holds, Theorem 3.2 gives linear convergence of the proximal gradient method with an iteration count of order βαln⁡1ϵ\frac\beta\alpha\ln\frac1\epsilonαβ​lnϵ1​, matching the rate familiar from strongly convex problems. The rest of the paper uses this equivalence as its main tool: §4 proves quadratic growth for structured problems f(Ax)+g(x)f(Ax)+g(x)f(Ax)+g(x) under dual strict complementarity, and §§5–8 extend the comparison to prox-linear methods for nonconvex compositions. Theorems 3.3 and 3.4 are statements about a single closed convex function and are of independent use in the analysis of proximal point methods.

Formalizing it. All results here are proved on paper; none of them is machine-checked. The mission produces a Lean statement of the equivalence with the paper's explicit constants, and of the step-length comparison between the forward-backward and the proximal point methods for maximal monotone operators. Formal proofs require the existence, uniqueness and nonexpansiveness of resolvents and proximal maps, the subdifferential sum rule for a smooth plus a convex function, and a quadratic growth argument for convex functions; these are reusable well beyond this paper.

Difficulty

The forward direction is a chain of three inequalities, but each link compares objects that live in different worlds: the subdifferential of φ\varphiφ, the proximal map of φ\varphiφ, and the proximal map of ggg evaluated at a gradient-shifted point. The proximal gradient step is not the proximal point step on φ\varphiφ, and the obvious attempt to compare Gt(x)\mathcal G_t(x)Gt​(x) with ∂φ(x)\partial\varphi(x)∂φ(x) directly gives only one inequality (3.10); the reverse comparison (3.11) needs the resolvent of the sum ∇f+∂g\nabla f + \partial g∇f+∂g and the Lipschitz constant of ∇f\nabla f∇f. The converse half of Theorem 3.3 (error bound implies growth) is the deepest step: the paper omits its proof and cites Drusvyatskiy–Ioffe and Drusvyatskiy–Mordukhovich–Nghia. It has to pass from a pointwise bound on subgradients to a bound on function values over the whole sublevel set, which no single subgradient inequality provides.

Formalization scope

  • Rn\mathbb R^nRn is EuclideanSpace ℝ (Fin n); R‾\overline{\mathbb R}R-valued functions are EReal-valued; fff is real-valued and φ=f+g\varphi = f + gφ=f+g is computed in EReal. "Closed convex" is the published RockafellarMaxMono.Shared.ProperConvex (never −∞-\infty−∞, somewhere finite, convex) together with LowerSemicontinuous.
  • SSS is the set of minimizers, assumed nonempty as in the paper; φ∗\varphi^*φ∗ is a real number equal to φ\varphiφ on SSS; dist⁡\operatorname{dist}dist is Metric.infDist; ν>0\nu>0ν>0 is real.
  • Proximal maps and resolvents are predicates, never chosen functions: p=prox⁡tg(z)p=\operatorname{prox}_{tg}(z)p=proxtg​(z) is the published GoldenRatioVI.Shared.IsProxPoint (fun y => t * g y) z p (same argmin for t>0t>0t>0), and resolvents are maps satisfying the published ThreeOpSplitting.Convergence.IsResolvent. Conditions are stated for every such point; existence and uniqueness are facts a solver proves.
  • dist⁡(0;∂h(x))\operatorname{dist}(0;\partial h(x))dist(0;∂h(x)) follows the convention dist⁡(0;∅)=+∞\operatorname{dist}(0;\emptyset) = +\inftydist(0;∅)=+∞: an inequality "a≤Ldist⁡(0;∂h(x))a\le L\operatorname{dist}(0;\partial h(x))a≤Ldist(0;∂h(x))" is stated as "a≤L∥v∥a\le L\|v\|a≤L∥v∥ for every v∈∂h(x)v\in\partial h(x)v∈∂h(x)". Using Metric.infDist 0 (∂h x), which is 000 on the empty set, would turn (3.7) into the false claim that every point of the sublevel set where ∂h\partial h∂h is empty is a minimizer; this trivializing or falsifying encoding is ruled out.
  • The subdifferential is the published ProxAlg.FixedPoint.subdifferential, the gradient is Mathlib's gradient.
  • Theorem 3.2 is stated at t=β−1t = \beta^{-1}t=β−1 with β>0\beta>0β>0: the printed range t≤β−1t\le\beta^{-1}t≤β−1 relies on the descent inequality (3.2), which fails for smaller ttt. Its first claim (an iteration count) and Corollary 3.7 are not stated.

Contributions welcome: proofs of the milestones in any order, general lemmas on resolvents of maximal monotone operators and on proximal maps of EReal-valued convex functions, and a proof of the converse half of Theorem 3.3.

Selected references

  • D. Drusvyatskiy, A. S. Lewis, Error bounds, quadratic growth, and linear convergence of proximal methods, Math. Oper. Res. 43(3), 2018. arXiv:1602.06661v2 — https://arxiv.org/abs/1602.06661
  • Z.-Q. Luo, P. Tseng, Error bounds and convergence analysis of feasible descent methods: a general approach, Ann. Oper. Res. 46/47:157–178, 1993. https://doi.org/10.1007/BF02096261
  • D. Drusvyatskiy, A. D. Ioffe, Quadratic growth and critical point stability of semi-algebraic functions, Math. Program. 153(2):635–653, 2015 (reference [15] of the paper).
  • D. Drusvyatskiy, B. S. Mordukhovich, T. T. A. Nghia, Second-order growth, tilt stability, and metric regularity of the subdifferential, J. Convex Anal. 21(4):1165–1192, 2014 (reference [19] of the paper).
  • R. T. Rockafellar, R. J.-B. Wets, Variational Analysis, Springer, 1998. https://doi.org/10.1007/978-3-642-02431-3
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Dynamical SystemsOptimization·Captain: mikedeng1

Fast Convergence of Inertial Dynamics and Algorithms with Asymptotic Vanishing Viscosity 2: For Strongly Convex Φ and α > 3, Φ(x(t)) − min Φ, ‖x(t) − x*‖² and ‖ẋ(t)‖² Are O(t^(−2α/3))Research Paper

Motivation

Nesterov's accelerated gradient method minimizes a smooth convex function at the rate O(k−2)\mathcal O(k^{-2})O(k−2) in the number of iterations kkk, against O(k−1)\mathcal O(k^{-1})O(k−1) for plain gradient descent. Su, Boyd and Candès (arXiv:1503.01243) observed that, as the step size tends to zero, Nesterov's scheme becomes the second-order differential equation

x¨(t)+αtx˙(t)+∇Φ(x(t))=0(1)\ddot x(t)+\frac{\alpha}{t}\dot x(t)+\nabla\Phi(x(t))=0\tag{1}x¨(t)+tα​x˙(t)+∇Φ(x(t))=0(1)

with α=3\alpha=3α=3, a heavy-ball system whose friction coefficient α/t\alpha/tα/t vanishes as t→+∞t\to+\inftyt→+∞ (asymptotic vanishing damping). Studying (1) in continuous time gives Lyapunov arguments that are then discretized into new algorithms.

Attouch, Chbani, Peypouquet and Redont (Math. Program. 168 (2018), DOI 10.1007/s10107-016-0992-8) analyse (1) for general α\alphaα. This mission formalizes their result for strongly convex Φ\PhiΦ, where the rate of convergence of (1) depends on α\alphaα and improves without bound as α\alphaα grows.

Timeline.

  • 2014–2016: Su, Boyd and Candès prove Φ(x(t))−min⁡Φ=O(t−2)\Phi(x(t))-\min\Phi=\mathcal O(t^{-2})Φ(x(t))−minΦ=O(t−2) for convex Φ\PhiΦ and α≥3\alpha\ge3α≥3, and O(t−3)\mathcal O(t^{-3})O(t−3) for strongly convex Φ\PhiΦ when α>9/2\alpha>9/2α>9/2 ([44, Theorem 4.2] in the paper).
  • 2015 (this paper): every trajectory converges weakly to a minimizer when α>3\alpha>3α>3; for strongly convex Φ\PhiΦ and every α>3\alpha>3α>3, the values, the squared distance to the minimizer and the squared velocity are O(t−2α/3)\mathcal O(t^{-2\alpha/3})O(t−2α/3).

Setting

Let H\mathcal HH be a real Hilbert space with inner product ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle⟨⋅,⋅⟩ and norm ∥⋅∥\|\cdot\|∥⋅∥, and let Φ:H→R\Phi:\mathcal H\to\mathbb RΦ:H→R be continuously differentiable with gradient ∇Φ\nabla\Phi∇Φ. Fix α>0\alpha>0α>0 and t0>0t_0>0t0​>0. A solution of (1) is a twice differentiable trajectory x:[t0,+∞[→Hx:[t_0,+\infty[\to\mathcal Hx:[t0​,+∞[→H with velocity x˙\dot xx˙ satisfying (1) at every t≥t0t\ge t_0t≥t0​.

Φ\PhiΦ is strongly convex with constant μ>0\mu>0μ>0 if

Φ(y)≥Φ(x)+⟨∇Φ(x),y−x⟩+μ2∥x−y∥2for all x,y∈H.\Phi(y)\ge\Phi(x)+\langle\nabla\Phi(x),y-x\rangle+\frac\mu2\|x-y\|^2\qquad\text{for all }x,y\in\mathcal H.Φ(y)≥Φ(x)+⟨∇Φ(x),y−x⟩+2μ​∥x−y∥2for all x,y∈H.

Such a Φ\PhiΦ has exactly one minimizer x∗x^*x∗, and min⁡Φ=Φ(x∗)\min\Phi=\Phi(x^*)minΦ=Φ(x∗).

For λ≥0\lambda\ge0λ≥0, p≥0p\ge0p≥0 the anchored energy is

Eλp(t)=tp(t2(Φ(x(t))−min⁡Φ)+12∥λ(x(t)−x∗)+tx˙(t)∥2),\mathcal E^p_\lambda(t)=t^p\Big(t^2\big(\Phi(x(t))-\min\Phi\big)+\tfrac12\|\lambda(x(t)-x^*)+t\dot x(t)\|^2\Big),Eλp​(t)=tp(t2(Φ(x(t))−minΦ)+21​∥λ(x(t)−x∗)+tx˙(t)∥2),

a sum of nonnegative terms. The proof of the main theorem fixes

p=23(α−3),λ=23α,t1=max⁡{t0,pλ/μ}.p=\tfrac23(\alpha-3),\qquad\lambda=\tfrac23\alpha,\qquad t_1=\max\Big\{t_0,\sqrt{p\lambda/\mu}\Big\}.p=32​(α−3),λ=32​α,t1​=max{t0​,pλ/μ​}.

Formalization targets

Goal: Theorem 3.4 (p. 11)

For strongly convex Φ\PhiΦ and α>3\alpha>3α>3, every solution xxx of (1) converges strongly to the unique minimizer x∗x^*x∗, and

Φ(x(t))−min⁡Φ=O(t−23α),∥x(t)−x∗∥2=O(t−23α),∥x˙(t)∥2=O(t−23α)(25)\Phi(x(t))-\min\Phi=\mathcal O\big(t^{-\frac23\alpha}\big),\qquad\|x(t)-x^*\|^2=\mathcal O\big(t^{-\frac23\alpha}\big),\qquad\|\dot x(t)\|^2=\mathcal O\big(t^{-\frac23\alpha}\big)\tag{25}Φ(x(t))−minΦ=O(t−32​α),∥x(t)−x∗∥2=O(t−32​α),∥x˙(t)∥2=O(t−32​α)(25)

as t→+∞t\to+\inftyt→+∞. The goal states the asymptotic form; the explicit constants are milestones.

Milestones (explicit forms, valid for t≥t1t\ge t_1t≥t1​)

  1. The derivative identity (10) for Eλp\mathcal E^p_\lambdaEλp​ along solutions of (1), for any λ,p≥0\lambda,p\ge0λ,p≥0.
  2. Its strongly convex upper bound (first display of the proof of Theorem 3.4).
  3. (26): Eλp(t)≤Eλp(t1)+λp4tp∥x(t)−x∗∥2≤Eλp(t1)+λp2μtp(Φ(x(t))−min⁡Φ)\mathcal E^p_\lambda(t)\le\mathcal E^p_\lambda(t_1)+\frac{\lambda p}{4}t^p\|x(t)-x^*\|^2\le\mathcal E^p_\lambda(t_1)+\frac{\lambda p}{2\mu}t^p(\Phi(x(t))-\min\Phi)Eλp​(t)≤Eλp​(t1​)+4λp​tp∥x(t)−x∗∥2≤Eλp​(t1​)+2μλp​tp(Φ(x(t))−minΦ).
  4. (27): Φ(x(t))−min⁡Φ≤2Eλp(t1) t−23α\Phi(x(t))-\min\Phi\le2\mathcal E^p_\lambda(t_1)\,t^{-\frac23\alpha}Φ(x(t))−minΦ≤2Eλp​(t1​)t−32​α.
  5. (28): ∥x(t)−x∗∥2≤2μ(Φ(x(t))−min⁡Φ)≤4μEλp(t1) t−23α\|x(t)-x^*\|^2\le\frac2\mu(\Phi(x(t))-\min\Phi)\le\frac4\mu\mathcal E^p_\lambda(t_1)\,t^{-\frac23\alpha}∥x(t)−x∗∥2≤μ2​(Φ(x(t))−minΦ)≤μ4​Eλp​(t1​)t−32​α.
  6. Last display of the proof: ∥x˙(t)∥2≤4(1+α/(α−3))2Eλp(t1) t−23α\|\dot x(t)\|^2\le4\big(1+\sqrt{\alpha/(\alpha-3)}\big)^2\mathcal E^p_\lambda(t_1)\,t^{-\frac23\alpha}∥x˙(t)∥2≤4(1+α/(α−3)​)2Eλp​(t1​)t−32​α.

Significance

The theorem shows that the rate of (1) on strongly convex functions is not capped at O(t−2)\mathcal O(t^{-2})O(t−2) or O(t−3)\mathcal O(t^{-3})O(t−3): the exponent 2α/32\alpha/32α/3 grows linearly in α\alphaα, and it already exceeds 222 for every α>3\alpha>3α>3. It extends [44, Theorem 4.2], which needs α>9/2\alpha>9/2α>9/2 and gives O(t−3)\mathcal O(t^{-3})O(t−3). The same parametrized energy Eλp\mathcal E^p_\lambdaEλp​ is the template for the discrete analyses of Nesterov-type algorithms with parameter α\alphaα, so its derivative identity (10) is reusable beyond this mission.

The result is proved on paper. To the best of current knowledge none of it is formalized: Mathlib has no theory of inertial dynamics, and the platform's strongly convex rates concern discrete methods. A completed mission gives a machine-checked Lyapunov analysis of a non-autonomous second-order ODE in a Hilbert space, with the explicit constants of the paper.

Difficulty

The derivative identity (10) is a computation, but it must be carried out with one-sided derivatives at t0t_0t0​, real powers tpt^ptp, and the chain rule for Φ∘x\Phi\circ xΦ∘x in an infinite-dimensional space. The obvious argument, that Eλp\mathcal E^p_\lambdaEλp​ is nonincreasing, fails: even with the best choice of ppp and λ\lambdaλ the bound on its derivative keeps a term λp2tp⟨x−x∗,x˙⟩\frac{\lambda p}{2}t^p\langle x-x^*,\dot x\rangle2λp​tp⟨x−x∗,x˙⟩ of no fixed sign, and only for t≥t1t\ge t_1t≥t1​ is the quadratic term in ∥x−x∗∥2\|x-x^*\|^2∥x−x∗∥2 nonpositive. Passing from the differential inequality to (26) therefore needs integration on [t1,t][t_1,t][t1​,t] for functions known only through one-sided derivatives. The velocity bound then combines (26), (27) and (28) through square roots, and the goal additionally requires the existence of the minimizer in an infinite-dimensional space, which is a compactness argument (weak lower semicontinuity) and not an algebraic one.

Formalization scope

  • H\mathcal HH is any real Hilbert space (InnerProductSpace ℝ H, CompleteSpace H), not Rn\mathbb R^nRn. Φ\PhiΦ is ContDiff ℝ 1 and ∇Φ\nabla\Phi∇Φ is Mathlib's gradient.
  • A solution is a pair (x,v)(x,v)(x,v) with t0>0t_0>0t0​>0, where xxx has derivative v(t)v(t)v(t) and vvv has derivative −αtv(t)−∇Φ(x(t))-\frac\alpha t v(t)-\nabla\Phi(x(t))−tα​v(t)−∇Φ(x(t)) within [t0,+∞[[t_0,+\infty[[t0​,+∞[ at every t≥t0t\ge t_0t≥t0​; x˙\dot xx˙ is vvv.
  • Strong convexity is the gradient inequality printed on p. 10, with μ>0\mu>0μ>0; min⁡Φ\min\PhiminΦ is written Φ(x∗)\Phi(x^*)Φ(x∗) with x∗x^*x∗ a minimizer.
  • tpt^ptp is the real power, only evaluated at t≥t0>0t\ge t_0>0t≥t0​>0; ppp, λ\lambdaλ, t1t_1t1​ are named definitions shared by the milestones.
  • O\mathcal OO in (25) is Asymptotics.IsBigO along atTop; strong convergence is norm convergence. The existence and uniqueness of x∗x^*x∗ are conclusions of the goal, not hypotheses, so the goal cannot be satisfied vacuously by an empty argmin; the strong-convexity hypothesis is satisfiable (e.g. Φ=∥⋅∥2\Phi=\|\cdot\|^2Φ=∥⋅∥2 with μ=2\mu=2μ=2, and x≡0x\equiv0x≡0 solves (1)).
  • Theorem numbers and pages are those of the Optimization Online preprint 5179 (October 2015), not of the journal typesetting.

Useful infrastructure: the derivative of Φ∘x\Phi\circ xΦ∘x via gradient, integration of differential inequalities on [t0,+∞[[t_0,+\infty[[t0​,+∞[, and existence of minimizers of strongly convex continuous functions on Hilbert spaces. Proofs of any milestone, and of the goal from the milestones, are welcome.

Selected references

  • H. Attouch, Z. Chbani, J. Peypouquet, P. Redont, Fast convergence of inertial dynamics and algorithms with asymptotic vanishing damping, Optimization Online preprint 5179, 2015. https://optimization-online.org/wp-content/uploads/2015/10/5179.pdf
  • H. Attouch, Z. Chbani, J. Peypouquet, P. Redont, Fast convergence of inertial dynamics and algorithms with asymptotic vanishing viscosity, Math. Program. 168 (2018), 123–175. https://doi.org/10.1007/s10107-016-0992-8
  • W. Su, S. Boyd, E. J. Candès, A differential equation for modeling Nesterov's accelerated gradient method: theory and insights, J. Mach. Learn. Res. 17 (2016). https://arxiv.org/abs/1503.01243
  • Y. Nesterov, A method of solving a convex programming problem with convergence rate O(1/k²), Soviet Math. Dokl. 27 (1983), 372–376.
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Optimization·Captain: mikedeng1

Error Bounds, Quadratic Growth, and Linear Convergence of Proximal Methods II: Dual Strict Complementarity and Firm Convexity of the Components Give the Error Bound for f(Ax) + g(x)Research Paper

Motivation

Proximal gradient methods are used to minimize an objective with one smooth part and one convex part whose proximal map can be evaluated. A small proximal gradient step is a practical stopping signal, but it indicates proximity to an optimizer only when the objective has an appropriate error bound. Section 4 of Drusvyatskiy and Lewis gives conditions for that bound in the structured problem f(Ax)+g(x)f(Ax)+g(x)f(Ax)+g(x): the conditions concern the dual problem and the growth of the two component functions, rather than requiring strong convexity of their sum. This matters for problems with a nontrivial solution set and for penalties that are not strongly convex. The paper places this result after its §3 comparison of quadratic growth and proximal gradient error bounds (pp. 9–11).

Setting

Let En=RnE_n=\mathbb R^nEn​=Rn and Em=RmE_m=\mathbb R^mEm​=Rm, with their Euclidean inner products and norms. Let A:En→EmA:E_n\to E_mA:En​→Em​ be linear, f:Em→Rf:E_m\to\mathbb Rf:Em​→R be continuously differentiable and convex, and g:En→(−∞,+∞]g:E_n\to(-\infty,+\infty]g:En​→(−∞,+∞] be proper, lower semicontinuous, and convex. The primal objective and its minimizer set are

φ(x)=f(Ax)+g(x),S=argmin⁡x∈Enφ(x).\varphi(x)=f(Ax)+g(x),\qquad S=\operatorname*{argmin}_{x\in E_n}\varphi(x).φ(x)=f(Ax)+g(x),S=x∈En​argmin​φ(x).

The mission assumes SSS is nonempty and bounded. Its minimum φ∗\varphi^*φ∗ is finite. For an extended-real function hhh, its Fenchel conjugate is h∗(v)=sup⁡z{⟨v,z⟩−h(z)}h^*(v)=\sup_z\{\langle v,z\rangle-h(z)\}h∗(v)=supz​{⟨v,z⟩−h(z)}. The dual objective is Ψ(y)=f∗(y)+g∗(−A⊤y)\Psi(y)=f^*(y)+g^*(-A^\top y)Ψ(y)=f∗(y)+g∗(−A⊤y), and yˉ\bar yyˉ​ denotes a dual minimizer. The effective domain is dom⁡h={z:h(z)<+∞}\operatorname{dom}h=\{z:h(z)<+\infty\}domh={z:h(z)<+∞}; ri⁡\operatorname{ri}ri denotes relative interior. The paper assumes dual nondegeneracy, 0∈A⊤(ri⁡dom⁡f∗)+ri⁡dom⁡g∗0\in A^\top(\operatorname{ri}\operatorname{dom}f^*)+\operatorname{ri}\operatorname{dom}g^*0∈A⊤(ridomf∗)+ridomg∗, and dual strict complementarity, 0∈ri⁡∂Ψ(yˉ)0\in\operatorname{ri}\partial\Psi(\bar y)0∈ri∂Ψ(yˉ​) (p. 10).

A closed convex function hhh is firmly convex relative to vvv when its tilt hv(x)=h(x)−⟨v,x⟩h_v(x)=h(x)-\langle v,x\ranglehv​(x)=h(x)−⟨v,x⟩ grows at least quadratically away from its minimizers on each compact set. The positive coefficient may depend on the compact set. Theorem 4.2 assumes this property for fff at yˉ\bar yyˉ​ and for ggg at −A⊤yˉ-A^\top\bar y−A⊤yˉ​ (Definition 4.1, p. 11).

For t>0t>0t>0, a proximal gradient step is p=prox⁡tg(x−t∇(f∘A)(x))p=\operatorname{prox}_{tg}(x-t\nabla(f\circ A)(x))p=proxtg​(x−t∇(f∘A)(x)), and its residual is Gt(x)=t−1(x−p)G_t(x)=t^{-1}(x-p)Gt​(x)=t−1(x−p). The error bound asks whether the distance from xxx to SSS is controlled by ∥Gt(x)∥\|G_t(x)\|∥Gt​(x)∥ whenever xxx lies below a prescribed objective threshold (Definition 3.1, p. 5).

Formalization targets

Component and composite growth

The milestone path records the Kuhn–Tucker description of SSS, the relative-interior identity (4.3), the compact-set distance estimate (4.4), the two component inequalities (4.5), and the resulting quadratic growth of φ\varphiφ on every sublevel set. In particular, for each ν>0\nu>0ν>0 there is μ>0\mu>0μ>0 such that

φ(x)≥φ∗+μdist⁡2(x,S)if φ(x)≤φ∗+ν.\varphi(x)\ge\varphi^*+\mu\operatorname{dist}^2(x,S) \quad\text{if }\varphi(x)\le\varphi^*+\nu.φ(x)≥φ∗+μdist2(x,S)if φ(x)≤φ∗+ν.

These are the claims stated in §4 and in the proof of Theorem 4.2, pp. 10–11. The milestone for (4.5) retains the paper's printed c,α≥0c,\alpha\ge0c,α≥0 in its quotation, while the Lean statement uses positive constants, as Definition 4.1 requires for nontrivial quadratic growth.

Goal: a proximal gradient error bound

The goal is Theorem 4.2: under the conditions above, for every t>0t>0t>0 there exist γ,ν>0\gamma,\nu>0γ,ν>0 such that

dist⁡(x,S)≤γ∥Gt(x)∥whenever φ(x)≤φ∗+ν.\operatorname{dist}(x,S)\le\gamma\|G_t(x)\| \quad\text{whenever }\varphi(x)\le\varphi^*+\nu.dist(x,S)≤γ∥Gt​(x)∥whenever φ(x)≤φ∗+ν.

The formal statement makes explicit that ∇f\nabla f∇f has a Lipschitz constant. This is part of the §3 setting used by the paper's Corollary 3.6 to reach the displayed error bound. A companion statement, Theorem 4.5, pp. 12–13, says that the Moreau envelope of a firmly convex function retains firm convexity relative to the same vector.

Significance

The conclusion converts dual geometric information and component growth into an error bound expressed through a proximal gradient step. The residual is available when running the method, whereas the distance to SSS is generally not. Combined with the paper's §3 results, the error bound yields local convergence guarantees for the proximal gradient method in structured convex problems (Corollary 3.6 and Theorem 4.2). The statement covers settings in which component functions have local quadratic growth after a tilt while the composite objective need not be strongly convex.

The research result is proved in the paper. The work of this mission is to formalize its exact assumptions and claims, including the convex dual and the relative-interior statements, then supply machine-checked proofs. The resulting Euclidean conjugate, firm-convexity, and structured-objective definitions can also support other convex optimization formalizations. The statements in this proposal are proof obligations; compiling the statements alone does not establish the theorems.

Difficulty

Component growth concerns distance to separate subdifferential inverse images. The desired error bound concerns distance to their intersection, which is the primal solution set. Two small component distances do not automatically control distance to an intersection: the sets can meet at a poor angle. The dual interior hypotheses supply the regularity needed in (4.4). The argument also changes the quantity being controlled from objective growth to a proximal gradient residual. Those two changes are the substantive steps a proof must justify; treating either as an unrestricted distance identity would change the theorem.

Formalization scope

The Lean spaces are EuclideanSpace ℝ (Fin n) and EuclideanSpace ℝ (Fin m); dimensions zero are permitted. The linear map is continuous, and A⊤A^\topA⊤ is its adjoint. Extended-real values use EReal; properness excludes −∞-\infty−∞ values, and lower semicontinuity encodes closedness. Conjugates take suprema in EReal, and the dual objective follows (4.2). Relative interior is intrinsicInterior ℝ. The published convex subdifferential, proper-convex predicate, and proximal-point predicate are imported as reference items because their meanings match the paper's objects. The paper's Euclidean conjugate is defined locally because the available published conjugate has a strong-dual codomain.

The minimum value is real and is pinned to the nonempty primal minimizer set. The dual point is pinned as a minimizer of Ψ\PsiΨ. Proximal steps are expressed as argmin predicates, so no default result is chosen for a failed minimization. The firm-convexity predicate requires a nonempty minimizer set of the tilted function: otherwise Lean's real distance to the empty set would be zero while the source uses an infinite distance. The growth constant α\alphaα of Definition 4.1 and the constants c,αc,\alphac,α of (4.5) are strictly positive: the page leaves the sign implicit or prints ≥0\ge 0≥0, but with a zero constant every convex function would be firmly convex, contradicting the page's own example x4x^4x4, and the growth statements would be empty. The error bound is restricted to the stated sublevel set, and all of its constants are positive. The goal includes a nonnegative Lipschitz constant for ∇f\nabla f∇f, disclosed because the source's §3 bridge to the error bound assumes one; the component-growth milestones do not assume it.

Contributions should establish the Euclidean convex-duality identities, the compact-set regularity estimate, the component and composite growth claims, and the proximal gradient conclusion. The Moreau-envelope preservation theorem is a separate companion target. None of the dual interior conditions or the firm-convexity assumptions may be replaced by a vacuous condition: the goal concerns their effect on the actual solution set of f(Ax)+g(x)f(Ax)+g(x)f(Ax)+g(x).

Selected references

  • D. Drusvyatskiy and A. S. Lewis, Error bounds, quadratic growth, and linear convergence of proximal methods, Mathematics of Operations Research 43(3), 2018. arXiv:1602.06661v2.
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Optimization·Captain: mikedeng1

Faster Convergence Rates of Relaxed Peaceman-Rachford and ADMM Under Regularity Assumptions I: Relaxed PRS Regularity Terms Have o(1/(k+1)) Best-Iterate and o(1/√(k+1)) Nonergodic RatesResearch Paper

Motivation

Peaceman–Rachford splitting and its relaxed forms solve the problem of minimizing a sum f+gf+gf+g by evaluating the two proximal maps separately. This is useful when minimizing either function by itself is simple while minimizing their sum directly is not. Douglas–Rachford splitting is the half-relaxed case. Davis and Yin study which properties of fff and ggg turn the basic convergence of this iteration into quantitative rates. Their Theorem 2.1 supplies the regularity estimates used throughout their later objective and fixed-point analyses (Davis and Yin, arXiv:1407.5210v3, §§1–2).

The theorem measures progress using a term that can respond to strong convexity, a Lipschitz gradient, or both. Its conclusions distinguish three observations of the same run: the best iterate found so far, a weighted average of the auxiliary points, and the current iterate. This distinction matters because a rate for a best iterate need not hold for every iterate; the authors explicitly leave open whether their best-iterate conclusion can be improved in that way (Davis and Yin, p. 9).

Setting

Let HHH be a real Hilbert space. The functions f,g:H→(−∞,+∞]f,g:H\to(-\infty,+\infty]f,g:H→(−∞,+∞] are closed, proper, and convex. For a positive step size γ\gammaγ, the proximal map of fff sends zzz to the unique minimizer of f(x)+∥x−z∥2/(2γ)f(x)+\|x-z\|^2/(2\gamma)f(x)+∥x−z∥2/(2γ). Define the reflection Rf=2prox⁡γf−IR_f=2\operatorname{prox}_{\gamma f}-IRf​=2proxγf​−I and likewise RgR_gRg​. The Peaceman–Rachford map is TPRS=Rf∘RgT_{\mathrm{PRS}}=R_f\circ R_gTPRS​=Rf​∘Rg​. Given relaxation parameters λk∈(0,1]\lambda_k\in(0,1]λk​∈(0,1], Algorithm 1 generates

zk+1=(1−λk)zk+λkTPRSzk.z^{k+1}=(1-\lambda_k)z^k+\lambda_kT_{\mathrm{PRS}}z^k.zk+1=(1−λk​)zk+λk​TPRS​zk.

At zkz^kzk, set xgk=prox⁡γg(zk)x_g^k=\operatorname{prox}_{\gamma g}(z^k)xgk​=proxγg​(zk) and xfk=prox⁡γf(Rgzk)x_f^k=\operatorname{prox}_{\gamma f}(R_gz^k)xfk​=proxγf​(Rg​zk). These points may differ, so the theorem tracks them separately. Their selected proximal subgradients are ∇~g(xgk)=γ−1(zk−xgk)\widetilde\nabla g(x_g^k)=\gamma^{-1}(z^k-x_g^k)∇g(xgk​)=γ−1(zk−xgk​) and ∇~f(xfk)=γ−1(Rgzk−xfk)\widetilde\nabla f(x_f^k)=\gamma^{-1}(R_gz^k-x_f^k)∇f(xfk​)=γ−1(Rg​zk−xfk​). The tilde means a particular member of a subdifferential when the function is not differentiable (Lemma 1.1, p. 7).

Suppose z∗z^*z∗ is a fixed point of TPRST_{\mathrm{PRS}}TPRS​ and put x∗=prox⁡γg(z∗)x^*=\operatorname{prox}_{\gamma g}(z^*)x∗=proxγg​(z∗). Each function h∈{f,g}h\in\{f,g\}h∈{f,g} has a nonnegative strong-convexity parameter μh\mu_hμh​ and a nonnegative smoothness parameter βh\beta_hβh​. If βh>0\beta_h>0βh​>0, the function is differentiable and its gradient is βh−1\beta_h^{-1}βh−1​-Lipschitz; a zero parameter imposes no such property. For the selected subgradients at xxx and yyy, define the regularity term

Sh(x,y)=max⁡{μh2∥x−y∥2,βh2∥∇~h(x)−∇~h(y)∥2}.S_h(x,y)=\max\left\{\frac{\mu_h}{2}\|x-y\|^2,\frac{\beta_h}{2}\|\widetilde\nabla h(x)-\widetilde\nabla h(y)\|^2\right\}.Sh​(x,y)=max{2μh​​∥x−y∥2,2βh​​∥∇h(x)−∇h(y)∥2}.

The partial relaxation weight is Λk=∑i=0kλi\Lambda_k=\sum_{i=0}^k\lambda_iΛk​=∑i=0k​λi​. All of these conventions are from the paper's notation, Algorithm 1, and equations (1.13)–(1.14) (Davis and Yin, pp. 3–8).

Formalization targets

One-step and summed bounds

The goal first asserts the exact one-step inequality (2.1):

8γλk(Sf(xfk,x∗)+Sg(xgk,x∗))≤∥zk−z∗∥2−∥zk+1−z∗∥2+(1−1λk)∥zk+1−zk∥2.8\gamma\lambda_k\bigl(S_f(x_f^k,x^*)+S_g(x_g^k,x^*)\bigr)\le \|z^k-z^*\|^2-\|z^{k+1}-z^*\|^2+ \left(1-\frac1{\lambda_k}\right)\|z^{k+1}-z^k\|^2.8γλk​(Sf​(xfk​,x∗)+Sg​(xgk​,x∗))≤∥zk−z∗∥2−∥zk+1−z∗∥2+(1−λk​1​)∥zk+1−zk∥2.

It also asserts that ∑i≥0λi(Sf(xfi,x∗)+Sg(xgi,x∗))\sum_{i\ge0}\lambda_i(S_f(x_f^i,x^*)+S_g(x_g^i,x^*))∑i≥0​λi​(Sf​(xfi​,x∗)+Sg​(xgi​,x∗)) converges and that eight times γ\gammaγ times this sum is at most ∥z0−z∗∥2\|z^0-z^*\|^2∥z0−z∗∥2. These are Theorem 2.1's common quantitative bounds (p. 8).

Best-iterate, ergodic, and nonergodic rates

If the λj\lambda_jλj​ are bounded below by a positive constant, the minimum through kkk of each regularity term is o(1/(k+1))o(1/(k+1))o(1/(k+1)). The weighted averages of xfix_f^ixfi​ and xgix_g^ixgi​, together with the matching weighted averages of their selected subgradients, have regularity terms whose sum is at most ∥z0−z∗∥2/(8γΛk)\|z^0-z^*\|^2/(8\gamma\Lambda_k)∥z0−z∗∥2/(8γΛk​). Finally, if the products λj(1−λj)\lambda_j(1-\lambda_j)λj​(1−λj​) have a positive lower bound, the sum of the two current regularity terms is o(1/k+1)o(1/\sqrt{k+1})o(1/k+1​) (Theorem 2.1, p. 9).

Significance

Strong convexity makes the regularity term control squared distance to x∗x^*x∗; a positive smoothness parameter makes it control the difference between selected gradients. Theorem 2.1 therefore connects properties of the objectives to rates for quantities produced by Algorithm 1. The one-step bound is also the stated input to later linear-convergence arguments in the same paper (§4, pp. 13–16). Without this result, those applications lack their common quantitative estimate.

The paper proves Theorem 2.1. This mission asks for a machine-checked proof of its precise statement and supporting claims, not for a new asymptotic rate. The proximal-map and subdifferential definitions already exist as published formal objects; the reusable remaining work includes their quantitative inequalities and the summable-sequence rate facts. The draft goal and milestones are theorem statements with proof holes and do not yet constitute verified proofs.

Difficulty

The obvious inference from a finite sum of nonnegative regularity terms gives a bound on cumulative error, but it does not directly give little-ooo rates for the current term. The theorem also separates a best-iterate conclusion from a last-iterate conclusion: the regularity terms need not be monotone, and the stronger condition on λj(1−λj)\lambda_j(1-\lambda_j)λj​(1−λj​) is required for the latter. The ergodic conclusion concerns weighted averages of both points and subgradients, so bounding only the average of pointwise regularity terms does not by itself state the result (Theorem 2.1 and its discussion, pp. 8–9).

Formalization scope

Lean uses EReal for the objectives, a complete real inner-product space for HHH, and published predicates for closed proper convex functions, proximal maps, and subgradients. A proximal map is supplied as a function satisfying the minimization property; uniqueness under the stated assumptions makes it the paper's map. Selected subgradients are fixed difference quotients from Lemma 1.1. The parameters μf,βf,μg,βg\mu_f,\beta_f,\mu_g,\beta_gμf​,βf​,μg​,βg​ are nonnegative, and positive β\betaβ requires a real-valued differentiable function with β−1\beta^{-1}β−1-Lipschitz gradient. A fixed point z∗z^*z∗ states the solution-existence assumption in the form used by Theorem 2.1. No hypothesis asserts any conclusion of the theorem.

The finite minimum uses the nonempty index range 0,…,k0,\ldots,k0,…,k; little-ooo uses Mathlib's asymptotic relation at infinity. The denominators λk\lambda_kλk​, Λk\Lambda_kΛk​, and k+1\sqrt{k+1}k+1​ are positive under the stated bounds. In supporting objective inequalities, conversion from EReal to real numbers occurs only at proximal outputs and points with subgradients, where function values are finite. The printed unweighted, repeated-kkk subgradient sum in the ergodic clause is corrected to the λi\lambda_iλi​-weighted average consistent with the page's definition of xˉfk\bar x_f^kxˉfk​ and with the result it states. Contributions proving the exact goal, any milestone, or reusable proximal and sequence lemmas are in scope.

Selected references

  • Damek Davis and Wotao Yin, Faster convergence rates of relaxed Peaceman–Rachford and ADMM under regularity assumptions, Mathematics of Operations Research 42(3), 2017; preprint arXiv:1407.5210v3, 2015. arXiv · DOI
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Optimal TransportOptimization·Captain: mikedeng1

Wasserstein Distributionally Robust Kalman Filtering 2: The Bisection Algorithm Returns a Feasible, ε-Suboptimal Solution of the Frank–Wolfe Direction-Finding SubproblemResearch Paper

Motivation

A Kalman filter estimates the hidden state xxx of a linear system from observations yyy, assuming the joint law of z=(x,y)z = (x, y)z=(x,y) is a known Gaussian. When that law is only approximately known, Shafieezadeh-Abadeh, Nguyen, Kuhn and Mohajerin Esfahani (arXiv:1809.08830v3, NeurIPS 2018) replace it by the worst Gaussian within a 2-Wasserstein ball of radius ρ\rhoρ around a nominal Gaussian with covariance Σ\SigmaΣ. Their Theorem 2.5 shows that the resulting minimax estimation problem is equivalent to a finite nonlinear semidefinite program, program (5), whose objective is f(S)=Tr[Sxx−SxySyy−1Syx]f(S) = \mathrm{Tr}[S_{xx} - S_{xy}S_{yy}^{-1}S_{yx}]f(S)=Tr[Sxx​−Sxy​Syy−1​Syx​].

Each step of the robust filter solves program (5), so the filter is only practical if (5) can be solved quickly. The paper solves it with a Frank–Wolfe method (Algorithm 2), which avoids projections by replacing the objective with its linearization at the current iterate and maximizing that linear function over the original feasible set. That inner problem, the direction-finding subproblem, is again a nonlinear SDP. The paper's Algorithm 1 solves it by a one-dimensional bisection, and Theorem 3.2 states that this bisection returns a feasible solution whose objective value is within a prescribed tolerance ε\varepsilonε of the optimum. This mission formalizes that guarantee.

Setting

Fix dimensions n≥1n \ge 1n≥1 (state) and mmm (observation), d=n+md = n + md=n+m, and index coordinates so that the first nnn belong to xxx. Let S+d\mathbb{S}^d_+S+d​ and S++d\mathbb{S}^d_{++}S++d​ denote the positive semidefinite and positive definite d×dd\times dd×d matrices, and ⟨A,B⟩=Tr[A⊤B]\langle A, B\rangle = \mathrm{Tr}[A^\top B]⟨A,B⟩=Tr[A⊤B] the trace inner product. The data are a nominal covariance Σ∈S++d\Sigma \in \mathbb{S}^d_{++}Σ∈S++d​ with smallest eigenvalue σ‾=λmin⁡(Σ)\underline\sigma = \lambda_{\min}(\Sigma)σ​=λmin​(Σ), a radius ρ>0\rho > 0ρ>0, a tolerance ε>0\varepsilon > 0ε>0, and the current Frank–Wolfe iterate S∈S+dS \in \mathbb{S}^d_+S∈S+d​, written in blocks Sxx,Sxy,Syx,SyyS_{xx}, S_{xy}, S_{yx}, S_{yy}Sxx​,Sxy​,Syx​,Syy​.

The gradient matrix is

D=∇f(S)=[In,−G]⊤[In,−G],G=SxySyy−1,D = \nabla f(S) = [I_n, -G]^\top [I_n, -G], \qquad G = S_{xy}S_{yy}^{-1},D=∇f(S)=[In​,−G]⊤[In​,−G],G=Sxy​Syy−1​,

which is positive semidefinite and nonzero. The direction-finding subproblem (7b) is

max⁡L⪰σ‾Id ⟨L,D⟩s.t.Tr[L+Σ−2(Σ1/2LΣ1/2)1/2]≤ρ2;\max_{L \succeq \underline\sigma I_d}\ \langle L, D\rangle \quad \text{s.t.}\quad \mathrm{Tr}\Big[L + \Sigma - 2\big(\Sigma^{1/2} L \Sigma^{1/2}\big)^{1/2}\Big] \le \rho^2 ;L⪰σ​Id​max​ ⟨L,D⟩s.t.Tr[L+Σ−2(Σ1/2LΣ1/2)1/2]≤ρ2;

its constraint says that the Gaussian with covariance LLL lies within Wasserstein distance ρ\rhoρ of the nominal Gaussian, and F\mathcal FF denotes its feasible set. For γ\gammaγ with γId≻D\gamma I_d \succ DγId​≻D the paper defines

h(γ)=ρ2−⟨Σ,(Id−γ(γId−D)−1)2⟩,L(γ)=γ2(γId−D)−1Σ(γId−D)−1,h(\gamma) = \rho^2 - \big\langle \Sigma, (I_d - \gamma(\gamma I_d - D)^{-1})^2\big\rangle, \qquad L(\gamma) = \gamma^2 (\gamma I_d - D)^{-1}\Sigma(\gamma I_d - D)^{-1},h(γ)=ρ2−⟨Σ,(Id​−γ(γId​−D)−1)2⟩,L(γ)=γ2(γId​−D)−1Σ(γId​−D)−1, Δ(γ)=γ(ρ2−Tr[Σ])−⟨L(γ),D⟩+γ2⟨(γId−D)−1,Σ⟩.\Delta(\gamma) = \gamma(\rho^2 - \mathrm{Tr}[\Sigma]) - \langle L(\gamma), D\rangle + \gamma^2\langle(\gamma I_d - D)^{-1}, \Sigma\rangle .Δ(γ)=γ(ρ2−Tr[Σ])−⟨L(γ),D⟩+γ2⟨(γId​−D)−1,Σ⟩.

Algorithm 1 takes the largest eigenvalue λ1\lambda_1λ1​ of DDD and a unit eigenvector v1v_1v1​, and starts from the bracket [LB,UB]=[γmin⁡,γmax⁡][LB, UB] = [\gamma_{\min}, \gamma_{\max}][LB,UB]=[γmin​,γmax​] with

γmin⁡=λ1(1+v1⊤Σv1/ρ),γmax⁡=λ1(1+Tr[Σ]/ρ).\gamma_{\min} = \lambda_1\big(1 + \sqrt{v_1^\top\Sigma v_1}/\rho\big), \qquad \gamma_{\max} = \lambda_1\big(1 + \sqrt{\mathrm{Tr}[\Sigma]}/\rho\big).γmin​=λ1​(1+v1⊤​Σv1​​/ρ),γmax​=λ1​(1+Tr[Σ]​/ρ).

Each pass sets γ=(UB+LB)/2\gamma = (UB + LB)/2γ=(UB+LB)/2 and L=L(γ)L = L(\gamma)L=L(γ), replaces LBLBLB by γ\gammaγ if h(γ)<0h(\gamma) < 0h(γ)<0 and UBUBUB by γ\gammaγ otherwise, and the loop exits with output LLL as soon as h(γ)>0h(\gamma) > 0h(γ)>0 and Δ(γ)<ε\Delta(\gamma) < \varepsilonΔ(γ)<ε.

Formalization targets

Goal: Theorem 3.2

For all inputs as above:

  1. Soundness. At every pass kkk whose exit test holds, with trial point γk\gamma_kγk​,
L(γk)∈Fand⟨L′,D⟩≤⟨L(γk),D⟩+ε  for all L′∈F.L(\gamma_k) \in \mathcal F \quad\text{and}\quad \langle L', D\rangle \le \langle L(\gamma_k), D\rangle + \varepsilon \ \text{ for all } L' \in \mathcal F .L(γk​)∈Fand⟨L′,D⟩≤⟨L(γk​),D⟩+ε  for all L′∈F.
  1. Termination. If hhh has no zero at a dyadic point γmin⁡+j(γmax⁡−γmin⁡)/2k\gamma_{\min} + j(\gamma_{\max} - \gamma_{\min})/2^kγmin​+j(γmax​−γmin​)/2k, 0<j≤2k0 < j \le 2^k0<j≤2k, then some pass satisfies the exit test.

The termination hypothesis is a correction: the printed theorem asserts that the algorithm outputs a solution, but if a trial point (or γmax⁡\gamma_{\max}γmax​) coincides exactly with the root of hhh, the upper end of the bracket becomes that root, all later trial points have h<0h < 0h<0, and the loop never exits. Soundness holds unconditionally. The normalization ∥v1∥=1\|v_1\| = 1∥v1​∥=1 is also added; the page says only "an eigenvector", and γmin⁡\gamma_{\min}γmin​ is not a lower bound for a rescaled one.

Milestones (App. A.3, p. 13, in the order the proof uses them)

  • L(γ)∈FL(\gamma) \in \mathcal FL(γ)∈F whenever γId≻D\gamma I_d \succ DγId​≻D and h(γ)>0h(\gamma) > 0h(γ)>0.
  • Weak duality: ⟨L′,D⟩≤γ(ρ2−Tr[Σ])+γ2⟨(γId−D)−1,Σ⟩\langle L', D\rangle \le \gamma(\rho^2 - \mathrm{Tr}[\Sigma]) + \gamma^2\langle (\gamma I_d - D)^{-1}, \Sigma\rangle⟨L′,D⟩≤γ(ρ2−Tr[Σ])+γ2⟨(γId​−D)−1,Σ⟩ for all L′∈FL' \in \mathcal FL′∈F and γ≥0\gamma \ge 0γ≥0 with γId≻D\gamma I_d \succ DγId​≻D.
  • The suboptimality display: if h(γ⋆)=0h(\gamma^\star) = 0h(γ⋆)=0 then ⟨L(γ⋆)−L(γ),D⟩≤γ(ρ2−Tr[Σ])+γ2⟨(γId−D)−1,Σ⟩−⟨L(γ),D⟩\langle L(\gamma^\star) - L(\gamma), D\rangle \le \gamma(\rho^2 - \mathrm{Tr}[\Sigma]) + \gamma^2\langle(\gamma I_d - D)^{-1}, \Sigma\rangle - \langle L(\gamma), D\rangle⟨L(γ⋆)−L(γ),D⟩≤γ(ρ2−Tr[Σ])+γ2⟨(γId​−D)−1,Σ⟩−⟨L(γ),D⟩.
  • Lemma A.3: every root γ⋆\gamma^\starγ⋆ of hhh with γ⋆Id≻D\gamma^\star I_d \succ Dγ⋆Id​≻D lies in [γmin⁡,γmax⁡][\gamma_{\min}, \gamma_{\max}][γmin​,γmax​].

Significance

Theorem 3.2 is what makes Algorithm 1 a valid linear-maximization oracle for the Frank–Wolfe method on program (5): the convergence analysis of Frank–Wolfe with inexact oracles requires exactly a feasible point whose linearized objective is within a known tolerance of the optimum. It also shows that the inner problem, a semidefinite program with a matrix square root in the constraint, reduces to a scalar root-finding problem once DDD is diagonalized, which is why the robust filter runs at a cost comparable to an eigendecomposition per step.

The result is proved in the paper; no machine-checked version exists. The formal version adds what the paper leaves implicit: the termination edge case, the normalization of v1v_1v1​, and the requirement D≠0D \ne 0D=0 (here n≥1n \ge 1n≥1). The milestone statements on Lagrangian weak duality for the Wasserstein–Gaussian trust region and on the location of the multiplier are reusable for other covariance-robust programs of the same shape, such as Wasserstein shrinkage estimation.

Difficulty

The algorithm is elementary; the analysis is not. Feasibility of L(γ)L(\gamma)L(γ) requires computing the matrix square root (Σ1/2L(γ)Σ1/2)1/2(\Sigma^{1/2}L(\gamma)\Sigma^{1/2})^{1/2}(Σ1/2L(γ)Σ1/2)1/2 in closed form and comparing eigenvalues of non-commuting products to obtain L(γ)⪰σ‾IdL(\gamma) \succeq \underline\sigma I_dL(γ)⪰σ​Id​. The dual bound is a semidefinite Lagrangian duality statement over a constraint involving a matrix square root, whose inner supremum (Lemma A.1, cited from earlier work) must be evaluated in closed form. Termination needs monotonicity and continuity of hhh on (λ1,∞)(\lambda_1, \infty)(λ1​,∞) and a careful account of which side of the root each bisection update lands on; the obvious invariant "the root stays strictly inside the bracket" fails precisely in the excluded dyadic case.

Formalization scope

Matrices are indexed by Fin n ⊕ Fin m with blocks toBlocks₁₁ (xxxxxx), toBlocks₁₂ (xyxyxy), toBlocks₂₂ (yyyyyy). The feasible set F\mathcal FF is the published definition WassersteinDRO.Shrinkage.sdpFeasibleSet ρ Σ σ, which uses the published positive semidefinite square root psdSqrt. Mathlib's matrix inverse returns 000 on singular matrices; every statement involving hhh, LLL or Δ\DeltaΔ assumes γId≻D\gamma I_d \succ DγId​≻D or works at trial points that lie above λ1\lambda_1λ1​, and Syy−1S_{yy}^{-1}Syy−1​ is allowed to be this junk value because the theorem admits any S∈S+dS \in \mathbb{S}^d_+S∈S+d​ (then D=diag(In,0)D = \mathrm{diag}(I_n, 0)D=diag(In​,0)). The constants σ‾\underline\sigmaσ​ and λ1\lambda_1λ1​ are passed as reals together with hypotheses that pin them to the smallest eigenvalue of Σ\SigmaΣ and the largest eigenvalue of DDD. The algorithm is modelled as its sequence of passes, not as a function returning an output, so a non-terminating run cannot silently produce a value.

A formalization that defines the output with a fuel bound or a default value, that states only optimality of L(γ⋆)L(\gamma^\star)L(γ⋆) at the exact root, or that assumes termination as a hypothesis would not be Theorem 3.2; ε\varepsilonε-suboptimality is stated against every feasible point, not against a supremum that could be a junk value.

A complete development needs the spectral theorem for symmetric matrices, uniqueness of the positive semidefinite square root, and semidefinite Lagrangian duality; Mathlib supplies the first two. Proofs of the milestones are welcome contributions.

Selected references

  • S. Shafieezadeh-Abadeh, V. A. Nguyen, D. Kuhn, P. Mohajerin Esfahani, Wasserstein Distributionally Robust Kalman Filtering, NeurIPS 2018; arXiv:1809.08830v3. https://arxiv.org/abs/1809.08830
  • V. A. Nguyen, D. Kuhn, P. Mohajerin Esfahani, Distributionally Robust Inverse Covariance Estimation: The Wasserstein Shrinkage Estimator, Optimization Online, 2018; arXiv:1805.07194 (reference [18] of the paper; source of Lemma A.1). https://arxiv.org/abs/1805.07194
  • M. Jaggi, Revisiting Frank–Wolfe: Projection-Free Sparse Convex Optimization, ICML 2013 (reference [13]; Frank–Wolfe with approximate oracles). https://proceedings.mlr.press/v28/jaggi13.html
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Dynamical SystemsOptimization·Captain: mikedeng1

Fast Convergence of Inertial Dynamics and Algorithms with Asymptotic Vanishing Viscosity 1: For α > 3 Every Trajectory of ẍ + (α/t)ẋ + ∇Φ(x) = 0 Converges Weakly to a Minimizer of ΦResearch Paper

Motivation

Nesterov's accelerated gradient method and its proximal variant FISTA minimize a smooth convex function with a value gap of order O(1/k2)O(1/k^2)O(1/k2) after kkk iterations, against O(1/k)O(1/k)O(1/k) for plain gradient descent. They are among the most widely used first-order methods in large-scale optimization, signal processing and machine learning. Su, Boyd and Candès (JMLR 2016) observed that, for α=3\alpha = 3α=3, the second-order differential equation

x¨(t)+αt x˙(t)+∇Φ(x(t))=0(1)\ddot x(t) + \frac{\alpha}{t}\,\dot x(t) + \nabla\Phi(x(t)) = 0 \tag{1}x¨(t)+tα​x˙(t)+∇Φ(x(t))=0(1)

is a continuous-time limit of Nesterov's scheme, and proved Φ(x(t))−min⁡Φ=O(1/t2)\Phi(x(t)) - \min\Phi = O(1/t^2)Φ(x(t))−minΦ=O(1/t2) for α≥3\alpha \ge 3α≥3. A rate on the values says nothing about the trajectory itself: whether x(t)x(t)x(t) (or the iterates xkx_kxk​) converges at all was a long-standing question. The paper of Attouch, Chbani, Peypouquet and Redont answers it for α>3\alpha > 3α>3: every trajectory of (1) converges weakly to a minimizer of Φ\PhiΦ.

Timeline:

  • 1983 — Nesterov introduces the accelerated gradient method with an O(1/k2)O(1/k^2)O(1/k2) rate on the values.
  • 2000 — Alvarez proves weak convergence of the trajectories of the heavy ball with friction, x¨+γx˙+∇Φ(x)=0\ddot x + \gamma\dot x + \nabla\Phi(x) = 0x¨+γx˙+∇Φ(x)=0, whose damping is constant (SIAM J. Control Optim. 38).
  • 2009 — Beck and Teboulle extend it to composite problems (FISTA), still with a rate on the values only.
  • 2014–2016 — Su, Boyd, Candès identify (1) as the continuous model of Nesterov's method and prove the O(1/t2)O(1/t^2)O(1/t2) rate for α≥3\alpha\ge3α≥3.
  • 2015 — Attouch, Chbani, Peypouquet, Redont prove weak convergence of the trajectories of (1) for α>3\alpha > 3α>3 (this mission), and of the iterates of the corresponding algorithms; Chambolle and Dossal obtain the discrete result independently. The case α=3\alpha = 3α=3 remains open.

Setting

Let H\mathcal HH be a real Hilbert space with inner product ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle⟨⋅,⋅⟩ and norm ∥⋅∥\|\cdot\|∥⋅∥, and let Φ:H→R\Phi:\mathcal H\to\mathbb RΦ:H→R be a continuously differentiable convex function with gradient ∇Φ\nabla\Phi∇Φ. Fix a damping parameter α>0\alpha>0α>0 and an initial time t0>0t_0>0t0​>0. A solution of (1) on [t0,+∞[[t_0,+\infty[[t0​,+∞[ is a pair of maps x,vx, vx,v from the time axis to H\mathcal HH such that, at every t≥t0t\ge t_0t≥t0​, xxx has derivative v(t)v(t)v(t) and vvv has derivative −αtv(t)−∇Φ(x(t))-\frac{\alpha}{t}v(t) - \nabla\Phi(x(t))−tα​v(t)−∇Φ(x(t)). So v=x˙v=\dot xv=x˙, and x¨\ddot xx¨ satisfies (1). The damping coefficient α/t\alpha/tα/t is singular at 000 and vanishes as t→+∞t\to+\inftyt→+∞; this is why the time origin is positive.

Three functions of time measure the progress of a solution:

  • the global energy W(t)=12∥x˙(t)∥2+Φ(x(t))W(t) = \frac12\|\dot x(t)\|^2 + \Phi(x(t))W(t)=21​∥x˙(t)∥2+Φ(x(t));
  • the anchored distance hz(t)=12∥x(t)−z∥2h_z(t) = \frac12\|x(t)-z\|^2hz​(t)=21​∥x(t)−z∥2 to a point z∈Hz\in\mathcal Hz∈H;
  • when Φ\PhiΦ has a minimizer x∗x^*x∗, the anchored energies, for λ,ξ≥0\lambda,\xi\ge0λ,ξ≥0,
Eλ,ξ(t)=t2(Φ(x(t))−min⁡Φ)+12∥λ(x(t)−x∗)+tx˙(t)∥2+ξ2∥x(t)−x∗∥2.\mathcal E_{\lambda,\xi}(t) = t^2\big(\Phi(x(t))-\min\Phi\big) + \tfrac12\|\lambda(x(t)-x^*) + t\dot x(t)\|^2 + \tfrac{\xi}{2}\|x(t)-x^*\|^2 .Eλ,ξ​(t)=t2(Φ(x(t))−minΦ)+21​∥λ(x(t)−x∗)+tx˙(t)∥2+2ξ​∥x(t)−x∗∥2.

x(t)x(t)x(t) converges weakly to xˉ\bar xxˉ as t→+∞t\to+\inftyt→+∞ if ⟨x(t),y⟩→⟨xˉ,y⟩\langle x(t),y\rangle\to\langle\bar x,y\rangle⟨x(t),y⟩→⟨xˉ,y⟩ for every y∈Hy\in\mathcal Hy∈H. A weak limit point of x(t)x(t)x(t) is the weak limit of a sequence x(sn)x(s_n)x(sn​) with sn→+∞s_n\to+\inftysn​→+∞. argmin⁡Φ\operatorname{argmin}\PhiargminΦ is the set of minimizers of Φ\PhiΦ.

Formalization targets

Goal: Theorem 2.16

If argmin⁡Φ≠∅\operatorname{argmin}\Phi\ne\emptysetargminΦ=∅ and α>3\alpha>3α>3, then for every solution xxx of (1) there is xˉ∈argmin⁡Φ\bar x\in\operatorname{argmin}\Phixˉ∈argminΦ with

x(t)⇀xˉ(t→+∞).x(t)\rightharpoonup\bar x\qquad(t\to+\infty).x(t)⇀xˉ(t→+∞).

The goal asserts only the qualitative conclusion; no rate or constant enters it.

Milestones

  1. Lemma 2.1 (energy dissipation): W˙(t)=−αt∥x˙(t)∥2\dot W(t) = -\frac{\alpha}{t}\|\dot x(t)\|^2W˙(t)=−tα​∥x˙(t)∥2 for t>t0t>t_0t>t0​; WWW is nonincreasing with a limit in R∪{−∞}\mathbb R\cup\{-\infty\}R∪{−∞}, finite when Φ\PhiΦ is bounded below.
  2. (7): h¨z(t)+αth˙z(t)+Φ(x(t))−Φ(z)≤∥x˙(t)∥2\ddot h_z(t) + \frac{\alpha}{t}\dot h_z(t) + \Phi(x(t)) - \Phi(z) \le \|\dot x(t)\|^2h¨z​(t)+tα​h˙z​(t)+Φ(x(t))−Φ(z)≤∥x˙(t)∥2.
  3. Lemma 2.2: ∫t0t1s(W(s)−Φ(z)) ds≤C−1th˙z(t)−32αW(t)\int_{t_0}^t \frac1s(W(s)-\Phi(z))\,ds \le C - \frac1t\dot h_z(t) - \frac{3}{2\alpha}W(t)∫t0​t​s1​(W(s)−Φ(z))ds≤C−t1​h˙z​(t)−2α3​W(t) with an explicit constant CCC.
  4. Theorem 2.3 i), ii) (minimizing property, every α>0\alpha>0α>0): lim⁡W(t)=lim⁡Φ(x(t))=inf⁡Φ∈R∪{−∞}\lim W(t) = \lim \Phi(x(t)) = \inf\Phi\in\mathbb R\cup\{-\infty\}limW(t)=limΦ(x(t))=infΦ∈R∪{−∞}, and every weak limit point of x(t)x(t)x(t) is a minimizer.
  5. Remark 2.6: the Lyapunov inequality for ddtEλ,ξ\frac{d}{dt}\mathcal E_{\lambda,\xi}dtd​Eλ,ξ​, and monotonicity of Eλ,λ(α−λ−1)\mathcal E_{\lambda,\lambda(\alpha-\lambda-1)}Eλ,λ(α−λ−1)​ for α≥3\alpha\ge3α≥3, 2≤λ≤α−12\le\lambda\le\alpha-12≤λ≤α−1.
  6. Theorem 2.14 ii) with (13), (15): for α>3\alpha>3α>3, ∥x(t)−x∗∥2≤E2,2(α−3)(t0)/(α−3)\|x(t)-x^*\|^2 \le \mathcal E_{2,2(\alpha-3)}(t_0)/(\alpha-3)∥x(t)−x∗∥2≤E2,2(α−3)​(t0​)/(α−3) and ∫t0∞t∥x˙(t)∥2 dt≤E2,2(α−3)(t0)/(α−3)\int_{t_0}^{\infty} t\|\dot x(t)\|^2\,dt \le \mathcal E_{2,2(\alpha-3)}(t_0)/(\alpha-3)∫t0​∞​t∥x˙(t)∥2dt≤E2,2(α−3)​(t0​)/(α−3).
  7. Lemma A.4: if tw¨+αw˙≤gt\ddot w + \alpha\dot w \le gtw¨+αw˙≤g a.e. with α>1\alpha>1α>1, g≥0g\ge0g≥0 integrable and www bounded below, then [w˙]+[\dot w]_+[w˙]+​ is integrable and lim⁡w(t)\lim w(t)limw(t) exists.
  8. Lemma A.2 (Opial's lemma, continuous form).

Significance

The result. Theorem 2.16 is the first proof that the trajectories of the continuous Nesterov model converge, not only their values. The paper's discrete analysis parallels the continuous one and yields weak convergence of the iterates of Nesterov-type forward–backward algorithms for α>3\alpha>3α>3 (Theorem 5.3, a companion mission). The minimizing property (Theorem 2.3) holds for every α>0\alpha>0α>0, with no minimizer assumed, and shows that a bounded trajectory exists only if Φ\PhiΦ has a minimizer. Strong convergence results under further geometric assumptions (Theorems 3.1–3.3) build directly on Theorem 2.16.

Formalizing it. All statements are proved on paper. None of them, nor the differential equation (1), is formalized on Prove2Me or in Mathlib; the discrete analogue (weak convergence of the unperturbed accelerated forward–backward iterates) exists on the platform as a separate result. A formal development provides: a reusable encoding of solutions of a non-autonomous second-order ODE in a Hilbert space; Lyapunov arguments with one-sided derivatives on a half-line; a continuous-time Opial lemma, which is the standard tool for weak convergence of evolution equations and of semigroups; and the scalar differential-inequality lemma A.4.

Difficulty

Lyapunov functions such as WWW or Eα−1,0\mathcal E_{\alpha-1,0}Eα−1,0​ give rates on the values but not convergence of x(t)x(t)x(t): a decreasing energy says nothing about where the trajectory goes, and the minimizer set may be a continuum. The natural first idea, showing that ∥x(t)−x∗∥\|x(t)-x^*\|∥x(t)−x∗∥ is eventually monotone as for the gradient flow, fails: the inertial term makes hx∗h_{x^*}hx∗​ oscillate, and (7) controls only th¨+αh˙t\ddot h + \alpha\dot hth¨+αh˙, a second-order quantity. Making it usable requires integrability of t∥x˙(t)∥2t\|\dot x(t)\|^2t∥x˙(t)∥2 on [t0,+∞[[t_0,+\infty[[t0​,+∞[, which is not available from the Su–Boyd–Candès energy and holds only for α>3\alpha>3α>3; the borderline α=3\alpha=3α=3 is open. In infinite dimension, convergence is genuinely weak: bounded sets are not compact, so the argument must identify weak limit points through weak lower semicontinuity of Φ\PhiΦ and conclude through Opial's lemma.

Formalization scope

  • Space. H\mathcal HH is a real inner product space that is complete (InnerProductSpace ℝ H, CompleteSpace H); no finite dimension is assumed, since in finite dimension weak and norm convergence coincide.
  • Potential. Φ:H→R\Phi:\mathcal H\to\mathbb RΦ:H→R with ConvexOn ℝ Set.univ Φ and ContDiff ℝ 1 Φ; ∇Φ\nabla\Phi∇Φ is Mathlib's gradient. Minimizers are points zzz with Φ(z)≤Φ(y)\Phi(z)\le\Phi(y)Φ(z)≤Φ(y) for all yyy; min⁡Φ\min\PhiminΦ is written Φ(x∗)\Phi(x^*)Φ(x∗) for such a point.
  • Solutions. (1) is the first-order system x˙=v\dot x=vx˙=v, v˙=−αtv−∇Φ(x)\dot v=-\frac{\alpha}{t}v-\nabla\Phi(x)v˙=−tα​v−∇Φ(x), with derivatives within [t0,+∞[[t_0,+\infty[[t0​,+∞[ at every t≥t0t\ge t_0t≥t0​ and t0>0t_0>0t0​>0. Existence of solutions is not assumed or proved: every statement concerns a given solution, as in the paper.
  • Limits and integrals. Limits in R∪{−∞}\mathbb R\cup\{-\infty\}R∪{−∞} are taken in EReal, inf⁡Φ\inf\PhiinfΦ as an EReal infimum. Improper integrals ∫t0+∞\int_{t_0}^{+\infty}∫t0​+∞​ carry an explicit integrability conjunct; integrals over [t0,t][t_0,t][t0​,t] are interval integrals of continuous functions.
  • Explicit constants. The constant CCC of Lemma 2.2 and the bounds E2,2(α−3)(t0)/(α−3)\mathcal E_{2,2(\alpha-3)}(t_0)/(\alpha-3)E2,2(α−3)​(t0​)/(α−3) of (13), (15) are stated exactly as the paper computes them.
  • Trivializations ruled out. Weak convergence is not replaced by norm convergence, the derivative relations between xxx, vvv and their energies are part of the hypotheses or conclusions (never a free deriv), and the solution predicate is non-vacuous: the constant trajectory for Φ=0\Phi=0Φ=0 and the explicit solution x(t)=t2x(t)=t^2x(t)=t2 of Example 2.5 satisfy it.
  • Citation. Theorem numbers and pages refer to the Optimization Online preprint 5179 (October 2015), titled "…asymptotic vanishing damping", not to the Mathematical Programming typesetting.

Contributions of reusable infrastructure are welcome, in particular a continuous-time Opial lemma, weak lower semicontinuity of continuous convex functions on a Hilbert space along weakly convergent sequences, and integration-by-parts lemmas for one-sided derivatives on a half-line.

Selected references

  • H. Attouch, Z. Chbani, J. Peypouquet, P. Redont, Fast convergence of inertial dynamics and algorithms with asymptotic vanishing damping, Optimization Online preprint 5179, 2015; published as …vanishing viscosity, Mathematical Programming 168 (2018) 123–175. https://optimization-online.org/wp-content/uploads/2015/10/5179.pdf, https://doi.org/10.1007/s10107-016-0992-8
  • W. Su, S. Boyd, E. J. Candès, A differential equation for modeling Nesterov's accelerated gradient method: theory and insights, Journal of Machine Learning Research 17 (2016) 1–43. https://jmlr.org/papers/v17/15-084.html
  • F. Alvarez, On the minimizing property of a second order dissipative system in Hilbert spaces, SIAM Journal on Control and Optimization 38 (2000) 1102–1119. https://doi.org/10.1137/S0363012998335802
  • Z. Opial, Weak convergence of the sequence of successive approximations for nonexpansive mappings, Bulletin of the AMS 73 (1967) 591–597. https://doi.org/10.1090/S0002-9904-1967-11761-0
  • A. Beck, M. Teboulle, A fast iterative shrinkage-thresholding algorithm for linear inverse problems, SIAM Journal on Imaging Sciences 2 (2009) 183–202. https://doi.org/10.1137/080716542
  • A. Chambolle, Ch. Dossal, On the convergence of the iterates of the "fast iterative shrinkage/thresholding algorithm", Journal of Optimization Theory and Applications 166 (2015) 968–982. https://doi.org/10.1007/s10957-015-0746-4
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Numerical AnalysisOptimization·Captain: mikedeng1

First-Order Optimization Algorithms via Inertial Systems with Hessian Driven Damping VI: For µ-Strongly Convex f, (IGAHD-SC) Satisfies f(x_k) − min f = O(q^k) and ‖x_k − x⋆‖ = O(q^{k/2})Research Paper

Motivation

First-order methods use function gradients to minimize an objective without solving a second-order subproblem at each iteration. Inertial methods also use the previous iterate, which can improve the convergence rate but complicates the choice of momentum and step size. Attouch, Chbani, Fadili, and Riahi study a family of such methods derived from continuous dynamical systems with Hessian driven damping. Their explicit strongly convex scheme, IGAHD-SC, uses a difference of consecutive gradients in addition to momentum and the current gradient. The difference represents the damping contribution without evaluating a Hessian matrix. Attouch et al., §5.2, pp. 28–29.

The question in this mission is quantitative. If the objective has strong curvature and a Lipschitz gradient, do the iterates, objective values, and a discounted sum of squared gradients decrease at the geometric rates claimed in Theorem 11? This is the final independent convergence theorem of the paper's series of discrete algorithms. Attouch et al., Theorem 11, p. 29.

Setting

Let HHH be a real Hilbert space and f:H→Rf:H\to\mathbb Rf:H→R a continuously differentiable objective. For μ>0\mu>0μ>0, the paper calls fff μ\muμ-strongly convex when z↦f(z)−μ2∥z∥2z\mapsto f(z)-\frac\mu2\|z\|^2z↦f(z)−2μ​∥z∥2 is convex. Let x∗x^*x∗ be a minimizer of fff. The paper assumes that the gradient is LLL-Lipschitz for a positive constant LLL: ∥∇f(u)−∇f(w)∥≤L∥u−w∥\|\nabla f(u)-\nabla f(w)\|\le L\|u-w\|∥∇f(u)−∇f(w)∥≤L∥u−w∥ for every u,w∈Hu,w\in Hu,w∈H. Strong convexity makes the minimizer unique. Attouch et al., Definition 1, p. 19; Theorem 11, p. 29.

Choose parameters β≥0\beta\ge0β≥0 and s>0s>0s>0, and write r=μsr=\sqrt{\mu s}r=μs​. Starting from arbitrary x0,x1∈Hx_0,x_1\in Hx0​,x1​∈H, IGAHD-SC determines xk+1x_{k+1}xk+1​ for k≥1k\ge1k≥1 by

xk+1=xk+1−r1+r(xk−xk−1)−βs1+r(∇f(xk)−∇f(xk−1))−s1+r∇f(xk).x_{k+1}=x_k+\frac{1-r}{1+r}(x_k-x_{k-1}) -\frac{\beta\sqrt s}{1+r}\bigl(\nabla f(x_k)-\nabla f(x_{k-1})\bigr) -\frac{s}{1+r}\nabla f(x_k).xk+1​=xk​+1+r1−r​(xk​−xk−1​)−1+rβs​​(∇f(xk​)−∇f(xk−1​))−1+rs​∇f(xk​).

The two differences have different roles: xk−xk−1x_k-x_{k-1}xk​−xk−1​ is the inertial part, and ∇f(xk)−∇f(xk−1)\nabla f(x_k)-\nabla f(x_{k-1})∇f(xk​)−∇f(xk−1​) is the Hessian damping term in this explicit discretization. The algorithm is exactly the displayed scheme on p. 28, with its two starting points free. Attouch et al., (25) and (IGAHD-SC), p. 28.

Formalization targets

Theorem 11 assumes β≤1/μ\beta\le1/\sqrt\muβ≤1/μ​ and the two smoothness bounds in (26). Define

q=11+12μs,θ=11+μs.q=\frac{1}{1+\frac12\sqrt{\mu s}},\qquad \theta=\frac{1}{1+\sqrt{\mu s}}.q=1+21​μs​1​,θ=1+μs​1​.

Both constants lie strictly between zero and one. The mission's goal is the paper's three-part conclusion:

∥xk−x∗∥=O(qk/2),f(xk)−f(x∗)=O(qk),\|x_k-x^*\|=O(q^{k/2}),\qquad f(x_k)-f(x^*)=O(q^k),∥xk​−x∗∥=O(qk/2),f(xk​)−f(x∗)=O(qk),

and

θk∑j=0k−2θ−j∥∇f(xj)∥2=O(qk)(k→∞).\theta^k\sum_{j=0}^{k-2}\theta^{-j}\|\nabla f(x_j)\|^2=O(q^k) \quad (k\to\infty).θkj=0∑k−2​θ−j∥∇f(xj​)∥2=O(qk)(k→∞).

The milestones record the auxiliary vector and energy from the proof, their velocity and strong-convexity estimates, the gradient majorization, the one-step energy inequality, and the geometric energy bound. These are claims displayed by the authors on pp. 30–32, in the order in which they lead to the goal. Attouch et al., proof of Theorem 11, pp. 30–32.

Significance

The first two bounds give geometric decay of distance to the optimizer and of objective error for the specified parameter regime. The third controls a discounted accumulation of squared gradients. Together they describe more than convergence of the objective alone: the same run has explicit asymptotic rates for its points and gradient behavior. The rate constants depend on the strong-convexity parameter, step size, and allowed damping range. Attouch et al., Theorem 11, p. 29.

This result is proved in the cited paper; the open work here is its Lean formalization. A completed development would include a reusable representation of the explicit inertial run, a precise strong-convexity interface matching Definition 1, and the energy estimates that support the theorem. The formal statements in this proposal are proof targets, not claims that already have machine-checked proofs. The two comparison methods mentioned in Remark 10 use different discretizations or hypotheses, so their rate theorems cannot replace this target. Attouch et al., Remark 10, p. 29.

Difficulty

Ordinary smooth gradient descent is controlled by the current gradient and one step difference. Here the recurrence also contains the preceding gradient and the preceding step. A direct estimate of f(xk+1)−f(x∗)f(x_{k+1})-f(x^*)f(xk+1​)−f(x∗) does not isolate a contracting quantity. The paper therefore tracks an auxiliary vector and an energy involving both the objective gap and that vector; the precise coefficients in the two bounds of (26) are needed for the final one-step inequality. The proof's intermediate display on p. 31 also changes a gradient index between lines, so each formalized displayed claim needs scrutiny against the recurrence and the final p. 32 inequality. Attouch et al., proof of Theorem 11, pp. 30–32.

Formalization scope

Lean represents HHH as a complete real inner-product space, ∇f\nabla f∇f by Mathlib's gradient, and the run as a predicate on a sequence x:N→Hx:\mathbb N\to Hx:N→H obeying (IGAHD-SC) for every k≥1k\ge1k≥1. The source's arbitrary initial pair is preserved. A witness x∗x^*x∗ and the hypothesis that it minimizes fff express the nonempty argmin assumption without taking an infimum of real values. The strong-convexity definition is exactly Definition 1. Positive sss, μ\muμ, and LLL make every square root and step-size denominator meaningful. The first bound in (26) is written 8βL≤μ8\beta L\le\sqrt\mu8βL≤μ​, which retains the paper's intended β=0\beta=0β=0 case; the paper later uses 0≤β0\le\beta0≤β explicitly, so it is included. Attouch et al., pp. 19, 28–32.

The rates use =O[Filter.atTop]. Lean writes qk/2q^{k/2}qk/2 as (q)k(\sqrt q)^k(q​)k, and the sum through k−2k-2k−2 as Finset.range (k - 1). For k=0,1k=0,1k=0,1 the finite range is empty; the asymptotic claim concerns large kkk. The source prints ppp in the sum limit and jjj in its summand; both are read as jjj. The goal itself mentions the iterates, objective values, and gradients, without assuming an energy decay bound. A complete proof can contribute reusable inequalities for strongly convex functions with Lipschitz gradients and geometric recurrences, alongside the paper-specific run and energy lemmas.

Selected references

  • H. Attouch, Z. Chbani, J. Fadili, and H. Riahi, First-order optimization algorithms via inertial systems with Hessian driven damping, Mathematical Programming, 2020; arXiv:1907.10536v2.
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Optimization·Captain: mikedeng1

The Direct Extension of ADMM for Multi-block Convex Minimization Problems is Not Necessarily Convergent II: On a Three-Block Linear System the Extended ADMM Diverges for Every β > 0Research Paper

Motivation

The alternating direction method of multipliers (ADMM) solves linearly constrained problems whose objective splits into separately treatable blocks. For two blocks, min⁡{θ1(x1)+θ2(x2):A1x1+A2x2=b}\min\{\theta_1(x_1)+\theta_2(x_2) : A_1x_1+A_2x_2=b\}min{θ1​(x1​)+θ2​(x2​):A1​x1​+A2​x2​=b}, it alternates one minimisation of the augmented Lagrangian in each block with a multiplier update. Its convergence for closed convex θ1,θ2\theta_1,\theta_2θ1​,θ2​ has been known since the work of Glowinski–Marrocco (1975) and Gabay–Mercier (1976), and the survey of Boyd, Parikh, Chu, Peleato and Eckstein (2011) made it a standard tool in statistics, imaging and machine learning.

Many applications have three or more blocks: robust principal component analysis with noisy and incomplete data, latent-variable graphical model selection, image alignment. Practitioners therefore apply the direct extension of ADMM, which simply cycles through all blocks in Gauss–Seidel order before updating the multiplier. Whether this extension converges for convex problems remained open for years: convergence was known under extra assumptions (strong convexity with a restricted penalty, Han–Yuan 2012; orthogonality of coefficient matrices, Section 2 of the source paper), and modified schemes with correction steps were proposed precisely because no proof was available.

Chen, He, Ye and Yuan (Math. Program., 2014) settled the question negatively by an explicit three-block example. This mission formalizes that example and the paper's main theorem.

Setting

Problem (1.1). Given Ai∈Rp×niA_i\in\mathbb R^{p\times n_i}Ai​∈Rp×ni​, b∈Rpb\in\mathbb R^pb∈Rp, closed convex sets Xi⊆Rni\mathcal X_i\subseteq\mathbb R^{n_i}Xi​⊆Rni​ and convex functions θi:Rni→R\theta_i:\mathbb R^{n_i}\to\mathbb Rθi​:Rni​→R (i=1,2,3)(i=1,2,3)(i=1,2,3), with a nonempty solution set,

min⁡ θ1(x1)+θ2(x2)+θ3(x3)s.t.A1x1+A2x2+A3x3=b, xi∈Xi.\min\ \theta_1(x_1)+\theta_2(x_2)+\theta_3(x_3)\quad\text{s.t.}\quad A_1x_1+A_2x_2+A_3x_3=b,\ x_i\in\mathcal X_i .min θ1​(x1​)+θ2​(x2​)+θ3​(x3​)s.t.A1​x1​+A2​x2​+A3​x3​=b, xi​∈Xi​.

Augmented Lagrangian (1.6). For a penalty β>0\beta>0β>0 and multiplier λ∈Rp\lambda\in\mathbb R^pλ∈Rp,

LA(x1,x2,x3,λ)=∑i=13θi(xi)−λT(A1x1+A2x2+A3x3−b)+β2∥A1x1+A2x2+A3x3−b∥2.\mathcal L_{\mathcal A}(x_1,x_2,x_3,\lambda)=\sum_{i=1}^3\theta_i(x_i)-\lambda^T(A_1x_1+A_2x_2+A_3x_3-b)+\tfrac{\beta}{2}\|A_1x_1+A_2x_2+A_3x_3-b\|^2 .LA​(x1​,x2​,x3​,λ)=i=1∑3​θi​(xi​)−λT(A1​x1​+A2​x2​+A3​x3​−b)+2β​∥A1​x1​+A2​x2​+A3​x3​−b∥2.

Direct extension of ADMM (1.5). From (x2k,x3k,λk)(x_2^k,x_3^k,\lambda^k)(x2k​,x3k​,λk): x1k+1x_1^{k+1}x1k+1​ minimises LA(⋅,x2k,x3k,λk)\mathcal L_{\mathcal A}(\cdot,x_2^k,x_3^k,\lambda^k)LA​(⋅,x2k​,x3k​,λk) over X1\mathcal X_1X1​; x2k+1x_2^{k+1}x2k+1​ minimises LA(x1k+1,⋅,x3k,λk)\mathcal L_{\mathcal A}(x_1^{k+1},\cdot,x_3^k,\lambda^k)LA​(x1k+1​,⋅,x3k​,λk) over X2\mathcal X_2X2​; x3k+1x_3^{k+1}x3k+1​ minimises LA(x1k+1,x2k+1,⋅,λk)\mathcal L_{\mathcal A}(x_1^{k+1},x_2^{k+1},\cdot,\lambda^k)LA​(x1k+1​,x2k+1​,⋅,λk) over X3\mathcal X_3X3​; and λk+1=λk−β(A1x1k+1+A2x2k+1+A3x3k+1−b)\lambda^{k+1}=\lambda^k-\beta(A_1x_1^{k+1}+A_2x_2^{k+1}+A_3x_3^{k+1}-b)λk+1=λk−β(A1​x1k+1​+A2​x2k+1​+A3​x3k+1​−b). A sequence satisfying these four conditions for every kkk is a run (IsRun15).

The example. System (3.1) is A1x1+A2x2+A3x3=0A_1x_1+A_2x_2+A_3x_3=0A1​x1​+A2​x2​+A3​x3​=0 with columns Ai∈R3A_i\in\mathbb R^3Ai​∈R3, scalar unknowns, zero objective, b=0b=0b=0 and Xi=R\mathcal X_i=\mathbb RXi​=R; its unique solution is x=0x=0x=0 when [A1,A2,A3][A_1,A_2,A_3][A1​,A2​,A3​] is nonsingular. The paper takes

A=(A1,A2,A3)=(111112122)(3.10),A=(A_1,A_2,A_3)=\begin{pmatrix}1&1&1\\1&1&2\\1&2&2\end{pmatrix}\qquad(3.10),A=(A1​,A2​,A3​)=​111​112​122​​(3.10),

the instance example310. With the scaled multiplier μ=λ/β\mu=\lambda/\betaμ=λ/β, the state is z=(x2,x3,μ1,μ2,μ3)∈R5z=(x_2,x_3,\mu_1,\mu_2,\mu_3)\in\mathbb R^5z=(x2​,x3​,μ1​,μ2​,μ3​)∈R5 (stateVec). The 5×55\times55×5 matrices LLL (3.6) and RRR (3.7) are built from the inner products AiTAjA_i^TA_jAiT​Aj​ and the columns, and M=L−1RM=L^{-1}RM=L−1R (3.9).

Formalization targets

Goal: Theorem 3.1

For the instance (3.10), which satisfies the standing assumptions of (1.1), there are a three-dimensional subspace S⊆R5S\subseteq\mathbb R^5S⊆R5 and a nonzero linear functional φ\varphiφ on SSS such that for every β>0\beta>0β>0 and every starting point with

(x20, x30, λ0/β)∈S,φ(x20,x30,λ0/β)>0,\bigl(x_2^0,\,x_3^0,\,\lambda^0/\beta\bigr)\in S,\qquad \varphi\bigl(x_2^0,x_3^0,\lambda^0/\beta\bigr)>0,(x20​,x30​,λ0/β)∈S,φ(x20​,x30​,λ0/β)>0,

a run of (1.5) from (x20,x30,λ0)(x_2^0,x_3^0,\lambda^0)(x20​,x30​,λ0) exists and no such run converges.

Milestones

  1. (3.4)–(3.5): on (3.1), every run satisfies x1k+1=1A1TA1(−A1TA2x2k−A1TA3x3k+A1Tμk)x_1^{k+1}=\frac{1}{A_1^TA_1}(-A_1^TA_2x_2^k-A_1^TA_3x_3^k+A_1^T\mu^k)x1k+1​=A1T​A1​1​(−A1T​A2​x2k​−A1T​A3​x3k​+A1T​μk) and Lzk+1=RzkLz^{k+1}=Rz^kLzk+1=Rzk, with L,RL,RL,R independent of β\betaβ.
  2. (3.8)–(3.9): zk=Mkz0z^k=M^kz^0zk=Mkz0.
  3. LLL, RRR, MMM for (3.10): the printed 5×55\times55×5 matrices, det⁡L=54\det L=54detL=54 and M=L−1RM=L^{-1}RM=L−1R.
  4. ρ(M)=∣d1∣=∣d2∣>1\rho(M)=|d_1|=|d_2|>1ρ(M)=∣d1​∣=∣d2​∣>1: MMM has a non-real eigenvalue of maximal modulus, and that modulus exceeds 111.
  5. (3.12)–(3.13): a three-dimensional real subspace and a nonzero functional φ\varphiφ on it such that ∥Mkz∥→∞\|M^kz\|\to\infty∥Mkz∥→∞ whenever φ(z)≠0\varphi(z)\neq0φ(z)=0.

Significance

The theorem shows that convexity alone does not make the cyclic three-block ADMM convergent, and the failure is robust: it holds for every penalty parameter and for an open half of a three-dimensional subspace of starting points, on a problem as simple as a nonsingular homogeneous linear system with zero objective. It explains why later convergent variants add assumptions (strong convexity, orthogonality, small step sizes, randomised block order) or modify the scheme, and it is the standard reference for that fact in the operator-splitting literature.

The result is proved in the paper; no machine-checked version is known. A formal version produces a certified negative example for the most widely used multi-block splitting heuristic, a reusable formal model of the extended ADMM (Problem, augLag, IsRun15) on which convergent variants can later be stated, and a worked instance of turning a numerically presented spectral argument (the paper prints its eigen-decomposition to four digits) into exact statements.

Difficulty

The first step, that the iteration on (3.1) is linear in (x2,x3,μ)(x_2,x_3,\mu)(x2​,x3​,μ) and independent of β\betaβ, is elementary but requires extracting minimisers of convex quadratics from the minimiser conditions of the run. The main difficulty is exact spectral information about a specific 5×55\times55×5 rational matrix whose characteristic polynomial is xxx times an irreducible quartic over Q\mathbb QQ with two pairs of complex roots of moduli about 1.02781.02781.0278 and 0.90440.90440.9044. The paper's evidence is a floating-point eigen-decomposition; a proof must instead locate the roots exactly, for example by certified bounds, and must show that the divergent component is present for a whole real subspace of starting points rather than for one numerically chosen vector. Finally, unboundedness of the scaled state has to be transferred back to the original sequence (x1k,x2k,x3k,λk)(x_1^k,x_2^k,x_3^k,\lambda^k)(x1k​,x2k​,x3k​,λk) for every β>0\beta>0β>0.

Formalization scope

Vectors are Fin n → ℝ, matrices Matrix (Fin p) (Fin n) ℝ, and ∥r∥2\|r\|^2∥r∥2 in (1.6) is the dot product r⋅rr\cdot rr⋅r. Each θi\theta_iθi​ is real-valued and convex on all of Rni\mathbb R^{n_i}Rni​; "closed" is automatic for such functions and is not stated separately. "Argmin" is read as "a minimiser": the run predicate does not select a minimiser, and the goal asserts that a run exists, so the non-convergence claim is not vacuous. The paper's blocks and multiplier components are 1-based, the Lean components 0-based. Convergence of the sequence is convergence of (x1k,x2k,x3k,λk)(x_1^k,x_2^k,x_3^k,\lambda^k)(x1k​,x2k​,x3k​,λk) in the product topology; x10x_1^0x10​ is never read by (1.5). "Divergent" means "not convergent". The "continuously dense half space of dimension 3" is {z∈S:φ(z)>0}\{z\in S:\varphi(z)>0\}{z∈S:φ(z)>0} for a three-dimensional subspace SSS and nonzero linear φ\varphiφ, expressed in the coordinates (x20,x30,λ0/β)(x_2^0,x_3^0,\lambda^0/\beta)(x20​,x30​,λ0/β); SSS and φ\varphiφ are chosen before β\betaβ, as in the paper. Requiring dim⁡S=3\dim S=3dimS=3 and φ≠0\varphi\neq0φ=0 rules out the trivial choices S={0}S=\{0\}S={0} or φ=0\varphi=0φ=0. Eigenvalues are complex roots of the characteristic polynomial; a statement using only real eigenvalues would be wrong, since the only real eigenvalue of MMM is 000. Norms enter only through "→∞\to\infty→∞", where the choice of norm on R5\mathbb R^5R5 is irrelevant. The rounded numbers of (3.11) are not used anywhere.

Every object is defined in ExtADMM.Diverge.Setting. The general definitions (problem, augmented Lagrangian, run) are written for arbitrary dimensions and are intended for reuse by later missions on multi-block splitting. Contributions welcome: proofs of the milestones, exact root localisation for the quartic factor of the characteristic polynomial, and general lemmas such as "a real matrix with an eigenvalue of modulus above one has unbounded orbits on a real subspace".

Selected references

  • C. Chen, B. He, Y. Ye, X. Yuan, The direct extension of ADMM for multi-block convex minimization problems is not necessarily convergent, Mathematical Programming 155 (2016) 57–79. https://doi.org/10.1007/s10107-014-0826-5
  • D. Gabay, B. Mercier, A dual algorithm for the solution of nonlinear variational problems via finite element approximation, Computers & Mathematics with Applications 2 (1976) 17–40. https://doi.org/10.1016/0898-1221(76)90003-1
  • R. Glowinski, A. Marrocco, Sur l'approximation, par éléments finis d'ordre un, et la résolution, par pénalisation-dualité, d'une classe de problèmes de Dirichlet non linéaires, RAIRO Analyse Numérique 9 (1975) 41–76. https://doi.org/10.1051/m2an/197509R200411
  • S. Boyd, N. Parikh, E. Chu, B. Peleato, J. Eckstein, Distributed optimization and statistical learning via the alternating direction method of multipliers, Foundations and Trends in Machine Learning 3 (2011) 1–122. https://doi.org/10.1561/2200000016
  • D. Han, X. Yuan, A note on the alternating direction method of multipliers, Journal of Optimization Theory and Applications 155 (2012) 227–238. https://doi.org/10.1007/s10957-012-0003-z
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Operations ResearchOptimal TransportOptimization·Captain: mikedeng1

Optimal Transport-Based Distributionally Robust Optimization: Structural Properties and Iterative Schemes 3: The Dual Objective Is √δκ₁-Strongly Convex in (β, λ) Near the Dual OptimizersResearch Paper

Motivation

A decision based on observed data can change when the data law differs from the one used to choose it. Distributionally robust optimization addresses this by evaluating each decision against a family of nearby probability laws. Optimal transport gives one way to define “nearby”: a candidate law is admissible when probability mass can be moved from the baseline law at a bounded expected cost. For a linear decision rule, the resulting worst-case expectation is usually harder to optimize than an ordinary sample-average loss. Blanchet, Murthy, and Zhang identify a dual objective whose variables are the decision vector and a scalar transport multiplier, then study its curvature near the multipliers that actually minimize it (Blanchet–Murthy–Zhang, 2022).

The paper proves that this dual objective is jointly strongly convex on a specified region for sufficiently small transport radius. This matters because ordinary convexity allows flat directions in the joint decision–multiplier space. The joint lower Hessian bound gives local curvature in every direction with one positive modulus that remains independent of the radius apart from the paper's explicit factor δ\sqrt{\delta}δ​ (Theorem 4, p. 11).

Setting

Let X∈RdX\in\mathbb R^dX∈Rd have a baseline probability law P0P_0P0​, and let a decision be a vector β\betaβ in a nonempty compact convex set B⊆RdB\subseteq\mathbb R^dB⊆Rd. The loss of a possible outcome xxx is ℓ(βTx)\ell(\beta^{\mathsf T}x)ℓ(βTx) for a convex function ℓ:R→R\ell:\mathbb R\to\mathbb Rℓ:R→R. A state-dependent positive-definite matrix A(x)A(x)A(x) sets the cost of moving mass from xxx to x′x'x′:

c(x,x′)=(x−x′)TA(x)(x−x′).c(x,x')=(x-x')^{\mathsf T}A(x)(x-x').c(x,x′)=(x−x′)TA(x)(x−x′).

Assumption 1 requires this cost to be lower semicontinuous and the eigenvalues of A(x)A(x)A(x) to lie between positive constants ρmin⁡\rho_{\min}ρmin​ and ρmax⁡\rho_{\max}ρmax​ for P0P_0P0​-almost every xxx. Assumption 2 requires at most quadratic growth of ℓ\ellℓ and a finite fourth moment of P0P_0P0​. The ambiguity radius δ\deltaδ is positive (Assumptions 1–2, pp. 9–10).

The paper's dual objective is an expectation under the known law P0P_0P0​. Write qA(β,x)=βTA(x)−1βq_A(\beta,x)=\beta^{\mathsf T}A(x)^{-1}\betaqA​(β,x)=βTA(x)−1β. For a scalar λ≥0\lambda\ge0λ≥0 and an auxiliary scalar γ\gammaγ, set

F(γ,β,λ;x)=ℓ(βTx+γδ qA(β,x))−λδ(γ2qA(β,x)−1),fδ(β,λ)=EP0 ⁣[sup⁡γ∈RF(γ,β,λ;X)].F(\gamma,\beta,\lambda;x) =\ell\bigl(\beta^{\mathsf T}x+\gamma\sqrt\delta\,q_A(\beta,x)\bigr) -\lambda\sqrt\delta\bigl(\gamma^2q_A(\beta,x)-1\bigr), \qquad f_\delta(\beta,\lambda)=\mathbb E_{P_0}\!\left[\sup_{\gamma\in\mathbb R}F(\gamma,\beta,\lambda;X)\right].F(γ,β,λ;x)=ℓ(βTx+γδ​qA​(β,x))−λδ​(γ2qA​(β,x)−1),fδ​(β,λ)=EP0​​[γ∈Rsup​F(γ,β,λ;X)].

This value may be +∞+\infty+∞. Under the paper's duality conditions, minimizing fδ(β,λ)f_\delta(\beta,\lambda)fδ​(β,λ) over λ≥0\lambda\ge0λ≥0 gives the worst-case loss at β\betaβ (Theorem 1 and (7), p. 10).

Formalization targets

Assumption 3 bounds ℓ′′\ell''ℓ′′ above by M>0M>0M>0 and excludes an almost surely zero ℓ′(βTX)\ell'(\beta^{\mathsf T}X)ℓ′(βTX) for each β∈B\beta\in Bβ∈B. Assumption 4 makes BBB compact. Lemma 6 supplies positive constants L‾,L‾\underline L,\overline LL​,L bounding EP0[ℓ′(βTX)2]\mathbb E_{P_0}[\ell'(\beta^{\mathsf T}X)^2]EP0​​[ℓ′(βTX)2] uniformly over BBB. With Rβ=sup⁡β∈B∥β∥R_\beta=\sup_{\beta\in B}\|\beta\|Rβ​=supβ∈B​∥β∥, the constants K1,K2K_1,K_2K1​,K2​ are those of (28), and

Vδ={(β,λ):β∈B, λ≥0, K1∥β∥≤λ≤K2∥β∥}.\mathbb V_\delta=\{(\beta,\lambda):\beta\in B,\ \lambda\ge0,\ K_1\|\beta\|\le\lambda\le K_2\|\beta\|\}.Vδ​={(β,λ):β∈B, λ≥0, K1​∥β∥≤λ≤K2​∥β∥}.

Theorem 3 first gives a bounded Hessian on Vδ\mathbb V_\deltaVδ​ and a positive lower bound on its β\betaβ block when 0<δ<δ00<\delta<\delta_00<δ<δ0​, with the explicit δ0\delta_0δ0​ from p. 36. The goal, Theorem 4, adds Assumption 5: ℓ\ellℓ is locally strongly convex and, at each β∈B\beta\in Bβ∈B, the loss derivative and the linear score are simultaneously separated from zero with positive probability. It asserts the joint bound

∃ δ1∈(0,δ0), κ1>0∀ δ∈(0,δ1), ∀ θ∈Vδ:∇2fδ(θ)⪰δ κ1Id+1.\exists\,\delta_1\in(0,\delta_0),\ \kappa_1>0\quad \forall\,\delta\in(0,\delta_1),\ \forall\,\theta\in\mathbb V_\delta:\quad \nabla^2 f_\delta(\theta)\succeq\sqrt\delta\,\kappa_1 I_{d+1}.∃δ1​∈(0,δ0​), κ1​>0∀δ∈(0,δ1​), ∀θ∈Vδ​:∇2fδ​(θ)⪰δ​κ1​Id+1​.

The order of the quantifiers is part of the target: κ1\kappa_1κ1​ works for every sufficiently small δ\deltaδ (Theorems 3–4, p. 11).

Significance

The Hessian bound makes the joint dual parameters locally identifiable by curvature on a region that contains every dual optimizer. In the paper, this structure also underlies the analysis of algorithms and of how the optimizer changes with the transport radius (Proposition 1, p. 11; §3 and §5.4). Theorem 4 is already proved in the paper; this mission asks for its machine-checked formalization, together with the stated bounds on multipliers, the maximizing scalar, and the intermediate curvature results. The general optimal-transport integral used here already has a published Prove2Me definition from Blanchet and Murthy's earlier model-risk work. The new definitions specify this paper's Mahalanobis model, regions, and smoothness assumptions.

Difficulty

Convexity alone gives only a nonnegative Hessian; it cannot produce a strictly positive joint lower bound. Even curvature of ℓ\ellℓ does not by itself control directions that combine a change in β\betaβ with a change in λ\lambdaλ. The inner supremum over γ\gammaγ can become infinite outside its effective domain, while at β=0\beta=0β=0 its maximizer ceases to be unique. The theorem therefore needs a region where the dual objective is finite and differentiable and a probabilistic condition that prevents the relevant score and derivative from vanishing together. The target keeps the actual δ\sqrt\deltaδ​ scale instead of settling for a radius-dependent positive constant (§2.2.2 and Remark 4, pp. 10–12, 39).

Formalization scope

Lean uses EuclideanSpace ℝ (Fin d) for Rd\mathbb R^dRd, a Borel probability measure for P0P_0P0​, and EReal for fδf_\deltafδ​ and the inner supremum. The reused extended-real integral records the +∞+\infty+∞ and −∞-\infty−∞ cases; the Hessian is taken only where fδf_\deltafδ​ is finite on a neighborhood and its real representative is differentiable there. Quadratic Hessian forms use ∥vβ∥2+vλ2\|v_\beta\|^2+v_\lambda^2∥vβ​∥2+vλ2​, since Lean's product norm is not the paper's Euclidean norm. The compact set BBB is explicitly nonempty, and the positive ambiguity radius δ\deltaδ is quantified inside the goal so that δ1\delta_1δ1​ and κ1\kappa_1κ1​ are uniform in δ\deltaδ. Theorem 3 additionally assumes Rβ>0R_\beta>0Rβ​>0 for the proof's explicit formula for δ0\delta_0δ0​: nonempty compact B={0}B=\{0\}B={0} would make that formula zero. Assumption 5 already gives Rβ>0R_\beta>0Rβ​>0 in the goal.

The goal retains Assumption 5's per-decision quantifiers. That assumption itself excludes 0∈B0\in B0∈B: its strict score event is empty at β=0\beta=0β=0. Intermediate statements where the printed wording includes β=0\beta=0β=0 but the claim fails there state β≠0\beta\ne0β=0 explicitly. Lemma 5 also states the differentiability and positive-multiplier conditions needed for its derivative and division. Proposition 9(b)'s printed strict curvature-margin inequality is corrected to the nonstrict inequality derived in its proof; its original wording is preserved in the milestone quotation. The claims are about the expectation fδf_\deltafδ​, with κ1\kappa_1κ1​ independent of δ\deltaδ, rather than a pointwise or merely convex substitute.

A complete development needs measurable extended-real integration, the matrix quadratic form and its inverse, almost-everywhere spectral bounds, differentiability under an expectation, and Hessian estimates for an optimized scalar. The transport integral, the assumptions and constants, and the multiplier bounds are intended as reusable interfaces for the companion missions. Contributions that close the listed lemmas or add the paper's omitted second-order kernel formula are within scope.

Selected references

  • José Blanchet, Karthyek Murthy, and Fan Zhang, Optimal Transport-Based Distributionally Robust Optimization: Structural Properties and Iterative Schemes, Mathematics of Operations Research 47(2), 2022. arXiv:1810.02403v3; DOI:10.1287/moor.2021.1178.
  • José Blanchet and Karthyek Murthy, Quantifying Distributional Model Risk via Optimal Transport, Mathematics of Operations Research 44(2), 2019. arXiv:1604.01446v2.
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Numerical AnalysisOptimization·Captain: mikedeng1

First-Order Optimization Algorithms via Inertial Systems with Hessian Driven Damping V: For µ-Strongly Convex f, (IPAHD-SC) Satisfies f(x_k) − min f ≤ E₁q^{k−1}, q = 1/(1 + ½√(µs))Research Paper

Motivation

Many first-order optimization methods are discretizations of second-order differential equations. In the continuous system the velocity carries the momentum, and the damping terms decide how fast the trajectory settles at a minimizer. Attouch, Chbani, Fadili and Riahi study inertial systems with Hessian driven damping: a friction term proportional to ∇2f(x(t))x˙(t)\nabla^2 f(x(t))\dot x(t)∇2f(x(t))x˙(t), which damps the oscillations that plain heavy-ball and Nesterov-type dynamics show. Because ∇2f(x(t))x˙(t)\nabla^2 f(x(t))\dot x(t)∇2f(x(t))x˙(t) is the time derivative of ∇f(x(t))\nabla f(x(t))∇f(x(t)), a discretization can use differences of gradients and never evaluate a Hessian. Attouch et al., §1, pp. 1–3.

For a μ\muμ-strongly convex objective, the paper shows that the dynamic

x¨(t)+2μ x˙(t)+β∇2f(x(t))x˙(t)+∇f(x(t))=0\ddot x(t)+2\sqrt\mu\,\dot x(t)+\beta\nabla^2f(x(t))\dot x(t)+\nabla f(x(t))=0x¨(t)+2μ​x˙(t)+β∇2f(x(t))x˙(t)+∇f(x(t))=0

makes f(x(t))−min⁡ff(x(t))-\min ff(x(t))−minf decay like e−μ2te^{-\frac{\sqrt\mu}{2}t}e−2μ​​t (Theorem 7, p. 19). Section 5.1 asks whether that rate survives an implicit (proximal) discretization. The answer is Theorem 9: the algorithm converges linearly, and the gradients also go to zero at a geometric rate. The authors remark that they know of no earlier result of this kind for such a proximal algorithm. Attouch et al., Theorem 9 and Remark 9, p. 23.

Setting

Let HHH be a real Hilbert space with inner product ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle⟨⋅,⋅⟩ and norm ∥⋅∥\|\cdot\|∥⋅∥, and let f:H→Rf:H\to\mathbb Rf:H→R be convex and continuously differentiable, with gradient ∇f\nabla f∇f. For μ>0\mu>0μ>0, fff is μ\muμ-strongly convex when z↦f(z)−μ2∥z∥2z\mapsto f(z)-\frac\mu2\|z\|^2z↦f(z)−2μ​∥z∥2 is convex (Definition 1, p. 19). Such an fff has at most one minimizer; write x⋆x^\starx⋆ for it.

For γ>0\gamma>0γ>0 and y∈Hy\in Hy∈H, the proximal point prox⁡γf(y)\operatorname{prox}_{\gamma f}(y)proxγf​(y) is the minimizer of z↦γf(z)+12∥z−y∥2z\mapsto\gamma f(z)+\frac12\|z-y\|^2z↦γf(z)+21​∥z−y∥2.

Fix β≥0\beta\ge0β≥0 and a step s>0s>0s>0 (the paper writes s=h2s=h^2s=h2 with hhh the step size). Starting from arbitrary x0,x1∈Hx_0,x_1\in Hx0​,x1​∈H, the inertial proximal algorithm with Hessian damping for strongly convex functions, (IPAHD-SC), produces for k≥1k\ge1k≥1

{yk=xk+(1−2μs1+2μs)(xk−xk−1)+βs(1−2μs1+2μs)∇f(xk),xk+1=prox⁡βs+s1+2μsf(yk).\begin{cases} y_k=x_k+\Big(1-\frac{2\sqrt{\mu s}}{1+2\sqrt{\mu s}}\Big)(x_k-x_{k-1})+\beta\sqrt s\Big(1-\frac{2\sqrt{\mu s}}{1+2\sqrt{\mu s}}\Big)\nabla f(x_k),\\[4pt] x_{k+1}=\operatorname{prox}_{\frac{\beta\sqrt s+s}{1+2\sqrt{\mu s}}f}(y_k). \end{cases}⎩⎨⎧​yk​=xk​+(1−1+2μs​2μs​​)(xk​−xk−1​)+βs​(1−1+2μs​2μs​​)∇f(xk​),xk+1​=prox1+2μs​βs​+s​f​(yk​).​

The first line is an extrapolation with momentum and an explicit gradient correction; the second is one implicit (proximal) step. Attouch et al., (IPAHD-SC), p. 23.

The rates are

q=11+12μs,θ=11+μs,q=\frac{1}{1+\frac12\sqrt{\mu s}},\qquad \theta=\frac{1}{1+\sqrt{\mu s}},q=1+21​μs​1​,θ=1+μs​1​,

both in ]0,1[]0,1[]0,1[, and the constant of the theorem is

E1=f(x1)−f(x⋆)+12∥μ(x1−x⋆)+1s(x1−x0)+β∇f(x1)∥2.E_1=f(x_1)-f(x^\star)+\tfrac12\Big\|\sqrt\mu(x_1-x^\star)+\tfrac{1}{\sqrt s}(x_1-x_0)+\beta\nabla f(x_1)\Big\|^2.E1​=f(x1​)−f(x⋆)+21​​μ​(x1​−x⋆)+s​1​(x1​−x0​)+β∇f(x1​)​2.

Formalization targets

Goal: Theorem 9

Assume 0≤β≤12μ0\le\beta\le\frac{1}{2\sqrt\mu}0≤β≤2μ​1​ and s≤β\sqrt s\le\betas​≤β. Then every sequence generated by (IPAHD-SC) satisfies, for every k≥1k\ge1k≥1,

μ2∥xk−x⋆∥2≤f(xk)−min⁡Hf≤E1qk−1,\frac\mu2\|x_k-x^\star\|^2\le f(x_k)-\min_H f\le E_1q^{k-1},2μ​∥xk​−x⋆∥2≤f(xk​)−Hmin​f≤E1​qk−1,

and

θk∑j=0k−2θ−j∥∇f(xj)∥2=O(qk)(k→+∞).\theta^k\sum_{j=0}^{k-2}\theta^{-j}\|\nabla f(x_j)\|^2=\mathcal O(q^k)\qquad(k\to+\infty).θkj=0∑k−2​θ−j∥∇f(xj​)∥2=O(qk)(k→+∞).

Milestones

The milestone targets are the paper's displayed intermediate claims, in order:

  1. the equivalent second-order form (20) of the algorithm;
  2. the increment of the auxiliary vector vk=μ(xk−x⋆)+1s(xk−xk−1)+β∇f(xk)v_k=\sqrt\mu(x_k-x^\star)+\frac{1}{\sqrt s}(x_k-x_{k-1})+\beta\nabla f(x_k)vk​=μ​(xk​−x⋆)+s​1​(xk​−xk−1​)+β∇f(xk​);
  3. the two "elementary algebra" quadratic-form inequalities, Term 1 and Term 2;
  4. the one-step inequality 1s(Ek+1−Ek)+12μEk+1≤0\frac{1}{\sqrt s}(E_{k+1}-E_k)+\frac12\sqrt\mu E_{k+1}\le0s​1​(Ek+1​−Ek​)+21​μ​Ek+1​≤0 for Ek=f(xk)−f(x⋆)+12∥vk∥2E_k=f(x_k)-f(x^\star)+\frac12\|v_k\|^2Ek​=f(xk​)−f(x⋆)+21​∥vk​∥2;
  5. the energy decay (21), Ek≤E1qk−1E_k\le E_1q^{k-1}Ek​≤E1​qk−1;
  6. the recursive inequality (22) for Zk=2β(f(xk)−f(x⋆))+μ∥xk−x⋆∥2Z_k=2\beta(f(x_k)-f(x^\star))+\sqrt\mu\|x_k-x^\star\|^2Zk​=2β(f(xk​)−f(x⋆))+μ​∥xk​−x⋆∥2;
  7. the discounted gradient-sum bound (24).

Significance

Theorem 9 gives linear convergence of a proximal algorithm for a smooth strongly convex objective with no Lipschitz assumption on ∇f\nabla f∇f and no upper bound on the step in terms of a smoothness constant: the step condition s≤β≤12μ\sqrt s\le\beta\le\frac1{2\sqrt\mu}s​≤β≤2μ​1​ involves only the strong convexity modulus. It also gives a geometric rate for a weighted sum of squared gradients, which the authors present as new for proximal algorithms of this type. In §5.1.2 the same estimate, applied to the Moreau envelope, gives linear convergence for nonsmooth strongly convex objectives (Theorem 10), and §5.2 shows the explicit gradient counterpart (Theorem 11).

The result is proved in the paper. A formal development would certify the exact constants (qqq, θ\thetaθ, and the factor 4E1/μ4E_1/\sqrt\mu4E1​/μ​ in (24)) and the index bookkeeping of the gradient sums, where the printed proof contains small slips. It would also provide reusable proximal optimality and strong convexity results for later formalizations.

Difficulty

The continuous-time estimate of Theorem 7 does not transfer term by term to the discrete energy EkE_kEk​. Its difference contains cross terms such as βμ⟨∇f(xk+1),xk+1−x⋆⟩\beta\mu\langle\nabla f(x_{k+1}),x_{k+1}-x^\star\rangleβμ⟨∇f(xk+1​),xk+1​−x⋆⟩ and μ⟨∇f(xk+1),xk+1−xk⟩\sqrt\mu\langle\nabla f(x_{k+1}),x_{k+1}-x_k\rangleμ​⟨∇f(xk+1​),xk+1​−xk​⟩, whose signs are not automatic. The upper bound on β\betaβ and the lower bound on s\sqrt ss​ must both survive the resulting estimates. The gradient conclusion introduces a separate weighted sum, with different index ranges in Theorem 9 and the final displayed line of its proof. The algorithm begins at k=1k=1k=1 and uses two free initial points, x0x_0x0​ and x1x_1x1​.

Formalization scope

The Lean development works on a real Hilbert space H (NormedAddCommGroup, InnerProductSpace ℝ, CompleteSpace), with ∇f\nabla f∇f Mathlib's gradient f. Conventions:

  • Hypotheses. fff is ConvexOn ℝ Set.univ f and ContDiff ℝ 1 f, and μ\muμ-strongly convex in the literal sense of Definition 1 (HessianDamping.DINSC.IsStronglyConvex, convexity of f−μ2∥⋅∥2f-\frac\mu2\|\cdot\|^2f−2μ​∥⋅∥2), with 0<μ0<\mu0<μ. The standing assumption argmin⁡f≠∅\operatorname{argmin}f\neq\emptysetargminf=∅ is a point x⋆x^\starx⋆ with f(x⋆)≤f(y)f(x^\star)\le f(y)f(x⋆)≤f(y) for every yyy, so min⁡Hf\min_H fminH​f is f(x⋆)f(x^\star)f(x⋆). The step sss is positive, as the page implies (s=h2s=h^2s=h2, h>0h>0h>0). The parameter hypotheses are 0≤β≤12μ0\le\beta\le\frac1{2\sqrt\mu}0≤β≤2μ​1​ and s≤β\sqrt s\le\betas​≤β, as printed.
  • Algorithm. The proximal step is the published predicate GoldenRatioVI.Shared.IsProxPoint: xk+1x_{k+1}xk+1​ minimizes z↦γf(z)+12∥z−yk∥2z\mapsto\gamma f(z)+\frac12\|z-y_k\|^2z↦γf(z)+21​∥z−yk​∥2. No proximal function is defined. A run imposes the step for every k≥1k\ge1k≥1; x0x_0x0​ and x1x_1x1​ are free.
  • Rates and sums. qqq and θ\thetaθ are written with Real.sqrt (μ * s). θ−j\theta^{-j}θ−j is an integer power. ∑j=0k−2\sum_{j=0}^{k-2}∑j=0k−2​ is a sum over Finset.range (k - 1). O(qk)\mathcal O(q^k)O(qk) is =O[Filter.atTop] with the constant allowed to depend on all the data. The side claims 0<q<10<q<10<q<1 and 0<θ<10<\theta<10<θ<1 are a conjunct of the goal.
  • Not trivial. The goal does not assume the energy decay, and it does not state the result for a single parameter choice or a vacuous hypothesis set: the hypotheses hold, for example, for f=12∥⋅∥2f=\frac12\|\cdot\|^2f=21​∥⋅∥2, μ=1\mu=1μ=1, s=116s=\frac1{16}s=161​, β=14\beta=\frac14β=41​. The goal also does not mention vkv_kvk​, EkE_kEk​ or ZkZ_kZk​; only the printed constant E1E_1E1​ appears.

Infrastructure needed: the first-order optimality condition of a proximal step for a differentiable function, and the first-order characterization of strong convexity, f(y)≥f(x)+⟨∇f(x),y−x⟩+μ2∥y−x∥2f(y)\ge f(x)+\langle\nabla f(x),y-x\rangle+\frac\mu2\|y-x\|^2f(y)≥f(x)+⟨∇f(x),y−x⟩+2μ​∥y−x∥2, from Definition 1. Both are reusable well beyond this mission, as is the iteration of linear recursive inequalities ak≤qak−1+bka_k\le qa_{k-1}+b_kak​≤qak−1​+bk​. Contributions of either kind, and proofs of the individual milestones, are welcome.

Selected references

  • H. Attouch, Z. Chbani, J. Fadili, H. Riahi, First-order optimization algorithms via inertial systems with Hessian driven damping, Mathematical Programming, 2020; preprint arXiv:1907.10536v2. https://arxiv.org/abs/1907.10536
  • H. Attouch, J. Peypouquet, P. Redont, Fast convex minimization via inertial dynamics with Hessian driven damping, Journal of Differential Equations 261(10) (2016), 5734–5783. https://doi.org/10.1016/j.jde.2016.08.020
  • B. T. Polyak, Some methods of speeding up the convergence of iteration methods, USSR Computational Mathematics and Mathematical Physics 4 (1964), 1–17. https://doi.org/10.1016/0041-5553(64)90137-5
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Optimization·Captain: mikedeng1

The Direct Extension of ADMM for Multi-block Convex Minimization Problems is Not Necessarily Convergent I: When A₁ᵀA₃ = 0 the Extended ADMM Is Contractive and Converges to a KKT PointResearch Paper

Motivation

The alternating direction method of multipliers (ADMM) solves a constrained optimization problem by minimizing an augmented Lagrangian over one block of variables at a time and then updating a multiplier. Its two-block version had established convergence results. Applying the same cycle to three or more blocks was natural in models whose objective separates into several terms, but its convergence was unresolved when Chen, He, Ye and Yuan wrote this paper. Their analysis gives both a sufficient condition for convergence and, elsewhere in the paper, a counterexample to unrestricted convergence. This mission concerns the sufficient condition: the first and third constraint matrices are orthogonal in the sense A1TA3=0A_1^{T}A_3=0A1T​A3​=0. Chen, He, Ye and Yuan (2014)

The condition matters because the third block is separated from the first in the quadratic part of the augmented Lagrangian, while the middle block still participates in both updates. The result therefore covers a genuine three-block algorithm. It identifies what the direct cyclic extension can guarantee under this structure. The companion result gives an ergodic rate for averages of auxiliary iterates, from any starting point.

Setting

The three-block problem has variables xi∈Xi⊆Rnix_i\in\mathcal X_i\subseteq\mathbb R^{n_i}xi​∈Xi​⊆Rni​, matrices Ai∈Rp×niA_i\in\mathbb R^{p\times n_i}Ai​∈Rp×ni​, and a vector b∈Rpb\in\mathbb R^pb∈Rp:

min⁡xi∈Xi  θ1(x1)+θ2(x2)+θ3(x3)subject toA1x1+A2x2+A3x3=b.\min_{x_i\in\mathcal X_i}\;\theta_1(x_1)+\theta_2(x_2)+\theta_3(x_3) \quad\text{subject to}\quad A_1x_1+A_2x_2+A_3x_3=b.xi​∈Xi​min​θ1​(x1​)+θ2​(x2​)+θ3​(x3​)subject toA1​x1​+A2​x2​+A3​x3​=b.

Each Xi\mathcal X_iXi​ is closed and convex, each θi:Rni→R\theta_i:\mathbb R^{n_i}\to\mathbb Rθi​:Rni​→R is convex, and the primal solution set is nonempty. For β>0\beta>0β>0, write r=A1x1+A2x2+A3x3−br=A_1x_1+A_2x_2+A_3x_3-br=A1​x1​+A2​x2​+A3​x3​−b. The augmented Lagrangian is Lβ=∑iθi(xi)−λTr+(β/2)∥r∥22\mathcal L_\beta=\sum_i\theta_i(x_i)-\lambda^Tr+(\beta/2)\|r\|_2^2Lβ​=∑i​θi​(xi​)−λTr+(β/2)∥r∥22​. The minus sign in front of λTr\lambda^TrλTr fixes the sign of the multiplier step λk+1=λk−β(A1x1k+A2x2k+1+A3x3k+1−b)\lambda^{k+1}=\lambda^k-\beta(A_1x_1^k+A_2x_2^{k+1}+A_3x_3^{k+1}-b)λk+1=λk−β(A1​x1k​+A2​x2k+1​+A3​x3k+1​−b) of (2.4c).

The paper analyzes a reordered cycle, numbered (2.4): minimize in x2x_2x2​, minimize in x3x_3x3​, update λ\lambdaλ, then minimize in x1x_1x1​. The input state is (x1k,x3k,λk)(x_1^k,x_3^k,\lambda^k)(x1k​,x3k​,λk); x2kx_2^kx2k​ is an intermediate variable. Each minimization may choose any minimizer. The reordered cycle is the cyclic direct extension with x1x_1x1​ shifted by one index. A run is any sequence satisfying all four update conditions. Chen et al., pp. 4–5

Let w=(x1,x2,x3,λ)w=(x_1,x_2,x_3,\lambda)w=(x1​,x2​,x3​,λ), Ω=X1×X2×X3×Rp\Omega=\mathcal X_1\times\mathcal X_2\times\mathcal X_3\times\mathbb R^pΩ=X1​×X2​×X3​×Rp, and θ(w)=∑iθi(xi)\theta(w)=\sum_i\theta_i(x_i)θ(w)=∑i​θi​(xi​). The affine map F(w)F(w)F(w) has blocks (−A1Tλ,−A2Tλ,−A3Tλ,r)(-A_1^T\lambda,-A_2^T\lambda,-A_3^T\lambda,r)(−A1T​λ,−A2T​λ,−A3T​λ,r). The variational inequality solution set Ω∗\Omega^*Ω∗ consists of w∗∈Ωw^*\in\Omegaw∗∈Ω for which θ(w)−θ(w∗)+(w−w∗)TF(w∗)≥0\theta(w)-\theta(w^*)+(w-w^*)^TF(w^*)\ge0θ(w)−θ(w∗)+(w−w∗)TF(w∗)≥0 for every w∈Ωw\in\Omegaw∈Ω. Such points are the KKT points used in this mission. The paper employs Ω\OmegaΩ and Ω∗\Omega^*Ω∗ without defining them; these definitions fix their intended meaning.

Formalization targets

Contraction and convergence

Let vk=(x1k,x3k,λk)v^k=(x_1^k,x_3^k,\lambda^k)vk=(x1k​,x3k​,λk), and let v∗v^*v∗ be the corresponding projection of w∗∈Ω∗w^*\in\Omega^*w∗∈Ω∗. With HHH the positive semidefinite block matrix in equation (2.11), the main target is Theorem 2.4:

∥vk+1−v∗∥H2≤∥vk−v∗∥H2−∥vk−vk+1∥H2(k≥1).\|v^{k+1}-v^*\|_H^2\le \|v^k-v^*\|_H^2-\|v^k-v^{k+1}\|_H^2 \qquad(k\ge1).∥vk+1−v∗∥H2​≤∥vk−v∗∥H2​−∥vk−vk+1∥H2​(k≥1).

If [A1,A2][A_1,A_2][A1​,A2​] and A3A_3A3​ have full column rank and Ω∗≠∅\Omega^*\ne\varnothingΩ∗=∅, the entire sequence wkw^kwk converges to a point of Ω∗\Omega^*Ω∗. The milestone list follows the paper's affine monotonicity statement, Lemmas 2.1–2.3, the displayed contraction, the summability and vanishing correction terms, and the cluster-point variational inequality. Chen et al., pp. 5–9

Ergodic companion

Theorem 2.5 bounds a gap at the average wˉt=(t+1)−1∑k=0tw~k\bar w_t=(t+1)^{-1}\sum_{k=0}^t\tilde w^kwˉt​=(t+1)−1∑k=0t​w~k, where w~k\tilde w^kw~k is the auxiliary point of (2.13). For every w∈Ωw\in\Omegaw∈Ω, the target is

θ(wˉt)−θ(w)+(wˉt−w)TF(w)≤∥v−v0∥H22(t+1).\theta(\bar w_t)-\theta(w)+(\bar w_t-w)^TF(w) \le\frac{\|v-v^0\|_H^2}{2(t+1)}.θ(wˉt​)−θ(w)+(wˉt​−w)TF(w)≤2(t+1)∥v−v0∥H2​​.

This companion is stated, as on the page, for an arbitrary starting point. Chen et al., p. 9

Significance

The contraction gives a quantitative decrease relative to any variational inequality solution, even though HHH is only semidefinite. Combined with the rank assumptions, it yields convergence of all primal blocks and the multiplier to a KKT point. The auxiliary average gives a finite-iteration gap bound with an explicit 1/(t+1)1/(t+1)1/(t+1) coefficient. These statements locate a useful structural regime inside a method that the same paper shows can diverge without additional conditions.

The formal development records the whole update cycle, the variational inequality, and the two block operators QQQ and HHH. It leaves the named theorems as proof targets; compiling their statements does not claim a machine-checked proof. The definitions and intermediate inequalities can be reused when formalizing other cyclic splitting schemes or comparing this one with two-block ADMM.

Difficulty

The familiar two-block ADMM convergence argument cannot simply be applied to a three-block cycle: the middle iterate is updated between the first and third blocks, and the multiplier update sits before the next first-block minimization. The resulting one-step inequality contains a correction involving the previous and next essential states. Even after that correction is controlled, HHH is semidefinite, so contraction in its quadratic form alone does not imply convergence of every coordinate. The full column rank conditions provide the additional control demanded by the paper's conclusion.

Formalization scope

Vectors are functions on Fin n; matrices are Mathlib matrices. Every occurrence of a squared Euclidean norm in the paper is represented by a dot product or the expanded HHH quadratic form. Mathlib's default norm on a function vector is a sup norm, so it is not used for those squares. The topology in the final convergence statement is the product topology on the four vector blocks. The block labels 1,2,31,2,31,2,3 in the paper correspond to separate fields in Lean. The initial x20x_2^0x20​ is unused by the run predicate. A zero-dimensional block is allowed when the stated conditions still make sense.

There are disclosed repairs to the printed text. Lemma 2.3 and the contraction are restricted to k≥1k\ge1k≥1: their derivation uses the preceding x3x_3x3​ optimality condition, which an arbitrary initial point need not satisfy. The convergence part additionally assumes Ω∗≠∅\Omega^*\ne\varnothingΩ∗=∅, since the paper assumes a primal optimizer but supplies no constraint qualification guaranteeing a KKT point. Lemma 2.2's displayed wk+1w^{k+1}wk+1 uses x1kx_1^kx1k​, while its inequality and the run use x1k+1x_1^{k+1}x1k+1​; Lean uses the latter. Theorem 2.5's verbal assertion that w~∈W\tilde w\in\mathcal Ww~∈W is represented as the indexed average wˉt∈Ω\bar w_t\in\Omegawˉt​∈Ω.

The convex objectives are real valued on all of Rni\mathbb R^{n_i}Rni​, as on p. 1. Such a convex function is continuous, so the paper's word “closed” adds no extra condition here. Runs quantify over actual minimizers and are not constructed by a default-valued argmin; this prevents an empty subproblem from creating a fictitious iterate. A complete proof can contribute the convex first-order conditions, matrix identities, summability argument and finite-dimensional convergence steps. The reusable interfaces are the three-block problem, run, variational inequality and block quadratic forms.

Selected references

  • Caihua Chen, Bingsheng He, Yinyu Ye and Xiaoming Yuan, The direct extension of ADMM for multi-block convex minimization problems is not necessarily convergent, Mathematical Programming, 2014. DOI: 10.1007/s10107-014-0826-5.
  • Stephen Boyd, Neal Parikh, Eric Chu, Borja Peleato and Jonathan Eckstein, Distributed Optimization and Statistical Learning via the Alternating Direction Method of Multipliers, Foundations and Trends in Machine Learning 3, 2011. DOI: 10.1561/2200000016.
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Numerical AnalysisOptimization·Captain: mikedeng1

From Error Bounds to the Complexity of First-Order Descent Methods for Convex Functions 3: ISTA for ℓ1-Regularized Least Squares Satisfies f(x_k) − min f ≤ (f(x_0) − min f)/q^k with q = 1 + 2aγ_R/b²Research Paper

Motivation

The ℓ1-regularized least squares problem (the Lasso, or basis pursuit denoising) is the model problem of compressed sensing and sparse inverse problems: given a matrix A∈Rm×nA\in\mathbb R^{m\times n}A∈Rm×n, data d∈Rmd\in\mathbb R^md∈Rm and a weight μ>0\mu>0μ>0, one seeks a vector xxx that fits Ax≈dAx\approx dAx≈d while having few nonzero entries. The standard first-order method for it is the iterative shrinkage thresholding algorithm (ISTA), a forward-backward splitting scheme whose backward step is componentwise soft thresholding. Each iteration costs two matrix–vector products, which is why ISTA and its variants are used on problems far too large for interior-point methods.

The classical complexity guarantee for ISTA is f(xk)−min⁡f=O(1/k)f(x_k)-\min f=O(1/k)f(xk​)−minf=O(1/k), the rate of the proximal gradient method on any convex composite problem (Beck–Teboulle 2009). ISTA itself goes back to Daubechies–Defrise–De Mol 2004, and its link with forward-backward splitting to Combettes–Wajs 2005. An asymptotic linear rate was known, with an explanation through partial smoothness (Liang–Fadili–Peyré), but there was no global, explicit, non-asymptotic bound. Bolte, Nguyen, Peypouquet and Suter (arXiv:1510.08234v3, Math. Program. 2017) derive such a bound from two ingredients: an error bound for the Lasso objective on ℓ1\ell_1ℓ1​ balls, with a constant written through a Hoffman constant, and their general theory turning a Kurdyka–Łojasiewicz (KL) inequality into complexity bounds for descent methods.

Setting

Write Rn\mathbb R^nRn with the Euclidean norm ∥⋅∥\|\cdot\|∥⋅∥, and ∥x∥1=∑i∣xi∣\|x\|_1=\sum_i|x_i|∥x∥1​=∑i​∣xi​∣. For a matrix MMM, ∥M∥\|M\|∥M∥ is its spectral norm, the operator norm from Rn\mathbb R^nRn to Rm\mathbb R^mRm with Euclidean norms. The objective is

f(x)=μ∥x∥1+12∥Ax−d∥2,μ>0,f(x)=\mu\|x\|_1+\tfrac12\|Ax-d\|^2,\qquad \mu>0,f(x)=μ∥x∥1​+21​∥Ax−d∥2,μ>0,

with min⁡f=inf⁡xf(x)\min f=\inf_x f(x)minf=infx​f(x) and S=argmin⁡fS=\operatorname{argmin} fS=argminf. Put g=μ∥⋅∥1g=\mu\|\cdot\|_1g=μ∥⋅∥1​ and h=12∥A⋅−d∥2h=\tfrac12\|A\cdot-d\|^2h=21​∥A⋅−d∥2. Then hhh is convex with gradient AT(Ax−d)A^T(Ax-d)AT(Ax−d), Lipschitz with constant L=∥ATA∥L=\|A^TA\|L=∥ATA∥.

Given stepsizes 0<λ−≤λk≤λ+0<\lambda^-\le\lambda_k\le\lambda^+0<λ−≤λk​≤λ+ with λ+L<2\lambda^+L<2λ+L<2 and any x0x_0x0​, ISTA is

xk+1=prox⁡λkμ∥⋅∥1(xk−λk(ATAxk−ATd)),k≥0,x_{k+1}=\operatorname{prox}_{\lambda_k\mu\|\cdot\|_1}\big(x_k-\lambda_k(A^TAx_k-A^Td)\big),\qquad k\ge0,xk+1​=proxλk​μ∥⋅∥1​​(xk​−λk​(ATAxk​−ATd)),k≥0,

where prox⁡φ(v)\operatorname{prox}_\varphi(v)proxφ​(v) is the minimizer of φ(y)+12∥y−v∥2\varphi(y)+\tfrac12\|y-v\|^2φ(y)+21​∥y−v∥2. More generally, in a real Hilbert space HHH with ggg proper, lower semicontinuous and convex and hhh convex with LLL-Lipschitz gradient, the forward-backward method takes xk+1x_{k+1}xk+1​ to be a minimizer of g(z)+⟨∇h(xk),z−xk⟩+12λk∥z−xk∥2g(z)+\langle\nabla h(x_k),z-x_k\rangle+\frac1{2\lambda_k}\|z-x_k\|^2g(z)+⟨∇h(xk​),z−xk​⟩+2λk​1​∥z−xk​∥2.

A sequence is a subgradient descent sequence for a convex fff with constants a,b>0a,b>0a,b>0 if x0∈dom⁡fx_0\in\operatorname{dom} fx0​∈domf and, for every k≥1k\ge1k≥1,

  • (H1) f(xk)+a∥xk−xk−1∥2≤f(xk−1)f(x_k)+a\|x_k-x_{k-1}\|^2\le f(x_{k-1})f(xk​)+a∥xk​−xk−1​∥2≤f(xk−1​);
  • (H2) some ωk∈∂f(xk)\omega_k\in\partial f(x_k)ωk​∈∂f(xk​) has ∥ωk∥≤b∥xk−xk−1∥\|\omega_k\|\le b\|x_k-x_{k-1}\|∥ωk​∥≤b∥xk​−xk−1​∥.

With min⁡f=0\min f=0minf=0, fff has the KL property on a set X∩[0<f<rˉ]X\cap[0<f<\bar r]X∩[0<f<rˉ] with desingularizing function φ\varphiφ if φ′(f(x))∥v∥≥1\varphi'(f(x))\|v\|\ge1φ′(f(x))∥v∥≥1 for every such xxx and every v∈∂f(x)v\in\partial f(x)v∈∂f(x).

A number ν≥0\nu\ge0ν≥0 is a Hoffman constant for a pair of matrices (A′,E)(A',E)(A′,E) if, for every right-hand side with X={A′x≤a′}X=\{A'x\le a'\}X={A′x≤a′} and Y={Ex=e}Y=\{Ex=e\}Y={Ex=e} intersecting, dist⁡(x,X∩Y)≤ν∥Ex−e∥\operatorname{dist}(x,X\cap Y)\le\nu\|Ex-e\|dist(x,X∩Y)≤ν∥Ex−e∥ for all x∈Xx\in Xx∈X.

Formalization targets

Goal: Theorem 25

Put a=1λ+−L2a=\frac1{\lambda^+}-\frac L2a=λ+1​−2L​ and b=1λ−+Lb=\frac1{\lambda^-}+Lb=λ−1​+L, and R=max⁡(f(x0)μ,1+∥d∥22μ)R=\max\big(\frac{f(x_0)}\mu,1+\frac{\|d\|^2}{2\mu}\big)R=max(μf(x0​)​,1+2μ∥d∥2​). Let γR>0\gamma_R>0γR​>0 be such that f(x)−min⁡f≥2γRdist⁡2(x,S)f(x)-\min f\ge2\gamma_R\operatorname{dist}^2(x,S)f(x)−minf≥2γR​dist2(x,S) whenever ∥x∥1≤R\|x\|_1\le R∥x∥1​≤R. Then ISTA converges to some x∗∈Sx^*\in Sx∗∈S and

f(xk)−min⁡f≤f(x0)−min⁡fqk(k≥0),∥xk−x∗∥≤C f(x0)−min⁡fq(k−1)/2(k≥1),f(x_k)-\min f\le\frac{f(x_0)-\min f}{q^k}\quad(k\ge0),\qquad \|x_k-x^*\|\le C\,\frac{\sqrt{f(x_0)-\min f}}{q^{(k-1)/2}}\quad(k\ge1),f(xk​)−minf≤qkf(x0​)−minf​(k≥0),∥xk​−x∗∥≤Cq(k−1)/2f(x0​)−minf​​(k≥1), q=1+2aγRb2,C=1a(1+1ab−2γR1+12ab−2γR).q=1+\frac{2a\gamma_R}{b^2},\qquad C=\frac1{\sqrt a}\Bigg(1+\frac1{ab^{-2}\gamma_R\sqrt{1+\frac1{2ab^{-2}\gamma_R}}}\Bigg).q=1+b22aγR​​,C=a​1​(1+ab−2γR​1+2ab−2γR​1​​1​).

Milestones

  1. Lemma 10, (9)–(10): for R>∥d∥2/(2μ)R>\|d\|^2/(2\mu)R>∥d∥2/(2μ) the error bound holds with γR=1/(4ν2(1+μR+(R∥A∥+∥d∥)(4R∥A∥+∥d∥)))\gamma_R=1/\big(4\nu^2(1+\mu R+(R\|A\|+\|d\|)(4R\|A\|+\|d\|))\big)γR​=1/(4ν2(1+μR+(R∥A∥+∥d∥)(4R∥A∥+∥d∥))). Here ν\nuν is a Hoffman constant of an explicit pair of matrices built from AAA and μ\muμ.
  2. Lemma 10, KL consequence: under the error bound, f−min⁡ff-\min ff−minf has the KL property on the ℓ1\ell_1ℓ1​ ball with φ(s)=2s/γR\varphi(s)=\sqrt{2s/\gamma_R}φ(s)=2s/γR​​.
  3. Proposition 13: the forward-backward method satisfies (H1) and (H2) with the constants a,ba,ba,b above.
  4. §5.3: every ISTA iterate satisfies ∥xk∥1≤R\|x_k\|_1\le R∥xk​∥1​≤R.
  5. Corollary 20 in the stable-set form of Corollary 19: a subgradient descent sequence that stays in a set XXX, on which the KL inequality holds with ψ(s)=ℓ2s2\psi(s)=\frac\ell2s^2ψ(s)=2ℓ​s2, satisfies f(xk)≤f(x0)/(1+2aσ)kf(x_k)\le f(x_0)/(1+2a\sigma)^kf(xk​)≤f(x0​)/(1+2aσ)k and the companion bound on ∥xk−x∗∥\|x_k-x^*\|∥xk​−x∗∥, σ=ℓb−2\sigma=\ell b^{-2}σ=ℓb−2.

Significance

The result. The theorem replaces the sublinear O(1/k)O(1/k)O(1/k) guarantee of ISTA by a global linear rate with explicit constants depending only on μ\muμ, AAA, ddd, the stepsizes, x0x_0x0​ and a Hoffman constant. It also bounds the distance of the iterates to the limit, not only the objective gap, and needs no uniqueness of the minimizer. Through γR\gamma_RγR​, it shows that conditioning of the objective near its minimizers, rather than strong convexity, governs the complexity of the method. The general machinery behind it (Theorem 16 of the paper, a separate mission of this series) applies to any method producing subgradient descent sequences.

Formalizing it. The result is proved on paper, and no machine-checked proof of it or of its ingredients is known. A formalization would give a verified linear-rate certificate for a widely deployed algorithm. It would also yield reusable lemmas: the descent and relative-error properties of the forward-backward method in a Hilbert space, and quadratic growth for the Lasso on ℓ1\ell_1ℓ1​ balls. Lemma 10 rests on an external result (Beck–Shtern, Lemma 2.5) that a complete development must also formalize.

Difficulty

The Lasso objective is not strongly convex when AAA has a nontrivial kernel, and its minimizer need not be unique. The textbook argument for linear convergence of proximal gradient methods, which uses strong convexity, therefore does not apply. Quadratic growth f−min⁡f≥2γdist⁡2(⋅,S)f-\min f\ge2\gamma\operatorname{dist}^2(\cdot,S)f−minf≥2γdist2(⋅,S) is the substitute, but it holds only on bounded sets, with a constant degrading in the radius. The analysis must therefore show that the iterates stay in a fixed ℓ1\ell_1ℓ1​ ball and keep track of how the growth constant enters the rate. Deriving the explicit γR\gamma_RγR​ requires recasting the problem as a quadratic program over a polyhedron with 2n+12^n+12n+1 facets and invoking a Hoffman-type error bound for it.

Formalization scope

Citations refer to the arXiv preprint arXiv:1510.08234v3 (20 July 2016), with its numbering and pages; the journal version is not used. Rn\mathbb R^nRn is EuclideanSpace ℝ (Fin n) and matrices act through Matrix.toEuclideanLin. Spectral norms are operator norms of the associated continuous linear maps, never Mathlib's default entrywise matrix norm. The data vector, called bbb in §3.2.1 of the paper and ddd in §5.3, is ddd throughout; bbb is the constant of (H2).

Functions with values in (−∞,+∞](-\infty,+\infty](−∞,+∞] are EReal-valued. The convex subdifferential, Γ₀, ∥⋅∥1\|\cdot\|_1∥⋅∥1​, the prox predicate and the class K(0,rˉ)\mathcal K(0,\bar r)K(0,rˉ) of desingularizing functions are reused from published platform definitions. The stepsize condition λ+<2/L\lambda^+<2/Lλ+<2/L is written λ+L<2\lambda^+L<2λ+L<2, so that A=0A=0A=0 (where L=0L=0L=0) is covered. min⁡f\min fminf is the infimum of fff, and q(k−1)/2q^{(k-1)/2}q(k−1)/2 is a real power.

In the goal, γR\gamma_RγR​ is any positive constant satisfying the error bound on the ball of radius RRR; it is not fixed to the value (10) and not existentially quantified. The constants a,b,q,C,Ra,b,q,C,Ra,b,q,C,R are fixed formulas, never existentials. A statement with an unspecified constant, with γR\gamma_RγR​ chosen after the sequence, or with the stepsize hypothesis written as λ+<2/L\lambda^+<2/Lλ+<2/L (unsatisfiable or vacuous at L=0L=0L=0) would trivialize the goal and is ruled out.

The subgradient-descent and KL notions duplicate, in the sub-namespace ErrBoundCplx.ISTA, those of the series' first mission, because draft items cannot import each other. Proofs of any milestone are welcome, in particular Proposition 13 and the KL consequence of Lemma 10, which are self-contained. A formalization of Hoffman's error bound and of Beck–Shtern's Lemma 2.5 is the main infrastructure Lemma 10 needs.

Selected references

  • J. Bolte, T. P. Nguyen, J. Peypouquet, B. W. Suter, From error bounds to the complexity of first-order descent methods for convex functions, Math. Program. 165 (2017) 471–507; arXiv:1510.08234v3. https://arxiv.org/abs/1510.08234v3
  • A. Beck, S. Shtern, Linearly convergent away-step conditional gradient for non-strongly convex functions, preprint (cited as [10], Lemma 2.5). https://arxiv.org/abs/1504.05002
  • A. Beck, M. Teboulle, A fast iterative shrinkage-thresholding algorithm for linear inverse problems, SIAM J. Imaging Sci. 2 (2009) 183–202. https://doi.org/10.1137/080716542
  • A. J. Hoffman, On approximate solutions of systems of linear inequalities, J. Res. Natl. Bur. Stand. 49 (1952) 263–265. https://doi.org/10.6028/jres.049.027
  • I. Daubechies, M. Defrise, C. De Mol, An iterative thresholding algorithm for linear inverse problems with a sparsity constraint, Comm. Pure Appl. Math. 57 (2004) 1413–1457. https://doi.org/10.1002/cpa.20042
  • J. Liang, J. Fadili, G. Peyré, Local linear convergence of forward-backward under partial smoothness, preprint. https://arxiv.org/abs/1407.5611
  • P. L. Combettes, V. R. Wajs, Signal recovery by proximal forward-backward splitting, Multiscale Model. Simul. 4 (2005) 1168–1200. https://doi.org/10.1137/050626090
  • H. Attouch, J. Bolte, B. F. Svaiter, Convergence of descent methods for semi-algebraic and tame problems, Math. Program. 137 (2013) 91–129. https://doi.org/10.1007/s10107-011-0484-9
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