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Convex OptimizationNumerical AnalysisOperations Research+1·Captain: Shuze Chen

Lectures on Modern Convex Optimization X: Complexity of the Ellipsoid MethodTextbook

Motivation

A convex program whose objective and feasible set are known only through oracles, routines that answer queries about one point at a time, can still be solved to any prescribed accuracy with a number of queries bounded in advance. The ellipsoid method is the classical algorithm that achieves this. It was introduced for convex minimization by Yudin and Nemirovski (Ekonomika i Matematicheskie Metody, 1976) and by Shor (Cybernetics, 1977), and it became widely known when Khachiyan used it to prove that linear programming is solvable in polynomial time (Soviet Math. Dokl., 1979). Grötschel, Lovász and Schrijver turned the method into a general tool of combinatorial optimization, the equivalence of separation and optimization (Springer, 1988).

Ben-Tal and Nemirovski's Lectures on Modern Convex Optimization (SIAM 2001) present the method in §5.2 as the engine of their theorem that convex programs are polynomially solvable, and prove an explicit, fully quantified complexity bound for it, Theorem 5.2.1. This mission is the tenth of a series formalizing the book's main results and covers §5.2 (pp. 342–352).

Setting

Vectors are elements of Rn\mathbb R^nRn, n≥2n \ge 2n≥2, with the Euclidean norm ∥x∥2=xTx\|x\|_2 = \sqrt{x^Tx}∥x∥2​=xTx​. The problem is

min⁡x{f(x):x∈X⊂Rn}(5.2.9)\min_x\{f(x) : x \in X \subset \mathbb R^n\} \tag{5.2.9}xmin​{f(x):x∈X⊂Rn}(5.2.9)

where f:Rn→Rf : \mathbb R^n \to \mathbb Rf:Rn→R is convex and XXX is a closed, bounded, convex set with nonempty interior. Two radii r,R>0r, R > 0r,R>0 are known in advance (assumption A): XXX lies in the ball E0={x∣∥x∥2≤R}E_0 = \{x \mid \|x\|_2 \le R\}E0​={x∣∥x∥2​≤R} and contains some ball {x∣∥x−xˉ∥2≤r}\{x \mid \|x - \bar x\|_2 \le r\}{x∣∥x−xˉ∥2​≤r}, whose centre xˉ\bar xxˉ is not known.

The data are accessed through two oracles. A separation oracle for XXX answers a query xxx by "x∈Xx \in Xx∈X" when that holds, and otherwise returns a vector a≠0a \ne 0a=0 with aTx≥aTya^Tx \ge a^TyaTx≥aTy for all y∈Xy \in Xy∈X. A first order oracle for fff returns f(x)f(x)f(x) and a subgradient η\etaη of fff at xxx: f(y)≥f(x)+ηT(y−x)f(y) \ge f(x) + \eta^T(y - x)f(y)≥f(x)+ηT(y−x) for all yyy.

An ellipsoid is E(c,B)={c+Bu∣uTu≤1}E(c, B) = \{c + Bu \mid u^Tu \le 1\}E(c,B)={c+Bu∣uTu≤1} with Det⁡B≠0\operatorname{Det} B \ne 0DetB=0. For a≠0a \ne 0a=0, put p=BTa/aTBBTap = B^Ta/\sqrt{a^TBB^Ta}p=BTa/aTBBTa​ and

c+=c−1n+1Bp,B+=nn2−1B+(nn+1−nn2−1)(Bp)pT.c^+ = c - \frac{1}{n+1}Bp,\qquad B^+ = \frac{n}{\sqrt{n^2-1}}B + \Big(\frac{n}{n+1} - \frac{n}{\sqrt{n^2-1}}\Big)(Bp)p^T .c+=c−n+11​Bp,B+=n2−1​n​B+(n+1n​−n2−1​n​)(Bp)pT.

The ellipsoid method with accuracy ϵ>0\epsilon > 0ϵ>0 starts from c0=0c_0 = 0c0​=0, B0=RIB_0 = RIB0​=RI, L0=0L_0 = 0L0​=0. At step t=1,2,…t = 1, 2, \dotst=1,2,… it queries the separation oracle at ct−1c_{t-1}ct−1​. If a separator aaa is returned, the step is nonproductive, at=aa_t = aat​=a and Lt=Lt−1L_t = L_{t-1}Lt​=Lt−1​. Otherwise the step is productive: the first order oracle is queried at ct−1c_{t-1}ct−1​; a zero subgradient stops the method with result ct−1c_{t-1}ct−1​; a nonzero one becomes ata_tat​, and Lt=max⁡{Lt−1,R∥at∥2−atTct−1}L_t = \max\{L_{t-1}, R\|a_t\|_2 - a_t^Tc_{t-1}\}Lt​=max{Lt−1​,R∥at​∥2​−atT​ct−1​}. Then ct=ct−1+c_t = c_{t-1}^+ct​=ct−1+​, Bt=Bt−1+B_t = B_{t-1}^+Bt​=Bt−1+​ (computed from ata_tat​), ρt=∣Det⁡Bt∣1/n\rho_t = |\operatorname{Det} B_t|^{1/n}ρt​=∣DetBt​∣1/n, and the method stops if

ρtr<ϵLt+ϵ,(5.2.17)\frac{\rho_t}{r} < \frac{\epsilon}{L_t + \epsilon}, \tag{5.2.17}rρt​​<Lt​+ϵϵ​,(5.2.17)

returning the productive search point cτ−1c_{\tau-1}cτ−1​, τ≤t\tau \le tτ≤t, with the smallest value of fff. Finally Var⁡R(f)=max⁡E0f−min⁡E0f\operatorname{Var}_R(f) = \max_{E_0} f - \min_{E_0} fVarR​(f)=maxE0​​f−minE0​​f.

Formalization targets

Goal: Theorem 5.2.1 (p. 349)

For every accuracy ϵ>0\epsilon > 0ϵ>0, every separation oracle for XXX and every first order oracle for fff, the ellipsoid method terminates after no more than

N(ϵ)=Ceil⁡(2n2[ln⁡(Rr)+ln⁡(ϵ+Var⁡R(f)ϵ)])+1(5.2.18)N(\epsilon) = \operatorname{Ceil}\Big(2n^2\Big[\ln\Big(\frac Rr\Big) + \ln\Big(\frac{\epsilon + \operatorname{Var}_R(f)}{\epsilon}\Big)\Big]\Big) + 1 \tag{5.2.18}N(ϵ)=Ceil(2n2[ln(rR​)+ln(ϵϵ+VarR​(f)​)])+1(5.2.18)

steps, and its result x^\widehat xx satisfies

x^∈Xandf(x^)−min⁡Xf≤ϵ.(5.2.19)\widehat x \in X \quad\text{and}\quad f(\widehat x) - \min_X f \le \epsilon. \tag{5.2.19}x∈Xandf(x)−Xmin​f≤ϵ.(5.2.19)

Milestones

  • Statement (∗), case n>1n > 1n>1 (p. 344): the half-ellipsoid {x∈E(c,B)∣aTx≤aTc}\{x \in E(c,B) \mid a^Tx \le a^Tc\}{x∈E(c,B)∣aTx≤aTc} lies in E(c+,B+)E(c^+, B^+)E(c+,B+), and Vol⁡E(c+,B+)=(n/n2−1)n−1nn+1Vol⁡E(c,B)≤e−1/(2n)Vol⁡E(c,B)\operatorname{Vol}E(c^+,B^+) = (n/\sqrt{n^2-1})^{n-1}\frac{n}{n+1}\operatorname{Vol}E(c,B) \le e^{-1/(2n)}\operatorname{Vol}E(c,B)VolE(c+,B+)=(n/n2−1​)n−1n+1n​VolE(c,B)≤e−1/(2n)VolE(c,B).
  • Eq. (5.2.21) (p. 350): ρτ≤e−τ/(2n2)R\rho_\tau \le e^{-\tau/(2n^2)}Rρτ​≤e−τ/(2n2)R at every step performed.
  • Eq. (5.2.28) (p. 352): Lt≤Var⁡R(f)L_t \le \operatorname{Var}_R(f)Lt​≤VarR​(f) for every ttt.
  • Claim 2∗ (p. 350): whenever the method terminates, its result is well defined and is a feasible ϵ\epsilonϵ-solution.

Significance

Theorem 5.2.1 bounds the number of oracle calls by a quantity that depends only on the dimension, on ln⁡(R/r)\ln(R/r)ln(R/r) and on ln⁡(1+Var⁡R(f)/ϵ)\ln(1 + \operatorname{Var}_R(f)/\epsilon)ln(1+VarR​(f)/ϵ): the cost of each additional digit of accuracy is O(n2)O(n^2)O(n2) steps, whatever the instance. Each step costs one call of each oracle and O(n2)O(n^2)O(n2) arithmetic operations. This is the ingredient the book's Theorem 5.3.1 combines with polynomial computability to conclude that convex programs are polynomially solvable, and it is the reason semidefinite and conic quadratic programs, the subject of the earlier lectures, are tractable in theory. The bound is also explicit enough to be checked numerically, with no hidden constants.

On the formal side, the platform has machine-checked versions of related results in other forms: Bertsimas and Tsitsiklis's half-ellipsoid lemma with the weaker ratio e−1/(2(n+1))e^{-1/(2(n+1))}e−1/(2(n+1)) and polyhedral feasibility version, Bubeck's version for objectives bounded on XXX with a convergence-rate conclusion, and Shor's localization theorem. None of these is the book's method: its guesses LtL_tLt​, its stopping rule (5.2.17), the explicit step count (5.2.18), or the exact volume identity (5.2.14). A formal proof of Theorem 5.2.1 gives a machine-checked oracle complexity bound with a stopping rule computable from the run alone.

Difficulty

The book's description of the method runs to two pages; the central difficulty is the termination analysis, not the geometry. The volume of the ellipsoids decreases geometrically, but their diameters need not, so the search points ctc_tct​ need not converge, and the method cannot know how close it is to the optimum. A naive argument that the search points approach the optimum therefore fails, and the stopping test (5.2.17), which only sees ρt\rho_tρt​, rrr and the guesses LtL_tLt​, has to be related to the unknown optimality gap. The analysis must also cover runs in which no step was productive for a long time, and the possibility that the result is undefined. On the geometric side, (∗) requires the exact determinant of a rank-one update and the elementary but not immediate inequality (n/n2−1)n−1nn+1≤e−1/(2n)(n/\sqrt{n^2-1})^{n-1}\frac{n}{n+1} \le e^{-1/(2n)}(n/n2−1​)n−1n+1n​≤e−1/(2n). Reasoning about a recursively defined algorithm also means carrying invariants (the ellipsoid contains every point of XXX not yet cut off, Det⁡Bt≠0\operatorname{Det} B_t \ne 0DetBt​=0) through the induction.

Formalization scope

Vectors are Fin n → ℝ, matrices Matrix (Fin n) (Fin n) ℝ, and the Euclidean norm eucNorm x = √(x ⬝ᵥ x) is defined explicitly (Mathlib's norm on Fin n → ℝ is the sup norm). Volumes are MeasureTheory.volume on Fin n → ℝ, valued in ℝ≥0∞. The setting (5.2.9) with assumption A is the predicate IsBlackBoxProgram f X r R. The oracles are arbitrary functions of the query point satisfying (5.2.10) and (5.2.11); every theorem is quantified over all of them, and none sees the centre xˉ\bar xxˉ. The method is a function run from the number of steps performed to an outcome, running with the current ct,Bt,Ltc_t, B_t, L_tct​,Bt​,Lt​ and best productive point, or stopped with an optional result; TerminatesAt t res says the run stops exactly at step t≥1t \ge 1t≥1. max⁡E0f\max_{E_0} fmaxE0​​f and min⁡E0f\min_{E_0} fminE0​​f are reals given by IsGreatest/IsLeast, and min⁡Xf\min_X fminX​f is expressed by comparison with every point of XXX, so no supremum or infimum with a default value occurs. Ceil is Int.ceil and the step bound is compared in Z\mathbb ZZ. A statement about an arbitrary sequence of ellipsoids or an arbitrary "state" carrying no link to the run would trivialize the goal; here the ellipsoids, guesses and result are those the method constructs from the oracles' answers.

Beyond the paper. The book's statement (∗) also has a case n=1n = 1n=1, whose printed centre c−12Ba/∣Ba∣c - \frac12 Ba/|Ba|c−21​Ba/∣Ba∣ moves by 12\frac1221​ regardless of the segment's length; the containment fails for c=0c = 0c=0, B=4B = 4B=4, a=1a = 1a=1. The case is posed as printed (expected to be disproved) and as a corrected variant with centre c−12B (Ba/∣Ba∣)c - \frac12 B\,(Ba/|Ba|)c−21​B(Ba/∣Ba∣). Theorem 5.2.1 assumes n≥2n \ge 2n≥2 and is unaffected.

A complete development needs the determinant of a rank-one update (Matrix.det_add_replicateCol_mul_replicateRow), Lebesgue measure of linear images (MeasureTheory.Measure.addHaar_image_linearMap), the continuity of convex functions on Rn\mathbb R^nRn, and an induction over run. The ellipsoid update lemma and the oracle and method definitions are reusable for other cutting-plane methods. Proofs of individual milestones, in particular (∗), are welcome as separate contributions.

Selected references

  • A. Ben-Tal, A. Nemirovski, Lectures on Modern Convex Optimization: Analysis, Algorithms, and Engineering Applications, MPS/SIAM Series on Optimization, SIAM, 2001. doi:10.1137/1.9780898718829
  • D. B. Yudin, A. S. Nemirovski, Informational complexity and efficient methods for the solution of convex extremal problems, Ekonomika i Matematicheskie Metody 12 (1976), 357–369.
  • N. Z. Shor, Cut-off method with space extension in convex programming problems, Cybernetics 13 (1977), 94–96. doi:10.1007/BF01071394
  • L. G. Khachiyan, A polynomial algorithm in linear programming, Soviet Math. Doklady 20 (1979), 191–194. mathnet
  • M. Grötschel, L. Lovász, A. Schrijver, Geometric Algorithms and Combinatorial Optimization, Springer, 1988. doi:10.1007/978-3-642-97881-4
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Convex OptimizationLinear algebraNumerical Analysis+2·Captain: Shuze Chen

Lectures on Modern Convex Optimization XI: Primal-Dual Path-Following for Semidefinite ProgrammingTextbook

Motivation

Semidefinite programming (SDP), the optimization of a linear function over the intersection of an affine subspace with the cone of positive semidefinite matrices, is the workhorse behind relaxations in combinatorial optimization, robust optimization and control. Its practical and theoretical tractability rests on interior point methods: algorithms that follow the central path, a curve of strictly feasible primal-dual pairs parametrized by a penalty parameter t>0t > 0t>0, along which the duality gap equals k/tk/tk/t. The polynomial-time analysis of these methods, due to Nesterov and Nemirovski (Interior-Point Polynomial Algorithms in Convex Programming, SIAM 1994) and, for the primal-dual SDP family considered here, to Monteiro and Zhang and others in the 1990s, reduces to one local statement: a single Newton-type update, started close to the path, lands close to the path again while the penalty parameter grows by a factor 1+Ω(k−1/2)1 + \Omega(k^{-1/2})1+Ω(k−1/2).

This mission formalizes that local statement in the form given by Ben-Tal and Nemirovski, Lectures on Modern Convex Optimization (SIAM 2001), Lecture 6, Theorem 6.5.2, for the whole family of primal-dual updates obtained from commutative scalings.

Setting

Let k≥1k \ge 1k≥1 and let Sk\mathbf S^kSk be the space of real symmetric k×kk\times kk×k matrices with the Frobenius inner product ⟨X,Y⟩F=Tr⁡(XY)\langle X, Y\rangle_F = \operatorname{Tr}(XY)⟨X,Y⟩F​=Tr(XY) and norm ∥A∥2=∑i,jAij2\|A\|_2 = \sqrt{\sum_{i,j}A_{ij}^2}∥A∥2​=∑i,j​Aij2​​. For X⪰0X \succeq 0X⪰0, X1/2X^{1/2}X1/2 is its positive semidefinite square root. Fix a linear subspace L⊆Sk\mathcal L \subseteq \mathbf S^kL⊆Sk, its orthogonal complement L⊥\mathcal L^\perpL⊥ in Sk\mathbf S^kSk, and B,C∈SkB, C \in \mathbf S^kB,C∈Sk. The primal-dual pair is

(P) min⁡X{Tr⁡(CX):X∈(L−B)∩S+k},(D) max⁡S{Tr⁡(BS):S∈(L⊥+C)∩S+k}.\text{(P)}\ \min_X\{\operatorname{Tr}(CX) : X \in (\mathcal L - B)\cap\mathbf S^k_+\},\qquad \text{(D)}\ \max_S\{\operatorname{Tr}(BS) : S \in (\mathcal L^\perp + C)\cap\mathbf S^k_+\}.(P) Xmin​{Tr(CX):X∈(L−B)∩S+k​},(D) Smax​{Tr(BS):S∈(L⊥+C)∩S+k​}.

XXX is strictly primal feasible if X∈L−BX \in \mathcal L - BX∈L−B and X≻0X \succ 0X≻0; SSS is strictly dual feasible if S∈L⊥+CS \in \mathcal L^\perp + CS∈L⊥+C and S≻0S \succ 0S≻0. For such a pair the duality gap is Tr⁡(CX)−Tr⁡(BS)+Tr⁡(CB)=Tr⁡(XS)\operatorname{Tr}(CX) - \operatorname{Tr}(BS) + \operatorname{Tr}(CB) = \operatorname{Tr}(XS)Tr(CX)−Tr(BS)+Tr(CB)=Tr(XS).

The distance of a pair X,S≻0X, S \succ 0X,S≻0 to the point of the central path with parameter ttt is

dist⁡((X,S),Z∗(t))=∥tX1/2SX1/2−I∥2,\operatorname{dist}((X,S), Z_*(t)) = \|tX^{1/2}SX^{1/2} - I\|_2 ,dist((X,S),Z∗​(t))=∥tX1/2SX1/2−I∥2​,

and the neighbourhood Nκ\mathcal N_\kappaNκ​ consists of the triples (t,X,S)(t, X, S)(t,X,S) with t>0t > 0t>0, X,SX, SX,S strictly feasible and distance at most κ\kappaκ.

The updating (U), with parameters κ,χ\kappa, \chiκ,χ, takes a strictly feasible pair (Xˉ,Sˉ)(\bar X, \bar S)(Xˉ,Sˉ) and

  1. sets tˉ=k/Tr⁡(XˉSˉ)\bar t = k/\operatorname{Tr}(\bar X\bar S)tˉ=k/Tr(XˉSˉ) and t+=(1−χ/k)−1 tˉt_+ = (1 - \chi/\sqrt k)^{-1}\,\bar tt+​=(1−χ/k​)−1tˉ;
  2. takes any Q≻0Q \succ 0Q≻0 such that QXˉQQ\bar XQQXˉQ and Q−1SˉQ−1Q^{-1}\bar SQ^{-1}Q−1SˉQ−1 commute;
  3. solves, for symmetric ΔX∈L\Delta X \in \mathcal LΔX∈L, ΔS∈L⊥\Delta S \in \mathcal L^\perpΔS∈L⊥, the linear system
Q[ΔX Sˉ+Xˉ ΔS]Q−1+Q−1[ΔS Xˉ+Sˉ ΔX]Q=2t+I−[QXˉSˉQ−1+Q−1SˉXˉQ];Q[\Delta X\,\bar S + \bar X\,\Delta S]Q^{-1} + Q^{-1}[\Delta S\,\bar X + \bar S\,\Delta X]Q = \tfrac{2}{t_+}I - [Q\bar X\bar SQ^{-1} + Q^{-1}\bar S\bar XQ];Q[ΔXSˉ+XˉΔS]Q−1+Q−1[ΔSXˉ+SˉΔX]Q=t+​2​I−[QXˉSˉQ−1+Q−1SˉXˉQ];
  1. returns X+=Xˉ+ΔXX_+ = \bar X + \Delta XX+​=Xˉ+ΔX, S+=Sˉ+ΔSS_+ = \bar S + \Delta SS+​=Sˉ+ΔS.

The choices Q=Xˉ−1/2Q = \bar X^{-1/2}Q=Xˉ−1/2, Q=Sˉ1/2Q = \bar S^{1/2}Q=Sˉ1/2 and the Nesterov–Todd scaling are all admissible in step 2.

Formalization targets

Goal: Theorem 6.5.2

If 0<χ≤κ≤0.10 < \chi \le \kappa \le 0.10<χ≤κ≤0.1 and the strictly feasible pair (Xˉ,Sˉ)(\bar X, \bar S)(Xˉ,Sˉ) satisfies ∥tˉ Xˉ1/2SˉXˉ1/2−I∥2≤κ\|\bar t\,\bar X^{1/2}\bar S\bar X^{1/2} - I\|_2 \le \kappa∥tˉXˉ1/2SˉXˉ1/2−I∥2​≤κ, then for every admissible QQQ the system of step 3 has exactly one solution, and

X+ and S+ are strictly feasible,t+=kTr⁡(X+S+),(t+,X+,S+)∈Nκ.X_+ \text{ and } S_+ \text{ are strictly feasible},\qquad t_+ = \frac{k}{\operatorname{Tr}(X_+S_+)},\qquad (t_+, X_+, S_+) \in \mathcal N_\kappa .X+​ and S+​ are strictly feasible,t+​=Tr(X+​S+​)k​,(t+​,X+​,S+​)∈Nκ​.

Milestones

The proof reduces to the case Q=IQ = IQ=I with Xˉ=Diag⁡(x)\bar X = \operatorname{Diag}(x)Xˉ=Diag(x), Sˉ=Diag⁡(s)\bar S = \operatorname{Diag}(s)Sˉ=Diag(s) and Tr⁡(XˉSˉ)=k\operatorname{Tr}(\bar X\bar S) = kTr(XˉSˉ)=k, and the milestones are the numbered facts of that reduced situation, with μ+=1−χk−1/2\mu_+ = 1 - \chi k^{-1/2}μ+​=1−χk−1/2 and ρ=χ2+κ2/(1−κ)\rho = \sqrt{\chi^2+\kappa^2}/(1-\kappa)ρ=χ2+κ2​/(1−κ):

  • (6.4.11): Tr⁡(X(tS−X−1)X(tS−X−1))=∥tX1/2SX1/2−I∥22\operatorname{Tr}(X(tS - X^{-1})X(tS - X^{-1})) = \|tX^{1/2}SX^{1/2} - I\|_2^2Tr(X(tS−X−1)X(tS−X−1))=∥tX1/2SX1/2−I∥22​.
  • Proposition 6.4.2, SDP case: dist⁡≤1\operatorname{dist} \le 1dist≤1 implies Tr⁡(XS)≤2k/t\operatorname{Tr}(XS) \le 2k/tTr(XS)≤2k/t.
  • Step 3∗: the reduced system ΔX⋅S+X⋅ΔS+ΔS⋅X+S⋅ΔX=2μ+I−2XS\Delta X\cdot S + X\cdot\Delta S + \Delta S\cdot X + S\cdot\Delta X = 2\mu_+I - 2XSΔX⋅S+X⋅ΔS+ΔS⋅X+S⋅ΔX=2μ+​I−2XS, ΔX∈L\Delta X \in \mathcal LΔX∈L, ΔS∈L⊥\Delta S \in \mathcal L^\perpΔS∈L⊥ has a unique solution.
  • (6.5.64)–(6.5.65): ∥X−1/2ΔXX−1/2∥2≤ρ\|X^{-1/2}\Delta XX^{-1/2}\|_2 \le \rho∥X−1/2ΔXX−1/2∥2​≤ρ and ∥X1/2ΔSX1/2∥2≤(1+κ)ρ\|X^{1/2}\Delta SX^{1/2}\|_2 \le (1+\kappa)\rho∥X1/2ΔSX1/2∥2​≤(1+κ)ρ.
  • 2∗(i)–(ii), (6.5.47), (6.5.66): X+,S+X_+, S_+X+​,S+​ are strictly feasible, Tr⁡(X+S+)=μ+k\operatorname{Tr}(X_+S_+) = \mu_+kTr(X+​S+​)=μ+​k, X+⪯(1+ρ)XX_+ \preceq (1+\rho)XX+​⪯(1+ρ)X.
  • (6.5.73): ∥μ+−1X+1/2S+X+1/2−I∥2≤ρ(1+ρ)1−χk−1/2[χk+ρ1−ρ+κ1−κ]\|\mu_+^{-1}X_+^{1/2}S_+X_+^{1/2} - I\|_2 \le \frac{\rho(1+\rho)}{1-\chi k^{-1/2}}\big[\frac{\chi}{\sqrt k} + \frac{\rho}{1-\rho} + \frac{\kappa}{1-\kappa}\big]∥μ+−1​X+1/2​S+​X+1/2​−I∥2​≤1−χk−1/2ρ(1+ρ)​[k​χ​+1−ρρ​+1−κκ​].
  • p. 421: for 0<χ≤κ≤0.10 < \chi \le \kappa \le 0.10<χ≤κ≤0.1 and every k≥1k \ge 1k≥1 the right-hand side of (6.5.73) is at most κ\kappaκ.

Significance

Theorem 6.5.2 is the step that turns the central path into an algorithm: once a pair in N0.1\mathcal N_{0.1}N0.1​ is known, iterating (U) keeps every iterate in N0.1\mathcal N_{0.1}N0.1​ and increases the penalty parameter by a constant factor every O(k)O(\sqrt k)O(k​) steps, so the duality gap Tr⁡(XS)≤2k/t\operatorname{Tr}(XS) \le 2k/tTr(XS)≤2k/t (Proposition 6.4.2) falls below ϵ\epsilonϵ after O(kln⁡(1/ϵ))O(\sqrt k\ln(1/\epsilon))O(k​ln(1/ϵ)) steps. The statement covers a whole family of search directions at once, including the Nesterov–Todd direction used by SDP solvers, and by Remark 6.5.2 it specializes to LP when all matrices are diagonal.

The result is classical and proved in the book; it has not been machine-checked. The platform has formalizations of central-path facts for LP and for inequality-form barrier problems, and open items on self-scaled short-step methods, but no statement about primal-dual Newton steps for SDP. A formal proof would supply reusable matrix-analysis infrastructure: Frobenius estimates through eigenvalues, the Löwner order under congruence, and unique solvability of Sylvester-type systems with subspace constraints.

Difficulty

The obvious approach, perturbation analysis of the Newton system in the original variables, does not close: the bound has to hold uniformly in the condition of Xˉ\bar XXˉ and Sˉ\bar SSˉ, and only the scaled quantities δX=X−1/2ΔXX−1/2\delta X = X^{-1/2}\Delta XX^{-1/2}δX=X−1/2ΔXX−1/2, δS=X1/2ΔSX1/2\delta S = X^{1/2}\Delta SX^{1/2}δS=X1/2ΔSX1/2 are controlled by κ\kappaκ and χ\chiχ. The reduction to Q=IQ = IQ=I with diagonal commuting Xˉ,Sˉ\bar X, \bar SXˉ,Sˉ has to be justified, including invariance of the distance under scaling and the change of the subspaces L\mathcal LL, L⊥\mathcal L^\perpL⊥ to QLQQ\mathcal LQQLQ, Q−1L⊥Q−1Q^{-1}\mathcal L^\perp Q^{-1}Q−1L⊥Q−1. Uniqueness uses the orthogonality Tr⁡(ΔXΔS)=0\operatorname{Tr}(\Delta X\Delta S) = 0Tr(ΔXΔS)=0 in an essential way. The final estimate passes from the scaled distance to the distance measured at the new point X+X_+X+​, which needs the Löwner bound X+⪯(1+ρ)XX_+ \preceq (1+\rho)XX+​⪯(1+ρ)X and monotonicity of the trace under congruence. The concluding numerical inequality holds for every k≥1k \ge 1k≥1, not only asymptotically.

Formalization scope

All matrices are Matrix (Fin k) (Fin k) ℝ with k≥1k \ge 1k≥1. L\mathcal LL is a Submodule ℝ of matrices with every element symmetric, and L⊥\mathcal L^\perpL⊥ is the set of symmetric SSS with Tr⁡(XS)=0\operatorname{Tr}(XS) = 0Tr(XS)=0 for all X∈LX \in \mathcal LX∈L, so the unknowns of the linear systems are symmetric. X1/2X^{1/2}X1/2 is Mathlib's CFC.sqrt (with open scoped MatrixOrder), positive (semi)definiteness is Matrix.PosDef/Matrix.PosSemidef, and the Frobenius norm is defined explicitly. The book's (P) comes from a conic problem min⁡{cTx:Ax−B⪰0}\min\{c^Tx : \mathcal Ax - B \succeq 0\}min{cTx:Ax−B⪰0} under Assumption A (A\mathcal AA injective) with L=Im⁡A\mathcal L = \operatorname{Im}\mathcal AL=ImA; every subspace is such an image, so the formal statements quantify over subspaces. The distance to the central path is defined by its SDP closed form (6.4.11), so no existence result for the central path is needed. The goal is stated for every admissible scaling QQQ, and "the system has a unique solution" is a separate conjunct from the properties of that solution, so the goal cannot hold vacuously through an unsolvable system. The milestones of the proof are stated in the book's reduced situation (diagonal Xˉ,Sˉ\bar X, \bar SXˉ,Sˉ, Q=IQ = IQ=I, Tr⁡(XˉSˉ)=k\operatorname{Tr}(\bar X\bar S) = kTr(XˉSˉ)=k) with all of its hypotheses.

Results of §§6.3–6.4 for general canonical cones (products of semidefinite and Lorentz cones with their barriers −ln⁡Det⁡X-\ln\operatorname{Det}X−lnDetX and −ln⁡(xTJx)-\ln(x^TJx)−ln(xTJx)), namely Propositions 6.3.1–6.3.2 and Theorems 6.4.1–6.4.2, and Theorem 6.5.1 (primal path-following), are not part of this mission: they need a calculus of canonical barriers on block-structured spaces. Proofs of any milestone, reusable lemmas on the Löwner order and the matrix square root, and a sorry-free proof of the numerical inequality are welcome.

Selected references

  • A. Ben-Tal, A. Nemirovski, Lectures on Modern Convex Optimization: Analysis, Algorithms, and Engineering Applications, MPS/SIAM Series on Optimization, SIAM, 2001, Lecture 6, §§6.4–6.5. https://doi.org/10.1137/1.9780898718829
  • Yu. Nesterov, A. Nemirovski, Interior-Point Polynomial Algorithms in Convex Programming, SIAM, 1994. https://doi.org/10.1137/1.9781611970791
  • Y. Zhang, On extending some primal–dual interior-point algorithms from linear programming to semidefinite programming, SIAM Journal on Optimization 8(2), 1998, 365–386. https://doi.org/10.1137/S1052623495296115
  • R. D. C. Monteiro, Primal–dual path-following algorithms for semidefinite programming, SIAM Journal on Optimization 7(3), 1997, 663–678. https://doi.org/10.1137/S1052623495293056
  • Yu. Nesterov, M. J. Todd, Self-scaled barriers and interior-point methods for convex programming, Mathematics of Operations Research 22(1), 1997, 1–42. https://doi.org/10.1287/moor.22.1.1
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Lectures on Modern Convex Optimization VIII: The Matrix Cube TheoremTextbook

Motivation

Many questions in robust control and robust optimization reduce to one test: does a whole family of symmetric matrices, generated by perturbing a nominal matrix along several directions at once, stay positive semidefinite? A linear system whose coefficients are only known to lie in intervals is a typical case. Showing that one quadratic Lyapunov function certifies stability of every member of such an interval matrix comes down to exactly this test. Ben-Tal and Nemirovski isolate it as the Matrix Cube problem. The problem is NP-hard (Ben-Tal & Nemirovski, On tractable approximations of uncertain linear matrix inequalities affected by interval uncertainty, SIAM J. Optim. 12 (2002)). They prove that a simple semidefinite sufficient condition is never far from exact. The gap is controlled by a universal factor that depends only on the ranks of the perturbation directions.

This mission formalizes that result as it appears in §4.4.3 of Lectures on Modern Convex Optimization (Ben-Tal & Nemirovski, SIAM 2001), pp. 189–197, together with the lemmas its proof uses and its application to interval Lyapunov stability.

Setting

Matrices are real. Sn\mathbf S^nSn is the space of symmetric n×nn\times nn×n matrices, S+n\mathbf S^n_+S+n​ its positive semidefinite cone, and X⪰YX\succeq YX⪰Y means X−Y∈S+nX-Y\in\mathbf S^n_+X−Y∈S+n​. For X∈SnX\in\mathbf S^nX∈Sn, λ(X)\lambda(X)λ(X) is its vector of eigenvalues, so ∥λ(X)∥1\|\lambda(X)\|_1∥λ(X)∥1​ is the sum of their absolute values.

Fix A0,A1,…,Am∈SnA_0,A_1,\dots,A_m\in\mathbf S^nA0​,A1​,…,Am​∈Sn with A0⪰0A_0\succeq0A0​⪰0. For a level ρ≥0\rho\ge0ρ≥0 the matrix cube is

Aρ={A0+∑i=1mziAi  :  ∥z∥∞≤ρ},\mathcal A_\rho=\Big\{A_0+\sum_{i=1}^m z_iA_i \;:\; \|z\|_\infty\le\rho\Big\},Aρ​={A0​+i=1∑m​zi​Ai​:∥z∥∞​≤ρ},

the image of the cube {∥z∥∞≤ρ}\{\|z\|_\infty\le\rho\}{∥z∥∞​≤ρ} under an affine map. The Matrix Cube problem asks for the largest ρ=R[A1,…,Am:A0]\rho=R[A_1,\dots,A_m:A_0]ρ=R[A1​,…,Am​:A0​] with Aρ⊂S+n\mathcal A_\rho\subset\mathbf S^n_+Aρ​⊂S+n​.

The system of LMIs (Sρ)(S_\rho)(Sρ​) in symmetric variables X1,…,XmX^1,\dots,X^mX1,…,Xm is

Xi⪰ρAi,Xi⪰−ρAi (i=1,…,m),∑i=1mXi⪯A0.X^i\succeq\rho A_i,\quad X^i\succeq-\rho A_i\ (i=1,\dots,m),\qquad \sum_{i=1}^mX^i\preceq A_0 .Xi⪰ρAi​,Xi⪰−ρAi​ (i=1,…,m),i=1∑m​Xi⪯A0​.

Its feasibility can be checked by semidefinite programming. The largest ρ\rhoρ for which it is solvable is ρ[A1,…,Am:A0]\rho[A_1,\dots,A_m:A_0]ρ[A1​,…,Am​:A0​], the optimal value of the semidefinite problem (4.4.45).

The approximation factor is the function

θ(k)=1min⁡{∫Rk∣α1u12+⋯+αkuk2∣ pk(u) du  :  α∈Rk, ∥α∥1=1},k≥1,\theta(k)=\frac{1}{\min\Big\{\int_{\mathbb R^k}|\alpha_1u_1^2+\cdots+\alpha_ku_k^2|\,p_k(u)\,du \;:\; \alpha\in\mathbb R^k,\ \|\alpha\|_1=1\Big\}},\qquad k\ge1,θ(k)=min{∫Rk​∣α1​u12​+⋯+αk​uk2​∣pk​(u)du:α∈Rk, ∥α∥1​=1}1​,k≥1,

where pk(u)=(2π)−k/2exp⁡{−uTu/2}p_k(u)=(2\pi)^{-k/2}\exp\{-u^Tu/2\}pk​(u)=(2π)−k/2exp{−uTu/2} is the standard Gaussian density on Rk\mathbb R^kRk. The relevant rank is μ=max⁡1≤i≤mRank⁡(Ai)\mu=\max_{1\le i\le m}\operatorname{Rank}(A_i)μ=max1≤i≤m​Rank(Ai​); A0A_0A0​ is not included.

For the application, A∗A^*A∗ is a stable n×nn\times nn×n matrix (all eigenvalues in the open left half-plane). D≠0D\neq0D=0 has nonnegative entries, and Uρ={A:∣Aij−Aij∗∣≤ρDij}\mathcal U_\rho=\{A:|A_{ij}-A^*_{ij}|\le\rho D_{ij}\}Uρ​={A:∣Aij​−Aij∗​∣≤ρDij​} is the interval matrix. (Ly[ρ])(\mathrm{Ly}[\rho])(Ly[ρ]) asks for X⪰IX\succeq IX⪰I with ATX+XA⪯−IA^TX+XA\preceq-IATX+XA⪯−I for all A∈UρA\in\mathcal U_\rhoA∈Uρ​, and R[A∗,D]R[A^*,D]R[A∗,D] is the supremum of the ρ≥0\rho\ge0ρ≥0 for which it is solvable. (A[ρ])(\mathrm A[\rho])(A[ρ]) is the analogue of (Sρ)(S_\rho)(Sρ​) for this cube. It uses matrix variables XXX and XijX^{ij}Xij for (i,j)∈D={Dij>0}(i,j)\in\mathcal D=\{D_{ij}>0\}(i,j)∈D={Dij​>0}, and ρ[A∗,D]\rho[A^*,D]ρ[A∗,D] is its supremum.

Formalization targets

Goal: the Matrix Cube Theorem (Theorem 4.4.1)

For all n,mn,mn,m, all A0⪰0A_0\succeq0A0​⪰0, all A1,…,Am∈SnA_1,\dots,A_m\in\mathbf S^nA1​,…,Am​∈Sn and all ρ≥0\rho\ge0ρ≥0:

(Sρ) not solvable ⟹ Aθ(μ)ρ⊄S+n,(S_\rho)\ \text{not solvable}\ \Longrightarrow\ \mathcal A_{\theta(\mu)\rho}\not\subset\mathbf S^n_+ ,(Sρ​) not solvable ⟹ Aθ(μ)ρ​⊂S+n​,

and

θ(k)≤πk2  (k≥1),θ(2)=π2.\theta(k)\le\frac{\pi\sqrt k}{2}\ \ (k\ge1),\qquad \theta(2)=\frac{\pi}{2}.θ(k)≤2πk​​  (k≥1),θ(2)=2π​.

Milestones, in attack order

  1. Proposition 4.4.5. If (Sρ)(S_\rho)(Sρ​) is solvable then Aρ⊂S+n\mathcal A_\rho\subset\mathbf S^n_+Aρ​⊂S+n​.
  2. Lemma 4.4.3. For W⪰0W\succeq0W⪰0 and A∈SnA\in\mathbf S^nA∈Sn,
max⁡U,V⪰0, U+V=WTr⁡([U−V]A)=max⁡X=XT, ∥λ(X)∥∞≤1Tr⁡(XW1/2AW1/2)=∥λ(W1/2AW1/2)∥1.\max_{U,V\succeq0,\,U+V=W}\operatorname{Tr}([U-V]A)=\max_{X=X^T,\ \|\lambda(X)\|_\infty\le1}\operatorname{Tr}(XW^{1/2}AW^{1/2})=\|\lambda(W^{1/2}AW^{1/2})\|_1 .U,V⪰0,U+V=Wmax​Tr([U−V]A)=X=XT, ∥λ(X)∥∞​≤1max​Tr(XW1/2AW1/2)=∥λ(W1/2AW1/2)∥1​.
  1. Lemma 4.4.4. For ξ∼N(0,In)\xi\sim\mathcal N(0,I_n)ξ∼N(0,In​) and A∈SnA\in\mathbf S^nA∈Sn: E{ξTAξ}=Tr⁡(A)\mathbf E\{\xi^TA\xi\}=\operatorname{Tr}(A)E{ξTAξ}=Tr(A) and E{∣ξTAξ∣}≥∥λ(A)∥1/θ(Rank⁡(A))\mathbf E\{|\xi^TA\xi|\}\ge\|\lambda(A)\|_1/\theta(\operatorname{Rank}(A))E{∣ξTAξ∣}≥∥λ(A)∥1​/θ(Rank(A)).
  2. Eq. (4.4.37). θ(k)≤πk/2\theta(k)\le\pi\sqrt k/2θ(k)≤πk​/2 for k≥1k\ge1k≥1, and θ(2)=π/2\theta(2)=\pi/2θ(2)=π/2.
  3. Corollary 4.4.1. If all Rank⁡(Ai)≤μ\operatorname{Rank}(A_i)\le\muRank(Ai​)≤μ, then
ρ[A1,…,Am:A0]≤R[A1,…,Am:A0]≤θ(μ) ρ[A1,…,Am:A0].\rho[A_1,\dots,A_m:A_0]\le R[A_1,\dots,A_m:A_0]\le\theta(\mu)\,\rho[A_1,\dots,A_m:A_0].ρ[A1​,…,Am​:A0​]≤R[A1​,…,Am​:A0​]≤θ(μ)ρ[A1​,…,Am​:A0​].
  1. Proposition 4.4.6. If (A[ρ])(\mathrm A[\rho])(A[ρ]) is solvable, its XXX-component solves (Ly[ρ])(\mathrm{Ly}[\rho])(Ly[ρ]). If it is not solvable, neither is (Ly[πρ/2])(\mathrm{Ly}[\pi\rho/2])(Ly[πρ/2]). Hence ρ[A∗,D]≤R[A∗,D]≤π2ρ[A∗,D]\rho[A^*,D]\le R[A^*,D]\le\frac\pi2\rho[A^*,D]ρ[A∗,D]≤R[A∗,D]≤2π​ρ[A∗,D].
  2. Lemma 4.4.5. ∥λ(fgT+gfT)∥1=2∥f∥2∥g∥2\|\lambda(fg^T+gf^T)\|_1=2\|f\|_2\|g\|_2∥λ(fgT+gfT)∥1​=2∥f∥2​∥g∥2​.

Significance

The result. Proposition 4.4.5 and Theorem 4.4.1 together bound the cube radius. It lies between the efficiently computable ρ[⋅]\rho[\cdot]ρ[⋅] and θ(μ)ρ[⋅]\theta(\mu)\rho[\cdot]θ(μ)ρ[⋅]. The factor is πμ/2\pi\sqrt\mu/2πμ​/2 in general, independent of nnn and mmm, and exactly π/2\pi/2π/2 when every perturbation has rank at most two. Rank two is the situation of interval matrices, of Lyapunov certificates for interval systems (Proposition 4.4.6), and of a re-derivation of Nesterov's π/2\pi/2π/2 theorem for quadratic maximization over the unit cube (pp. 200–201). The same estimate underlies tractable approximations of robust LMIs with box uncertainty in robust semidefinite optimization.

Formalizing it. The results are proved in the book. None of them, and nothing on the matrix cube, the function θ\thetaθ or interval Lyapunov stability, is machine-checked on the platform. The formalization adds three things: a checked definition of θ\thetaθ as a Gaussian integral; a checked proof of the constants πk/2\pi\sqrt k/2πk​/2 and π/2\pi/2π/2; and a checked bridge from semidefinite duality to a probabilistic rounding argument. The proof of Proposition 4.4.5 already has a sorry-free local check, which also exposed a sign slip in the printed proof.

Difficulty

The sufficient direction is elementary. The converse is not. Unsolvability of (Sρ)(S_\rho)(Sρ​) is a statement about a semidefinite program, and turning it into an explicit point zzz with ∥z∥∞≤θ(μ)ρ\|z\|_\infty\le\theta(\mu)\rho∥z∥∞​≤θ(μ)ρ and A0+∑ziAi⪰̸0A_0+\sum z_iA_i\not\succeq0A0​+∑zi​Ai​⪰0 needs three ingredients:

  • a strictly feasible conic duality argument, to obtain dual certificates;
  • an exact spectral identity (Lemma 4.4.3);
  • an averaging argument over a Gaussian direction, with a sharp lower bound on E∣ξTAξ∣\mathbf E|\xi^TA\xi|E∣ξTAξ∣ in terms of rank and trace norm.

Bounding coordinate by coordinate, or using a worst-case vertex of the cube, gives a factor that grows with mmm. The rank-dependent constant is what makes the theorem useful.

The constants need real analysis on Gaussian integrals. θ(2)=π/2\theta(2)=\pi/2θ(2)=π/2 requires an exact minimization of ∫∣θu12−(1−θ)u22∣p2(u) du\int|\theta u_1^2-(1-\theta)u_2^2|p_2(u)\,du∫∣θu12​−(1−θ)u22​∣p2​(u)du over θ∈[0,1]\theta\in[0,1]θ∈[0,1]. The bound πk/2\pi\sqrt k/2πk​/2 requires a symmetrization and an independence argument. Lemma 4.4.4 needs rotational invariance of the Gaussian measure and diagonalization inside an integral.

Formalization scope

  • Matrices are Matrix (Fin n) (Fin n) ℝ, and X⪰YX\succeq YX⪰Y is (X - Y).PosSemidef (which includes symmetry). The index i=1,…,mi=1,\dots,mi=1,…,m is Fin m, and ∥z∥∞≤ρ\|z\|_\infty\le\rho∥z∥∞​≤ρ is ∣zi∣≤ρ|z_i|\le\rho∣zi​∣≤ρ for every iii.
  • W1/2W^{1/2}W1/2 is CFC.sqrt W under MatrixOrder. Eigenvalues are Mathlib's IsHermitian.eigenvalues, used only through order-independent quantities.
  • Expectations under N(0,In)\mathcal N(0,I_n)N(0,In​) are Lebesgue integrals against the density pnp_npn​, which is how the book describes the distribution.
  • θ\thetaθ is the specific function (4.4.38), with the minimum as a real infimum, attained for k≥1k\ge1k≥1. The book leaves θ(0)\theta(0)θ(0) undefined. Lean's formula gives it the value 000, and no statement depends on it: where μ=0\mu=0μ=0 the hypotheses of Theorem 4.4.1 cannot hold, and Corollary 4.4.1 assumes μ≥1\mu\ge1μ≥1.
  • The radii R[⋅]R[\cdot]R[⋅], ρ[⋅]\rho[\cdot]ρ[⋅], R[A∗,D]R[A^*,D]R[A∗,D], ρ[A∗,D]\rho[A^*,D]ρ[A∗,D] are suprema in EReal, so +∞+\infty+∞ is represented. Ratios are stated in product form, for example R≤θ(μ)ρ[⋅]R\le\theta(\mu)\rho[\cdot]R≤θ(μ)ρ[⋅]. The "max" in (4.4.45) is stated as attained.
  • The level ρ≥0\rho\ge0ρ≥0 is a hypothesis, as in the book's setting. For negative ρ\rhoρ the cube is empty and the theorem fails.

A formalization that replaced θ\thetaθ by an arbitrary function satisfying (4.4.37), or set μ=max⁡0≤i≤m\mu=\max_{0\le i\le m}μ=max0≤i≤m​, or allowed ρ<0\rho<0ρ<0, would state a different (false or ill-posed) theorem; the statements here rule these out.

Infrastructure needed and reusable beyond this mission:

  • Gaussian integrals of quadratic forms on Rn\mathbb R^nRn and their rotation invariance;
  • the trace-norm identity of Lemma 4.4.3;
  • strict-feasibility semidefinite duality for the problem (4.4.39);
  • the spectrum of rank-two symmetric matrices.

Contributions of separate lemmas are welcome, for example monotonicity of θ\thetaθ or θ(1)=1\theta(1)=1θ(1)=1.

Selected references

  • A. Ben-Tal, A. Nemirovski, Lectures on Modern Convex Optimization: Analysis, Algorithms, and Engineering Applications, SIAM/MPS Series on Optimization, 2001, §4.4.3. https://doi.org/10.1137/1.9780898718829
  • A. Ben-Tal, A. Nemirovski, On tractable approximations of uncertain linear matrix inequalities affected by interval uncertainty, SIAM Journal on Optimization 12(3), 2002. https://doi.org/10.1137/S1052623401384392
  • Yu. Nesterov, Semidefinite relaxation and nonconvex quadratic optimization, Optimization Methods and Software 9, 1998. https://doi.org/10.1080/10556789808805690
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Lectures on Modern Convex Optimization VII: The S-Lemma with Two Quadratic ConstraintsTextbook

Motivation

A homogeneous quadratic inequality xTBx≥0x^TBx \ge 0xTBx≥0 may hold at every point where other quadratic inequalities xTAix≥0x^TA_ix \ge 0xTAi​x≥0 hold. Deciding when this happens is the quadratic analogue of the question the Farkas lemma answers for linear inequalities. It is the core of robust optimization with ellipsoidal uncertainty, of absolute stability in control (where it is known as the S-procedure), and of trust-region and quadratically constrained programming. The answer one wants is a linear certificate: nonnegative multipliers λi\lambda_iλi​ with B⪰∑iλiAiB \succeq \sum_i \lambda_iA_iB⪰∑i​λi​Ai​, a condition that can be checked by semidefinite programming.

Lecture 4 of Ben-Tal and Nemirovski, Lectures on Modern Convex Optimization (SIAM, 2001, doi:10.1137/1.9780898718829), states the classical case and, in its exercises (§4.10.5), traces how far it extends:

  • V. A. Yakubovich (1971) proved the S-lemma: with one strictly feasible constraint, the certificate exists exactly when the implication holds.
  • L. L. Dines (1941) proved that the joint range {(xTAx,xTBx)}\{(x^TAx, x^TBx)\}{(xTAx,xTBx)} of two quadratic forms is convex.
  • B. T. Polyak (J. Optim. Theory Appl. 99, 1998, doi:10.1023/A:1021798932766) proved that for n≥3n \ge 3n≥3 the joint range of three forms is closed and convex once some linear combination of the matrices is positive definite. From this he derived an S-lemma with two constraints.
  • For three constraints, or without Polyak's hypotheses, the certificate can fail to exist even though the implication holds (Exercises 4.47, 4.54, 4.56 of the book).

Setting

Vectors are x∈Rnx \in \mathbb R^nx∈Rn and matrices are real n×nn\times nn×n. For a symmetric matrix AAA, the quadratic form is xTAxx^TAxxTAx. P⪰QP \succeq QP⪰Q means that P−QP - QP−Q is positive semidefinite, and P≻0P \succ 0P≻0 means PPP is positive definite. A quadratic inequality xTCx≥0x^TCx \ge 0xTCx≥0 is a consequence of a system xTAx≥0x^TAx \ge 0xTAx≥0, xTBx≥0x^TBx \ge 0xTBx≥0 if it holds at every x∈Rnx \in \mathbb R^nx∈Rn satisfying the system. The system is strictly feasible if some xˉ\bar xxˉ satisfies both inequalities strictly.

The inhomogeneous case uses f(x)=xTAx+2aTx+αf(x) = x^TAx + 2a^Tx + \alphaf(x)=xTAx+2aTx+α and g(x)=xTBx+2bTx+βg(x) = x^TBx + 2b^Tx + \betag(x)=xTBx+2bTx+β. For the topological steps, Sn−1S^{n-1}Sn−1 is the unit sphere of Rn\mathbb R^nRn. The projective space Pn−1P^{n-1}Pn−1 is Sn−1S^{n-1}Sn−1 with each eee identified with −e-e−e, and Φ:Sn−1→Pn−1\Phi : S^{n-1} \to P^{n-1}Φ:Sn−1→Pn−1 is the canonical projection.

Formalization targets

Goal: the two-constraint S-lemma, (SL.C) (pp. 306–307)

Let n≥3n \ge 3n≥3 and let A,B,CA, B, CA,B,C be symmetric matrices such that (i) some linear combination aA+bB+cCaA + bB + cCaA+bB+cC is positive definite and (ii) xˉTAxˉ>0\bar x^TA\bar x > 0xˉTAxˉ>0, xˉTBxˉ>0\bar x^TB\bar x > 0xˉTBxˉ>0 for some xˉ\bar xxˉ. Then

(∀x: xTAx≥0, xTBx≥0⇒xTCx≥0)  ⟺  ∃ λ,μ≥0: C⪰λA+μB.\Big(\forall x:\ x^TAx \ge 0,\ x^TBx \ge 0 \Rightarrow x^TCx \ge 0\Big) \iff \exists\, \lambda, \mu \ge 0:\ C \succeq \lambda A + \mu B.(∀x: xTAx≥0, xTBx≥0⇒xTCx≥0)⟺∃λ,μ≥0: C⪰λA+μB.

Milestones

  1. Proposition 4.3.4 (p. 176): if B⪰∑iλiAiB \succeq \sum_i\lambda_iA_iB⪰∑i​λi​Ai​ with λi≥0\lambda_i \ge 0λi​≥0, then xTAix≥0x^TA_ix \ge 0xTAi​x≥0 for all iii implies xTBx≥0x^TBx \ge 0xTBx≥0.
  2. Theorem 4.3.3, S-lemma (p. 176): if xˉTAxˉ>0\bar x^TA\bar x > 0xˉTAxˉ>0 for some xˉ\bar xxˉ, then xTBx≥0x^TBx \ge 0xTBx≥0 is a consequence of xTAx≥0x^TAx \ge 0xTAx≥0 iff B⪰λAB \succeq \lambda AB⪰λA for some λ≥0\lambda \ge 0λ≥0.
  3. Proposition 4.10.1, inhomogeneous S-lemma (p. 303): if f(xˉ)<0f(\bar x) < 0f(xˉ)<0 for some xˉ\bar xxˉ, then f≤0⇒g≤0f \le 0 \Rightarrow g \le 0f≤0⇒g≤0 holds iff g≤λfg \le \lambda fg≤λf on Rn\mathbb R^nRn for some λ≥0\lambda \ge 0λ≥0. Equivalently, as printed, iff (λα[λa−b]Tλa−bλA−B)⪰0\begin{pmatrix}\lambda\alpha & [\lambda a - b]^T\\ \lambda a - b & \lambda A - B\end{pmatrix} \succeq 0(λαλa−b​[λa−b]TλA−B​)⪰0 for some λ≥0\lambda \ge 0λ≥0. If moreover g(x)≥0g(x) \ge 0g(x)≥0 is strictly feasible, then λ>0\lambda > 0λ>0.
  4. Theorem 4.10.1, general Helly theorem (p. 305): a family of closed convex sets in Rn\mathbb R^nRn has a common point if every n+1n+1n+1 of them do and some finite subfamily has bounded intersection.
  5. (SL.B) (p. 305): if xˉTAxˉ>0\bar x^TA\bar x > 0xˉTAxˉ>0 for some xˉ\bar xxˉ and xTAx≥0x^TAx \ge 0xTAx≥0, x≠0x \ne 0x=0 imply xTBx>0x^TBx > 0xTBx>0, then B⪰λAB \succeq \lambda AB⪰λA for some λ≥0\lambda \ge 0λ≥0.
  6. Proposition 4.10.2 (p. 308): if any two points of Y⊂Sn−1Y \subset S^{n-1}Y⊂Sn−1 can be linked inside YYY to a common antipodal pair {y,−y}\{y, -y\}{y,−y}, then Φ(Y)\Phi(Y)Φ(Y) is path connected.
  7. Proposition 4.10.4 (p. 308): for n≥3n \ge 3n≥3 and a nonempty zero set Y={x∈Sn−1:xTQx=0}Y = \{x \in S^{n-1} : x^TQx = 0\}Y={x∈Sn−1:xTQx=0}, Y=−YY = -YY=−Y and Φ(Y)\Phi(Y)Φ(Y) is connected.
  8. (SL.D), Polyak's theorem (p. 307): for n≥3n \ge 3n≥3 and symmetric A1,A2,A3A_1, A_2, A_3A1​,A2​,A3​ with a positive definite linear combination, {(xTA1x,xTA2x,xTA3x):x∈Rn}\{(x^TA_1x, x^TA_2x, x^TA_3x) : x \in \mathbb R^n\}{(xTA1​x,xTA2​x,xTA3​x):x∈Rn} is closed and convex.

Significance

The S-lemma converts a semi-infinite family of quadratic implications into one linear matrix inequality. This is what makes robust counterparts of conic quadratic constraints with ellipsoidal uncertainty semidefinite-representable (Proposition 4.5.1 of the book), and it gives trust-region subproblems and quadratic programs with one constraint their exact semidefinite duals. The two-constraint version extends this exactness to problems with two quadratic constraints in dimension at least three. Polyak's convexity theorem is the structural fact behind it, and it is of independent use in the study of joint numerical ranges.

All statements are proved in the literature. On Prove2Me, the inhomogeneous S-procedure in another sign convention is proved (ConvexOptimization.s_procedure), as is the finite Helly theorem (FamousTheorems.helly_theorem). The homogeneous S-lemma is a special case of the former but is not stated on the platform. The infinite Helly theorem with the boundedness condition, Polyak's theorem, the projective-space connectedness facts and the two-constraint S-lemma have no machine-checked statement or proof there. Two statements beyond the book are posed alongside it (see Formalization scope).

Difficulty

The "if" directions are one line each. Every "only if" direction must produce multipliers from a pointwise implication, and there is no Farkas lemma for quadratic inequalities to do it. With two constraints a direct separation argument needs the joint range of three quadratic forms to be convex. That range is not convex in general, and it can fail to be convex for n=2n = 2n=2, so any argument has to use the dimension. The book's milestones for this step are topological: paths on spheres, quotients by the antipodal map, and connectedness in projective space. None of this is packaged for this use in Mathlib. Two printed details mislead a solver who follows the page. The matrix in Proposition 4.10.1 omits −β-\beta−β in its northwestern entry. The hint for (SL.C) (Exercise 4.48) asks for a positive definite combination θC−λA−μB\theta C - \lambda A - \mu BθC−λA−μB, where only semidefiniteness can be obtained. The proof of Theorem 4.3.3 also swaps the roles of DTADD^TADDTAD and DTBDD^TBDDTBD at one step.

Formalization scope

Vectors are Fin n → ℝ and matrices Matrix (Fin n) (Fin n) ℝ. The form xTAxx^TAxxTAx is x ⬝ᵥ (A *ᵥ x) and symmetry is Matrix.IsHermitian. ⪰0\succeq 0⪰0 and ≻0\succ 0≻0 are Mathlib's Matrix.PosSemidef and Matrix.PosDef, both of which include symmetry. The bordered (n+1)×(n+1)(n+1)\times(n+1)(n+1)×(n+1) matrix of Proposition 4.10.1 is indexed by Unit ⊕ Fin n with the scalar entry first, as printed. For Propositions 4.10.2 and 4.10.4, the sphere is Metric.sphere (0 : EuclideanSpace ℝ (Fin n)) 1. Pn−1P^{n-1}Pn−1 is its quotient by e∼±ee \sim \pm ee∼±e with the quotient topology (one definition item), which has the same topology as the book's metric min⁡{∥e+e′∥2,∥e−e′∥2}\min\{\|e+e'\|_2, \|e-e'\|_2\}min{∥e+e′∥2​,∥e−e′∥2​}. The book's linear connectedness, which allows the empty set, is stated pairwise. Every hypothesis of the page is an explicit binder. In particular, strict feasibility appears in every S-lemma variant, n≥3n \ge 3n≥3 appears in (SL.C), (SL.D) and Proposition 4.10.4, and the positive definite combination in (SL.C) involves all three of A,B,CA, B, CA,B,C with coefficients of any sign. The implication is quantified over all of Rn\mathbb R^nRn and the multipliers carry their sign constraints. Dropping (ii), or leaving λ,μ\lambda, \muλ,μ unconstrained, turns the goal into a statement that is false or trivial, and neither is the book's.

Beyond the paper. Two variants are posed beside the faithful items. One is a corrected Proposition 4.10.1 with northwestern entry λα−β\lambda\alpha - \betaλα−β: as printed, the matrix criterion fails for n=1n = 1n=1, f=x2−1f = x^2 - 1f=x2−1, g=x2−4g = x^2 - 4g=x2−4. The other is a sharpness probe of (SL.C) without n≥3n \ge 3n≥3, for which A=diag(1,−1)A = \mathrm{diag}(1,-1)A=diag(1,−1), B=(0110)B = \begin{pmatrix}0&1\\1&0\end{pmatrix}B=(01​10​), C=(011−2)C = \begin{pmatrix}0&1\\1&-2\end{pmatrix}C=(01​1−2​) is a counterexample; its disproof is the sought outcome.

Contributions welcome: the joint range of quadratic forms (Dines's theorem, Polyak's theorem), the projective space as a topological space, and infinite Helly-type intersection theorems. All are reusable beyond this chapter.

Selected references

  • A. Ben-Tal, A. Nemirovski, Lectures on Modern Convex Optimization: Analysis, Algorithms, and Engineering Applications, SIAM, 2001. doi:10.1137/1.9780898718829
  • B. T. Polyak, Convexity of quadratic transformations and its use in control and optimization, J. Optim. Theory Appl. 99 (1998), 553–583. doi:10.1023/A:1021798932766
  • I. Pólik, T. Terlaky, A survey of the S-lemma, SIAM Review 49 (2007), 371–418. doi:10.1137/S003614450444614X
  • L. L. Dines, On the mapping of quadratic forms, Bull. Amer. Math. Soc. 47 (1941), 494–498. doi:10.1090/S0002-9904-1941-07494-X
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Lectures on Modern Convex Optimization IV: The Compliance of a Truss Is Conic Quadratic RepresentableTextbook

Motivation

Truss topology design asks for the stiffest elastic bar construction that can be built from a given set of potential bars with a given amount of material. It is one of the oldest test cases of structural optimization (Bendsøe and Sigmund, Topology Optimization, Springer 2003) and one of the main applications in Ben-Tal and Nemirovski's Lectures on Modern Convex Optimization (SIAM 2001). The quantity being minimized, the compliance of the truss under a load, is defined through the solution of a linear system and takes the value +∞+\infty+∞ when the structure cannot carry the load, so it is not obviously a convex function, let alone one a solver can handle. Lecture 1 of the book shows that the single-load problem happens to become a linear program. Section 3.4.3 explains why: the compliance, as a function of the bar volumes and of the load jointly, is conic quadratic representable, and its epigraph has an explicit description by second-order cone constraints. That description is what turns multiload designs, bounds on bar volumes and other variants into conic quadratic programs.

This mission is the fourth of a series formalizing the book's main results, and covers Lecture 3, §3.4.3 (pp. 120–128), together with Proposition 2.4.2 of Lecture 2, on which it relies.

Setting

A ground structure (n,m,B1,…,Bn)(n, m, B_1, \dots, B_n)(n,m,B1​,…,Bn​) consists of real m×kim \times k_im×ki​ matrices BiB_iBi​, i=1,…,ni = 1, \dots, ni=1,…,n (for a classical truss ki=1k_i = 1ki​=1 and BiB_iBi​ is the direction vector of bar iii). A truss is a vector t∈Rnt \in \mathbb R^nt∈Rn with t≥0t \ge 0t≥0 (the bar volumes) and a load is f∈Rmf \in \mathbb R^mf∈Rm. The bar-stiffness matrix is

A(t)=∑i=1ntiBiBiT,A(t) = \sum_{i=1}^n t_i B_i B_i^T,A(t)=i=1∑n​ti​Bi​BiT​,

and the compliance is

Complf(t)=12fTvwhere A(t)v=f,\mathrm{Compl}_f(t) = \tfrac12 f^Tv \quad\text{where } A(t)v = f,Complf​(t)=21​fTvwhere A(t)v=f,

with Complf(t)=+∞\mathrm{Compl}_f(t) = +\inftyComplf​(t)=+∞ when the equilibrium equation A(t)v=fA(t)v = fA(t)v=f has no solution; the value does not depend on which solution vvv is used. For ttt that are not nonnegative the compliance is extended by +∞+\infty+∞. The potential energy of the loaded truss is Ct,f(v)=12vTA(t)v−fTv\mathcal C_{t,f}(v) = \tfrac12 v^TA(t)v - f^TvCt,f​(v)=21​vTA(t)v−fTv.

The ice cream cone is Lk={x∈Rk:xk≥x12+⋯+xk−12}\mathbf L^k = \{x \in \mathbb R^k : x_k \ge \sqrt{x_1^2 + \dots + x_{k-1}^2}\}Lk={x∈Rk:xk​≥x12​+⋯+xk−12​​}. A set X⊂RNX \subset \mathbb R^NX⊂RN is conic quadratic representable (CQr) if there are finitely many inequalities Aj(x;u)−bj∈LmjA_j(x; u) - b_j \in \mathbf L^{m_j}Aj​(x;u)−bj​∈Lmj​, affine in xxx and in additional variables u∈Rlu \in \mathbb R^lu∈Rl, such that x∈Xx \in Xx∈X exactly when some uuu satisfies all of them; a function with values in R∪{+∞}\mathbb R \cup \{+\infty\}R∪{+∞} is CQr when its epigraph is. A linear vector inequality Ax−b∈KAx - b \in \mathbf KAx−b∈K is almost solvable if for every ε>0\varepsilon > 0ε>0 some b′b'b′ with ∥b′−b∥2<ε\|b' - b\|_2 < \varepsilon∥b′−b∥2​<ε makes Ax−b′∈KAx - b' \in \mathbf KAx−b′∈K solvable.

Formalization targets

Goal: Proposition 3.4.5 (p. 127)

For all t∈Rnt \in \mathbb R^nt∈Rn, f∈Rmf \in \mathbb R^mf∈Rm and τ∈R\tau \in \mathbb Rτ∈R, Complf(t)≤τ\mathrm{Compl}_f(t) \le \tauComplf​(t)≤τ (extended compliance) if and only if there are vectors si∈Rkis_i \in \mathbb R^{k_i}si​∈Rki​ with

(a) ∑i=1nBisi=f,(b) ∑i=1nsiTsi2ti≤τ,(c) t≥0,\text{(a)}\ \sum_{i=1}^n B_is_i = f, \qquad \text{(b)}\ \sum_{i=1}^n \frac{s_i^Ts_i}{2t_i} \le \tau, \qquad \text{(c)}\ t \ge 0,(a) i=1∑n​Bi​si​=f,(b) i=1∑n​2ti​siT​si​​≤τ,(c) t≥0,

where 0/0=00/0 = 00/0=0 and a/0=+∞a/0 = +\inftya/0=+∞ for a>0a > 0a>0. In particular, (t,f)↦Complf(t)(t, f) \mapsto \mathrm{Compl}_f(t)(t,f)↦Complf​(t) is CQr.

Milestones

  • Lemma 3.4.1 (p. 122): for a symmetric positive semidefinite AAA, the form 12vTAv−bTv\tfrac12 v^TAv - b^Tv21​vTAv−bTv is bounded below iff it attains its minimum iff Av=bAv = bAv=b is solvable; the minimizers are the solutions, and the minimum is −12bTv-\tfrac12 b^Tv−21​bTv.
  • Proposition 3.4.4 (p. 122): for t≥0t \ge 0t≥0, Complf(t)\mathrm{Compl}_f(t)Complf​(t) is finite iff Ct,f\mathcal C_{t,f}Ct,f​ is bounded below, and then −Complf(t)=min⁡vCt,f(v)-\mathrm{Compl}_f(t) = \min_v \mathcal C_{t,f}(v)−Complf​(t)=minv​Ct,f​(v).
  • Statement (O) (p. 124): with B(t)=2 [t1B1T;… ;tnBnT]B(t) = \sqrt2\,[\sqrt{t_1}B_1^T; \dots; \sqrt{t_n}B_n^T]B(t)=2​[t1​​B1T​;…;tn​​BnT​], the inequality 12vTA(t)v−fTv+τ≤0\tfrac12 v^TA(t)v - f^Tv + \tau \le 021​vTA(t)v−fTv+τ≤0 has no solution iff ∥(B(t)v; 1−fTv+τ)∥2≤1+fTv−τ\|(B(t)v;\ 1 - f^Tv + \tau)\|_2 \le 1 + f^Tv - \tau∥(B(t)v; 1−fTv+τ)∥2​≤1+fTv−τ has none.
  • Proposition 2.4.2 (pp. 61–62): for a pointed closed convex cone K\mathbf KK with nonempty interior, Ax−b∈KAx - b \in \mathbf KAx−b∈K is not almost solvable iff some λ∈K∗\lambda \in \mathbf K_*λ∈K∗​ has ATλ=0A^T\lambda = 0ATλ=0 and λTb>0\lambda^Tb > 0λTb>0 (with parts (i) and (ii)).
  • Statement (!!) (p. 125): for t≥0t \ge 0t≥0, Complf(t)<τ\mathrm{Compl}_f(t) < \tauComplf​(t)<τ iff the conic quadratic inequality above is not almost solvable.
  • Lemma 3.4.2 (p. 126): for t≥0t \ge 0t≥0, Complf(t)<τ\mathrm{Compl}_f(t) < \tauComplf​(t)<τ iff some λ∈Lk\lambda \in \mathbf L^kλ∈Lk has ATλ=0A^T\lambda = 0ATλ=0 and bTλ>0b^T\lambda > 0bTλ>0, for the explicit AAA, bbb of (3.4.49).
  • Lemma 3.4.3 (p. 127): for t≥0t \ge 0t≥0, Complf(t)<τ\mathrm{Compl}_f(t) < \tauComplf​(t)<τ iff some sis_isi​ satisfy ∑iBisi=f\sum_i B_is_i = f∑i​Bi​si​=f and ∑isiTsi/(2ti)<τ\sum_i s_i^Ts_i/(2t_i) < \tau∑i​siT​si​/(2ti​)<τ.

Significance

The proposition gives an explicit second-order cone description of the epigraph of the compliance, jointly in the design ttt and the load fff. Consequences: single-load, multiload and volume-constrained truss design problems become conic quadratic programs solvable by interior-point methods; the compliance is a convex function of (t,f)(t, f)(t,f); and the proposition contains a second variational principle (the reaction forces sis_isi​ minimize the stored energy subject to equilibrium, p. 128). It also explains the linear-programming formulation of Lecture 1.

The results are classical and proved in the book; none of them is machine-checked. A formalization adds checked statements of the variational principle for positive semidefinite quadratic forms, the conic theorem of the alternative for almost solvability, and a first instance of conic quadratic representability on the platform, with the 0/00/00/0 convention made explicit.

Difficulty

The compliance is defined through solvability of a singular linear system, so neither convexity nor any representation is visible from the definition. The equivalence in the goal must handle trusses with missing bars (ti=0t_i = 0ti​=0), where A(t)A(t)A(t) is singular and the convention a/0=+∞a/0 = +\inftya/0=+∞ matters, and loads outside the range of A(t)A(t)A(t), where the compliance is infinite. The book's route goes through a conic theorem of the alternative, which in the conic case characterizes only almost solvability, not solvability; passing from the strict epigraph to the non-strict one in the goal requires a separate attainment argument. A step-by-step translation must keep track of the perturbations of the right-hand side.

Formalization scope

Vectors are functions on finite index types (Fin m → ℝ, Fin n → ℝ, Fin (k i) → ℝ); the stacked inequality of (3.4.49) is indexed by the pairs (i,j)(i, j)(i,j), j<kij < k_ij<ki​, followed by two extra coordinates, the last of which is the distinguished coordinate of Lk\mathbf L^kLk. The compliance takes values in EReal: ⊤ exactly when A(t)v=fA(t)v = fA(t)v=f is unsolvable, and otherwise the real number 12fTv\tfrac12 f^Tv21​fTv; it only ever appears in comparisons with a real τ\tauτ. The convention 0/0=00/0 = 00/0=0, a/0=+∞a/0 = +\inftya/0=+∞ is encoded by requiring si=0s_i = 0si​=0 whenever ti=0t_i = 0ti​=0 together with Lean's real division; Lean's x/0=0x/0 = 0x/0=0 alone would let a missing bar carry any force, and this trivializing reading is ruled out. The CQr conclusion is not "some representation exists" in an unconstrained sense: it is a finite system of Lorentz-cone constraints Aj(x;u)−bj∈LmjA_j(x; u) - b_j \in \mathbf L^{m_j}Aj​(x;u)−bj​∈Lmj​, mj≥2m_j \ge 2mj​≥2, affine in the variables, exactly as on p. 86. Proposition 2.4.2 carries the book's standing assumptions: a pointed closed convex cone with nonempty interior, and Assumption A (full column rank of AAA, p. 53, in force by Remark 2.4.1).

Beyond the paper. One variant is posed: a strengthened Proposition 2.4.2 without Assumption A and on arbitrary finite index sets. Evidence: the systems involved depend on AAA only through its column space, so a basis of that space reduces the general case to the stated one. This is the form actually used on p. 126, where the matrix of (3.4.49) can fail Assumption A (for example t=0t = 0t=0, f=0f = 0f=0), a gap in the printed argument recorded as a finding.

Needed infrastructure: positive semidefinite quadratic forms and their minimization (Mathlib's Matrix.PosSemidef), dual cones and separation in finite dimension, the ice cream cone and its self-duality, and continuity of minimum values of quadratic forms under perturbation. The definitions of the Lorentz cone, CQr sets and functions, and almost solvability are reusable across the series. Proofs of individual milestones are welcome independently; Lemma 3.4.1 and statement (O) are self-contained.

Selected references

  • A. Ben-Tal, A. Nemirovski, Lectures on Modern Convex Optimization: Analysis, Algorithms, and Engineering Applications, MPS/SIAM Series on Optimization, SIAM, 2001. https://doi.org/10.1137/1.9780898718829
  • M. P. Bendsøe, O. Sigmund, Topology Optimization: Theory, Methods, and Applications, Springer, 2003. https://doi.org/10.1007/978-3-662-05086-6
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Lectures on Modern Convex Optimization II: The Conic Duality TheoremTextbook

Motivation

Linear, second-order cone and semidefinite programming are three instances of one format: minimize a linear objective subject to the requirement that an affine image of the decision vector lie in a fixed convex cone. Ben-Tal and Nemirovski's Lectures on Modern Convex Optimization (SIAM 2001) builds its whole treatment of modelling and algorithms on this conic programming format, and the first result it needs is a duality theorem for it. That theorem is what certifies optimality of a solution returned by an interior-point solver, what turns a robust or semidefinite reformulation into a tractable problem, and what every later lecture of the book uses when it passes to a dual problem. Conic duality in this form goes back to Nesterov and Nemirovski's monograph on interior-point methods (SIAM 1994); the Lagrangian form of the same phenomenon (Slater's condition) is the textbook version in Boyd and Vandenberghe (Cambridge 2004).

This mission is the second of a series formalizing the book's capstone results, and covers Lecture 2, §2.3–2.4.

Setting

Let K⊂Rm\mathbf K \subset \mathbb R^mK⊂Rm be a good cone: a nonempty set closed under addition and under multiplication by nonnegative reals (a convex cone), pointed (if a∈Ka \in \mathbf Ka∈K and −a∈K-a \in \mathbf K−a∈K then a=0a = 0a=0), closed, and with nonempty interior. Write a≥Kba \ge_{\mathbf K} ba≥K​b for a−b∈Ka - b \in \mathbf Ka−b∈K and a>Kba >_{\mathbf K} ba>K​b for a−b∈int⁡Ka - b \in \operatorname{int}\mathbf Ka−b∈intK. The dual cone is

K∗={λ∈Rm:λTa≥0  for all a∈K}.\mathbf K_* = \{\lambda \in \mathbb R^m : \lambda^T a \ge 0 \ \text{ for all } a \in \mathbf K\}.K∗​={λ∈Rm:λTa≥0  for all a∈K}.

Given an m×nm\times nm×n matrix AAA, b∈Rmb \in \mathbb R^mb∈Rm and c∈Rnc \in \mathbb R^nc∈Rn, the conic problem and its conic dual are

(CP)c∗=min⁡x{cTx∣Ax≥Kb},(D)b∗=max⁡λ{bTλ∣ATλ=c, λ≥K∗0}.\text{(CP)}\quad c^* = \min_x\{c^Tx \mid Ax \ge_{\mathbf K} b\}, \qquad \text{(D)}\quad b^* = \max_\lambda\{b^T\lambda \mid A^T\lambda = c,\ \lambda \ge_{\mathbf K_*} 0\}.(CP)c∗=xmin​{cTx∣Ax≥K​b},(D)b∗=λmax​{bTλ∣ATλ=c, λ≥K∗​​0}.

A point xxx is feasible for (CP) if Ax−b∈KAx - b \in \mathbf KAx−b∈K; (CP) is strictly feasible if Ax−b∈int⁡KAx - b \in \operatorname{int}\mathbf KAx−b∈intK for some xxx; it is bounded below if cTxc^TxcTx is bounded below on the feasible set (an infeasible problem counts as bounded below); it is solvable if some feasible xxx attains the infimum c∗c^*c∗. The same notions for (D) use ATλ=cA^T\lambda = cATλ=c, λ∈K∗\lambda \in \mathbf K_*λ∈K∗​, λ∈int⁡K∗\lambda \in \operatorname{int}\mathbf K_*λ∈intK∗​, and upper bounds. Throughout the book (from p. 53 on) Assumption A is in force: the columns of AAA are linearly independent.

Formalization targets

Goal: the conic duality theorem (Theorem 2.4.1, pp. 57–58)

Under the standing assumptions:

  1. (weak duality) cTx−bTλ≥0c^Tx - b^T\lambda \ge 0cTx−bTλ≥0 for every primal-dual feasible pair (x,λ)(x, \lambda)(x,λ);
  2. (3.a) if (CP) is bounded below and strictly feasible, then (D) is solvable and c∗=b∗c^* = b^*c∗=b∗;
  3. (3.b) if (D) is bounded above and strictly feasible, then (CP) is solvable and c∗=b∗c^* = b^*c∗=b∗;
  4. (4) if one of the problems is bounded and strictly feasible, a primal-dual feasible pair is optimal if and only if
bTλ=cTxand if and only ifλT(Ax−b)=0.b^T\lambda = c^Tx \qquad\text{and if and only if}\qquad \lambda^T(Ax - b) = 0.bTλ=cTxand if and only ifλT(Ax−b)=0.

Item 1 of the printed theorem (the dual of the dual is equivalent to the primal) is an informal equivalence of problems and is not part of the target.

Milestones

  • Theorem 2.3.1 (p. 52): K∗\mathbf K_*K∗​ is a closed convex cone; it is pointed if int⁡K≠∅\operatorname{int}K \ne \emptysetintK=∅; int⁡K∗≠∅\operatorname{int}K_* \ne \emptysetintK∗​=∅ if KKK is a closed convex pointed cone; and (K∗)∗=K(K_*)_* = K(K∗​)∗​=K for a closed convex cone KKK.
  • Proposition 2.3.1 (p. 52): the optimal value of (D) is a lower bound on that of (CP).
  • Theorem 2.4.2 (p. 58): two nonempty disjoint convex sets in Rm\mathbb R^mRm are separated by a nonzero linear functional.
  • Proposition 2.4.1 (p. 59): cTx−bTλ=(Ax−b)Tλc^Tx - b^T\lambda = (Ax - b)^T\lambdacTx−bTλ=(Ax−b)Tλ for every primal-dual feasible pair.
  • Corollary 2.4.1 (p. 60): if both problems are strictly feasible, both are solvable with equal optimal values, and zero gap and complementary slackness each characterize optimal pairs.
  • Proposition 2.4.2 (pp. 61–62): λ≥K∗0\lambda \ge_{\mathbf K_*} 0λ≥K∗​​0, ATλ=0A^T\lambda = 0ATλ=0, λTb>0\lambda^Tb > 0λTb>0 is solvable exactly when Ax−b≥K0Ax - b \ge_{\mathbf K} 0Ax−b≥K​0 is not almost solvable (not solvable for every arbitrarily small perturbation of bbb in ∥⋅∥2\|\cdot\|_2∥⋅∥2​).
  • Proposition 2.4.3 (p. 63): cTx≥dc^Tx \ge dcTx≥d follows from a strictly feasible Ax≥KbAx \ge_{\mathbf K} bAx≥K​b if and only if it is an admissible aggregation ATλ=cA^T\lambda = cATλ=c, λTb≥d\lambda^Tb \ge dλTb≥d, λ≥K∗0\lambda \ge_{\mathbf K_*} 0λ≥K∗​​0.

Beyond the book

One strengthened variant is posed beside the goal: items 2 and 3.a of Theorem 2.4.1 for every matrix AAA, without Assumption A (finding F3: the printed proof of 3.a never uses the rank of AAA). The faithful theorem remains the goal.

Significance

The theorem gives, for any of the cones used in practice (nonnegative orthant, Lorentz cones, positive semidefinite matrices and their products), the existence of a dual certificate of optimality and the absence of a duality gap under strict feasibility. The rest of the book uses it constantly: the conic-quadratic and semidefinite representations of Lectures 3–4, the S-lemma, the analysis of semidefinite relaxations and the primal-dual path-following method of Lecture 6 all pass to a dual problem through it. Propositions 2.4.2 and 2.4.3 are the conic analogues of the theorem on alternatives and the inhomogeneous Farkas lemma.

The result is classical and fully proved in the book. Related statements are machine-checked on the platform in other forms: a Lagrangian strong duality under a generalized Slater condition (ConvexOptimization.conic_slater_strong_duality), duality for equality-form conic quadratic programs (ConicQuadIPM.Homogeneous.*), and the bipolar theorem for proper cones. None of them is the pair (CP)/(D) of this book with attainment in both directions and the optimality conditions of item 4. The mission produces the book's statement and its supporting results as a coherent, reusable layer for the rest of the series.

Difficulty

Weak duality and the gap identity are one-line computations. The content lies in items 3.a and 3.b. The obvious attempt—copying the LP proof via Farkas' lemma—fails because the image of a nonpolyhedral cone under a linear map need not be closed, so a limit of dual certificates need not be a certificate. The book's Example 2.4.1 is strictly feasible and bounded below with optimal value 000 but no optimal solution, and Example 2.4.2 is solvable with an infeasible dual: any argument that does not use strict feasibility essentially is wrong. Separation is needed in finite dimension for convex sets that are neither open nor closed, which is not the form in which Mathlib states it, and item 3.b, which the book obtains from 3.a by symmetry, depends on the dual-cone facts of Theorem 2.3.1, including (K∗)∗=K(\mathbf K_*)_* = \mathbf K(K∗​)∗​=K and int⁡K∗≠∅\operatorname{int}\mathbf K_* \ne \emptysetintK∗​=∅.

Formalization scope

Vectors are Fin m → ℝ, matrices Matrix (Fin m) (Fin n) ℝ, inner products ⬝ᵥ; the topology is the product (Euclidean) topology. The cone properties, the dual cone, feasibility, strict feasibility, boundedness, optimal solutions and optimal values are explicit predicates in one definition file, ModernConvex.ConicDuality.ConicProblem. Optimal values are never a real-valued sInf/sSup: "vvv is the optimal value" is IsGLB/IsLUB of the set of feasible objective values, which no real satisfies for an infeasible or unbounded problem, and "c∗=b∗c^* = b^*c∗=b∗" is stated through an optimal solution whose value is the other problem's infimum or supremum. A formalization that dropped strict feasibility, or that expressed the optimal values as sInf/sSup with their junk value 000, would make the conic duality theorem either false or trivially true; the targets rule this out by stating attainment and value equality as explicit predicates. Assumption A is Function.Injective A.mulVec, an explicit hypothesis wherever the book has it in force, including Propositions 2.4.2–2.4.3 per the book's Remark 2.4.1.

Needed infrastructure: finite-dimensional separation of convex sets (Mathlib has geometric_hahn_banach_open and relatives for open sets; the nonopen finite-dimensional case goes through relative interiors), dual-cone facts (Mathlib's innerDualCone lives on inner-product spaces, while this mission works on Fin m → ℝ with the dot product), and closedness arguments for cones. The definitions and Theorem 2.3.1 are reusable by the later missions of this series. Proofs of individual milestones, and proofs or refutations of the variant, are welcome.

Selected references

  • A. Ben-Tal, A. Nemirovski, Lectures on Modern Convex Optimization: Analysis, Algorithms, and Engineering Applications, MPS/SIAM Series on Optimization, SIAM, 2001. https://doi.org/10.1137/1.9780898718829
  • Yu. Nesterov, A. Nemirovskii, Interior-Point Polynomial Algorithms in Convex Programming, SIAM Studies in Applied Mathematics, SIAM, 1994. https://doi.org/10.1137/1.9781611970791
  • S. Boyd, L. Vandenberghe, Convex Optimization, Cambridge University Press, 2004. https://web.stanford.edu/~boyd/cvxbook/
  • R. T. Rockafellar, Convex Analysis, Princeton University Press, 1970. https://doi.org/10.1515/9781400873173
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Lectures on Modern Convex Optimization III: The Convex Hull of Conic Quadratic Representable SetsTextbook

Motivation

Conic quadratic programs (second-order cone programs) minimize a linear objective subject to finitely many constraints of the form ∥Dx−d∥2≤pTx−q\|Dx - d\|_2 \le p^Tx - q∥Dx−d∥2​≤pTx−q. They are solved by interior-point methods in polynomial time, and a large share of convex models in engineering, statistics and robust optimization can be rewritten in this form. Whether a given convex problem can be so rewritten is a question about its feasible set and objective: can they be described by conic quadratic inequalities, possibly after adding auxiliary variables? Ben-Tal and Nemirovski answer this question in Lecture 3 of Lectures on Modern Convex Optimization (SIAM, 2001, doi:10.1137/1.9780898718829) with a calculus of conic quadratic representability: a list of elementary representable sets and functions together with operations that preserve representability, each operation producing an explicit representation from given ones. The same calculus underlies modelling tools such as CVX and YALMIP.

The more advanced operations in §3.3 — conic hulls, projective transformations, polars, Legendre transformations, convex hulls of unions and recessive cones — are only nearly representability-preserving: each holds exactly under a closedness or strict feasibility condition, and otherwise produces a set sandwiched between the target and its closure. The rule for convex hulls of unions is credited in the book to Nesterov.

Setting

For m≥2m \ge 2m≥2 the ice cream cone (Lorentz cone) is Lm={x∈Rm∣xm≥x12+⋯+xm−12}L^m = \{x \in \mathbb R^m \mid x_m \ge \sqrt{x_1^2 + \cdots + x_{m-1}^2}\}Lm={x∈Rm∣xm​≥x12​+⋯+xm−12​​}. Let K=Lm1×⋯×LmN\mathbf K = L^{m_1} \times \cdots \times L^{m_N}K=Lm1​×⋯×LmN​ be a direct product of ice cream cones, and write y≥K0y \ge_{\mathbf K} 0y≥K​0 for y∈Ky \in \mathbf Ky∈K and y>K0y >_{\mathbf K} 0y>K​0 for y∈int⁡Ky \in \operatorname{int}\mathbf Ky∈intK.

A set X⊂RnX \subset \mathbb R^nX⊂Rn is CQr (conic quadratic representable) if there are such a K\mathbf KK, a number ppp of additional variables and data A,B,bA, B, bA,B,b with

X={x∈Rn∣∃u∈Rp:Ax+Bu+b≥K0};X = \{x \in \mathbb R^n \mid \exists u \in \mathbb R^p : Ax + Bu + b \ge_{\mathbf K} 0\};X={x∈Rn∣∃u∈Rp:Ax+Bu+b≥K​0};

the system is a conic quadratic representation (CQR) of XXX. No rank condition is imposed on it. A function f:Rn→R∪{+∞}f : \mathbb R^n \to \mathbb R \cup \{+\infty\}f:Rn→R∪{+∞} is CQr when its epigraph Epi⁡{f}={(x,t)∣f(x)≤t}\operatorname{Epi}\{f\} = \{(x,t) \mid f(x) \le t\}Epi{f}={(x,t)∣f(x)≤t} is.

For X⊂RnX \subset \mathbb R^nX⊂Rn the mission uses the convex hull Conv⁡(X)\operatorname{Conv}(X)Conv(X) and its closure; the conic hull X+={(x,t):t>0, t−1x∈X}∪{0}⊂Rn+1X^+ = \{(x,t) : t > 0,\ t^{-1}x \in X\} \cup \{0\} \subset \mathbb R^{n+1}X+={(x,t):t>0, t−1x∈X}∪{0}⊂Rn+1 and its closure X^+\widehat X^+X+; the polar X∗={y∣yTx≤1 ∀x∈X}X_* = \{y \mid y^Tx \le 1\ \forall x \in X\}X∗​={y∣yTx≤1 ∀x∈X}; and the recessive cone Rec⁡(X)={h∣x+th∈X ∀x∈X,t≥0}\operatorname{Rec}(X) = \{h \mid x + th \in X\ \forall x \in X, t \ge 0\}Rec(X)={h∣x+th∈X ∀x∈X,t≥0}. For fff as above it uses the Legendre transformation f∗(y)=sup⁡x[yTx−f(x)]f_*(y) = \sup_x [y^Tx - f(x)]f∗​(y)=supx​[yTx−f(x)] and the projective transformation f^+\widehat f^+f​+, whose epigraph is the closure of {(x,t,s)∣s>0, s−1(x,t)∈Epi⁡{f}}\{(x,t,s) \mid s > 0,\ s^{-1}(x,t) \in \operatorname{Epi}\{f\}\}{(x,t,s)∣s>0, s−1(x,t)∈Epi{f}}.

Formalization targets

Goal: Proposition 3.3.5 (pp. 99–100)

Let X1,…,Xk⊂RnX_1, \dots, X_k \subset \mathbb R^nX1​,…,Xk​⊂Rn be nonempty convex CQr sets, Xi={x∣∃ui:Aix+Biui+bi≥Ki0}X_i = \{x \mid \exists u_i : A_ix + B_iu_i + b_i \ge_{\mathbf K_i} 0\}Xi​={x∣∃ui​:Ai​x+Bi​ui​+bi​≥Ki​​0}, and let

Y={x  ∣  ∃ξi,ti,ηi: Aiξi+Biηi+tibi≥Ki0, ti≥0 (i=1,…,k), ∑iξi=x, ∑iti=1}.Y = \Bigl\{x \;\Bigm|\; \exists \xi^i, t_i, \eta^i :\ A_i\xi^i + B_i\eta^i + t_ib_i \ge_{\mathbf K_i} 0,\ t_i \ge 0\ (i = 1,\dots,k),\ \textstyle\sum_i \xi^i = x,\ \sum_i t_i = 1\Bigr\}.Y={x​∃ξi,ti​,ηi: Ai​ξi+Bi​ηi+ti​bi​≥Ki​​0, ti​≥0 (i=1,…,k), ∑i​ξi=x, ∑i​ti​=1}.

Then

Conv⁡(⋃i=1kXi)⊂Y⊂cl⁡Conv⁡(⋃i=1kXi),\operatorname{Conv}\Bigl(\bigcup_{i=1}^k X_i\Bigr) \subset Y \subset \operatorname{cl}\operatorname{Conv}\Bigl(\bigcup_{i=1}^k X_i\Bigr),Conv(i=1⋃k​Xi​)⊂Y⊂clConv(i=1⋃k​Xi​),

and if (i) all XiX_iXi​ are closed and bounded, or (ii) Xi=Zi+WX_i = Z_i + WXi​=Zi​+W with ZiZ_iZi​ closed and bounded and WWW convex and closed, all three sets are equal and CQr.

Milestones

  1. Lemma 3.3.1 (p. 95): if Qv∈KQv \in \mathbf KQv∈K only when Qv=0Qv = 0Qv=0, then ∥Qv∥2≤C(1+∥Py+r∥2)\|Qv\|_2 \le C(1 + \|Py + r\|_2)∥Qv∥2​≤C(1+∥Py+r∥2​) on the solution set of Py+Qv+r≥K0Py + Qv + r \ge_{\mathbf K} 0Py+Qv+r≥K​0, and the projection {y∣∃v:Py+Qv+r≥K0}\{y \mid \exists v : Py + Qv + r \ge_{\mathbf K} 0\}{y∣∃v:Py+Qv+r≥K​0} is closed.
  2. Proposition 3.3.1 (p. 94): for nonempty CQr XXX, X+⊂X~+⊂X^+X^+ \subset \widetilde X^+ \subset \widehat X^+X+⊂X+⊂X+ with X~+={(x,t)∣t≥0,∃u:Ax+Bu+tb≥K0}\widetilde X^+ = \{(x,t) \mid t \ge 0, \exists u : Ax + Bu + tb \ge_{\mathbf K} 0\}X+={(x,t)∣t≥0,∃u:Ax+Bu+tb≥K​0}, with equality X~+=X^+\widetilde X^+ = \widehat X^+X+=X+ when Bu∈KBu \in \mathbf KBu∈K forces Bu=0Bu = 0Bu=0.
  3. Proposition 3.3.2 (p. 96): Epi⁡{f^+}={(x,t,s)∣s≥0,∃u:Ax+tp+Bu+sb≥K0}\operatorname{Epi}\{\widehat f^+\} = \{(x,t,s) \mid s \ge 0, \exists u : Ax + tp + Bu + sb \ge_{\mathbf K} 0\}Epi{f​+}={(x,t,s)∣s≥0,∃u:Ax+tp+Bu+sb≥K​0}.
  4. Proposition 3.3.3 (p. 97): under strict feasibility, X∗={y∣∃ξ:ATξ+y=0,BTξ=0,bTξ≤1,ξ≥K0}X_* = \{y \mid \exists \xi : A^T\xi + y = 0, B^T\xi = 0, b^T\xi \le 1, \xi \ge_{\mathbf K} 0\}X∗​={y∣∃ξ:ATξ+y=0,BTξ=0,bTξ≤1,ξ≥K​0}.
  5. Proposition 3.3.4 (p. 98): under strict feasibility, Epi⁡{f∗}={(y,s)∣∃ξ:ATξ=−y,BTξ=0,pTξ=1,s≥bTξ,ξ≥K0}\operatorname{Epi}\{f_*\} = \{(y,s) \mid \exists \xi : A^T\xi = -y, B^T\xi = 0, p^T\xi = 1, s \ge b^T\xi, \xi \ge_{\mathbf K} 0\}Epi{f∗​}={(y,s)∣∃ξ:ATξ=−y,BTξ=0,pTξ=1,s≥bTξ,ξ≥K​0}.
  6. Proposition 3.3.6 (p. 102): if Bu∈KBu \in \mathbf KBu∈K forces Bu=0Bu = 0Bu=0, then XXX is closed and Rec⁡(X)={h∣∃v:Ah+Bv≥K0}\operatorname{Rec}(X) = \{h \mid \exists v : Ah + Bv \ge_{\mathbf K} 0\}Rec(X)={h∣∃v:Ah+Bv≥K​0}.

Significance

The goal shows that a disjunction of conic quadratic constraints — "xxx lies in one of X1,…,XkX_1, \dots, X_kX1​,…,Xk​" — can be convexified exactly, under a compactness-type condition, by a conic quadratic system whose size is the sum of the sizes of the given representations. This is the conic quadratic analogue of Balas's disjunctive programming formulation for polyhedra and is the basis of perspective reformulations in mixed-integer conic optimization. The milestones are the other closure rules of the calculus: they let a modeller pass to conic hulls, perspectives, polars, conjugates and recession cones without leaving the conic quadratic class, always with an explicit representation.

These results are classical and proved in the book; none of them is formalized on the platform, and there is no formal library of conic quadratic representability. The mission produces that library's core definitions and its main closure theorems as machine-checked statements. Propositions 3.3.3 and 3.3.4 depend on conic duality, which a companion mission of this series (II: The Conic Duality Theorem) states.

Difficulty

The inclusions are not symmetric in difficulty. Conv⁡(⋃Xi)⊂Y\operatorname{Conv}(\bigcup X_i) \subset YConv(⋃Xi​)⊂Y is a direct substitution, but YYY contains points with some ti=0t_i = 0ti​=0, where the block inequality Aiξi+Biηi≥Ki0A_i\xi^i + B_i\eta^i \ge_{\mathbf K_i} 0Ai​ξi+Bi​ηi≥Ki​​0 no longer certifies membership in any XiX_iXi​; such points are only limits of convex combinations, and showing they lie in the closure requires the nonemptiness of every XiX_iXi​. The equality under (i) or (ii) is a closedness statement for a convex hull, which fails in general (two closed convex sets can have a non-closed convex hull of their union), so the compactness of the ZiZ_iZi​ must be used. Closedness of projections (Lemma 3.3.1) is the analogous obstacle in the milestones: the projection of a closed convex set is not closed in general.

Formalization scope

Vectors are Fin n → ℝ; the Euclidean norm is written out (eucNorm) because Mathlib's norm on this type is the sup norm. A product of ice cream cones is a structure IceCreamProduct with NNN factors of dimensions mj=dj+1≥2m_j = d_j + 1 \ge 2mj​=dj​+1≥2, its vectors indexed by (block, coordinate) pairs, the last coordinate of each block being the dominant one. cqrSet K A B b is the represented set and IsCQr X says XXX equals some cqrSet; the existential is over the fixed shape (finitely many Lorentz factors and an affine map), so an arbitrary set is not CQr by fiat. Pairs (x,t)(x,t)(x,t) of the conic hull are vectors of Fin (n+1) → ℝ with last coordinate ttt. Functions into R∪{+∞}\mathbb R \cup \{+\infty\}R∪{+∞} are EReal-valued and assumed never −∞-\infty−∞; the Legendre transformation is an EReal supremum, in which points with f(x)=+∞f(x) = +\inftyf(x)=+∞ contribute −∞-\infty−∞. Conv is convexHull ℝ, and closures are topological closures. Every "is CQr" conclusion is stated together with the book's explicit representation as an equality or sandwich of sets; stating "is CQr" alone would be a weaker theorem.

Beyond the paper. Proposition 3.3.2 as printed omits Epi⁡{f}≠∅\operatorname{Epi}\{f\} \neq \emptysetEpi{f}=∅ and is false for f≡+∞f \equiv +\inftyf≡+∞ (the right-hand side contains (0,0,0)(0,0,0)(0,0,0) while the left-hand side is empty; a Lean refutation of the formal statement was built during drafting). The faithful statement is kept as a milestone, and a corrected variant adds the missing hypothesis.

Reusable beyond this mission: the definitions of ice cream products, CQr sets, conic hull, polar, recessive cone and projective/Legendre transformations, and Lemma 3.3.1 as a closedness criterion. Contributions toward a general "closed projection" lemma and conic duality for products of Lorentz cones are welcome.

Selected references

  • A. Ben-Tal, A. Nemirovski, Lectures on Modern Convex Optimization: Analysis, Algorithms, and Engineering Applications, MPS/SIAM Series on Optimization, SIAM, 2001, §3.3, pp. 86–103. doi:10.1137/1.9780898718829
  • Yu. Nesterov, A. Nemirovski, Interior-Point Polynomial Algorithms in Convex Programming, SIAM Studies in Applied Mathematics, 1994. doi:10.1137/1.9781611970791
  • M. S. Lobo, L. Vandenberghe, S. Boyd, H. Lebret, Applications of second-order cone programming, Linear Algebra and its Applications 284 (1998), 193–228. doi:10.1016/S0024-3795(98)10032-0
  • E. Balas, Disjunctive programming: properties of the convex hull of feasible points, Discrete Applied Mathematics 89 (1998), 3–44. doi:10.1016/S0166-218X(98)00136-X
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Lectures on Modern Convex Optimization I: The Linear Programming Duality TheoremTextbook

Why linear programming duality

Every linear program comes with a second linear program, its dual, whose feasible points certify lower bounds on the first program's optimal value. The duality theorem says that these certificates are complete: the best bound equals the optimal value whenever either is finite. It is the reason an LP solver can return a proof of optimality alongside a solution, the basis of sensitivity analysis and of primal–dual algorithms, and the template for every duality theory in convex optimization.

This mission opens a series formalizing A. Ben-Tal and A. Nemirovski, Lectures on Modern Convex Optimization (SIAM 2001, doi:10.1137/1.9780898718829). Lecture 1 develops LP duality from a theorem on the alternative for mixed strict and non-strict linear inequalities, and proves that theorem from the homogeneous Farkas lemma by way of the theorems of Helly and Radon. Lecture 2 reruns the same argument for conic programs, so the statements here are the ones later missions of the series generalize.

Setting

Let A∈Rm×nA \in \mathbb R^{m\times n}A∈Rm×n have rows a1T,…,amTa_1^T, \dots, a_m^Ta1T​,…,amT​, and let b∈Rmb \in \mathbb R^mb∈Rm, c∈Rnc \in \mathbb R^nc∈Rn. Vector inequalities are componentwise. The LP program and its dual are

(LP)min⁡x{cTx∣Ax≥b},(LP∗)max⁡y{bTy∣ATy=c, y≥0}.\text{(LP)}\quad \min_x\{c^Tx \mid Ax \ge b\}, \qquad \text{(LP}^*)\quad \max_y\{b^Ty \mid A^Ty = c,\ y \ge 0\}.(LP)xmin​{cTx∣Ax≥b},(LP∗)ymax​{bTy∣ATy=c, y≥0}.

A point xxx with Ax≥bAx \ge bAx≥b is feasible, and (LP) is feasible if such a point exists. (LP) is bounded below if cTxc^TxcTx is bounded below on the feasible set. It is solvable if some feasible point minimizes cTxc^TxcTx. A real aaa is a lower bound on the optimal value c∗c^*c∗ if cTx≥ac^Tx \ge acTx≥a for every feasible xxx. The optimal value is c∗=inf⁡{cTx:Ax≥b}c^* = \inf\{c^Tx : Ax \ge b\}c∗=inf{cTx:Ax≥b}, which is +∞+\infty+∞ for an infeasible and −∞-\infty−∞ for an unbounded program. The same notions apply to the dual with "bounded above" and "maximizes". No rank condition is imposed on AAA.

The system on the alternative is

(S):aiTx>bi (i≤ms),aiTx≥bi (ms<i≤m),(\mathcal S):\quad a_i^Tx > b_i\ (i \le m_s),\qquad a_i^Tx \ge b_i\ (m_s < i \le m),(S):aiT​x>bi​ (i≤ms​),aiT​x≥bi​ (ms​<i≤m),

and its two certificate systems in λ∈Rm\lambda \in \mathbb R^mλ∈Rm are

TI: λ≥0, ∑iλiai=0, ∑iλibi≥0, ∑i≤msλi>0;TII: λ≥0, ∑iλiai=0, ∑iλibi>0.\mathcal T_{\rm I}:\ \lambda \ge 0,\ \textstyle\sum_i\lambda_ia_i = 0,\ \sum_i\lambda_ib_i \ge 0,\ \sum_{i\le m_s}\lambda_i > 0;\qquad \mathcal T_{\rm II}:\ \lambda \ge 0,\ \sum_i\lambda_ia_i = 0,\ \sum_i\lambda_ib_i > 0.TI​: λ≥0, ∑i​λi​ai​=0, ∑i​λi​bi​≥0, ∑i≤ms​​λi​>0;TII​: λ≥0, ∑i​λi​ai​=0, ∑i​λi​bi​>0.

In Lean, vectors are functions Fin n → ℝ, cTxc^TxcTx is c ⬝ᵥ x, and the definitions live in ModernConvex.LPDuality.LinearProgram and ModernConvex.LPDuality.AlternativeSystems.

Formalization targets

Goal: Theorem 1.3.2, the duality theorem in linear programming (p. 18)

  1. The duality is symmetric. Write (LP∗^*∗) as min⁡{−bTy∣A′y≥b′}\min\{-b^Ty \mid A'y \ge b'\}min{−bTy∣A′y≥b′} with A′=[Im;AT;−AT]A' = [I_m; A^T; -A^T]A′=[Im​;AT;−AT] and b′=(0;c;−c)b' = (0; c; -c)b′=(0;c;−c). The dual of this program, in w=(ξ,η,ζ)w = (\xi, \eta, \zeta)w=(ξ,η,ζ), is mapped onto (LP) by x=ζ−ηx = \zeta - \etax=ζ−η, with objective b′Tw=−cTxb'^Tw = -c^Txb′Tw=−cTx.
  2. Weak duality. bTy≤cTxb^Ty \le c^TxbTy≤cTx for every primal feasible xxx and dual feasible yyy.
  3. Strong duality. The following are equivalent: (i) the primal is feasible and bounded below; (ii) the dual is feasible and bounded above; (iii) the primal is solvable; (iv) the dual is solvable; (v) both are feasible. When they hold, there is a real vvv with
v=inf⁡{cTx∣Ax≥b}=sup⁡{bTy∣ATy=c, y≥0}.v = \inf\{c^Tx \mid Ax \ge b\} = \sup\{b^Ty \mid A^Ty = c,\ y \ge 0\}.v=inf{cTx∣Ax≥b}=sup{bTy∣ATy=c, y≥0}.

Milestones, in the book's order of proof

  • Theorem 1.4.3 (Radon, p. 38): any m≥n+2m \ge n+2m≥n+2 points of Rn\mathbb R^nRn split into two nonempty parts whose convex hulls meet.
  • Theorem 1.4.2 (Helly, p. 37): if every k≤n+1k \le n+1k≤n+1 of finitely many convex sets in Rn\mathbb R^nRn have a common point, then all of them do.
  • Lemma 1.4.1 (homogeneous Farkas lemma, p. 34): the system aTx<0, aiTx≥0a^Tx < 0,\ a_i^Tx \ge 0aTx<0, aiT​x≥0 is infeasible if and only if a=∑iλiaia = \sum_i\lambda_ia_ia=∑i​λi​ai​ for some λ≥0\lambda \ge 0λ≥0.
  • Proposition 1.3.1 (pp. 13–14): if TI\mathcal T_{\rm I}TI​ or TII\mathcal T_{\rm II}TII​ is solvable, then (S)(\mathcal S)(S) is infeasible.
  • Theorem 1.3.1 (general theorem on the alternative, p. 14): (S)(\mathcal S)(S) is infeasible if and only if TI\mathcal T_{\rm I}TI​ or TII\mathcal T_{\rm II}TII​ is solvable.
  • Proposition 1.3.2 (p. 17): the solutions (y,a)(y, a)(y,a) of y≥0y \ge 0y≥0, ATy=cA^Ty = cATy=c, bTy≥ab^Ty \ge abTy≥a give exactly the lower bounds aaa on the optimal value of a feasible (LP).
  • Proposition 1.3.3 (p. 17): bTyb^TybTy is a lower bound on c∗c^*c∗ for every dual feasible yyy, and when (LP) is feasible, every a≤c∗a \le c^*a≤c∗ is dominated by some bTyb^TybTy.
  • Theorem 1.4.1 (Bernshtein, p. 31): ∥f′∥∞≤k∥f∥∞\|f'\|_\infty \le k\|f\|_\infty∥f′∥∞​≤k∥f∥∞​ on [0,2π][0, 2\pi][0,2π] for every trigonometric polynomial fff of degree ≤k\le k≤k. This milestone is off the duality path. The book uses it to bound the grid size when uniform approximation is discretized.

Significance

LP duality underlies most of the book's later material. The conic duality theorem of Lecture 2 has the same statement with the nonnegative orthant replaced by a cone. Robust counterparts, the S-lemma and the semidefinite relaxations of Lecture 4 are all proved by dualizing an inner problem. A machine-checked version in exactly this form, with explicit predicates for "bounded" and "solvable", is the base that later missions of the series can cite.

The results here are classical and proved. The platform already has proved LP duality theorems, in other standard forms: LinearOptimization.lp_strong_duality (general form with equalities), MatousekLP.Duality.duality_theorem (max/≤\le≤ form, four-case statement) and VanderbeiLP.StrictComp.strong_duality. It has Farkas lemmas in several forms (LinearOptimization.farkas_cone_corollary, which is one direction of Lemma 1.4.1, and MatousekLP.Duality.farkas_geometric). It also has Helly and Radon in Mathlib's form (FamousTheorems.helly_theorem, which assumes at least dim⁡+1\dim + 1dim+1 sets and subfamilies of size exactly dim⁡+1\dim + 1dim+1; FamousTheorems.radon_theorem, which assumes affine dependence). The open MangasarianFJ.GenFJ.motzkin_transposition is a related alternative theorem. None of them states the book's inequality-form pair (LP)/(LP∗^*∗), the five-way equivalence, or the mixed strict/non-strict theorem on the alternative. These are the remaining work. Several of them should follow quickly from the existing items, and solvers are encouraged to reuse them.

Difficulty

The obstacle is the existence of certificates of infeasibility. Proposition 1.3.1 is a one-line computation, but its converse, Theorem 1.3.1, is not: the existence of a certificate is a global statement about the system that no local computation produces. The mixed system needs care: when ms=0m_s = 0ms​=0 only TII\mathcal T_{\rm II}TII​ can certify, and the homogenization that reduces Theorem 1.3.1 to the Farkas lemma has to keep strict and non-strict rows apart. In the duality theorem, the step from "feasible and bounded below" to "solvable" is where attainment must be shown. It is true for LPs and false for general convex programs (min⁡{1/x∣x≥1}\min\{1/x \mid x \ge 1\}min{1/x∣x≥1}), so a proof cannot avoid the linear structure.

The book's own proof of item 1 has a sign slip. The displayed dual of the rewritten (LP∗^*∗) has the constraint ξ−Aη+Aζ=−b\xi - A\eta + A\zeta = -bξ−Aη+Aζ=−b with x=η−ζx = \eta - \zetax=η−ζ, which describes max⁡{cTx∣Ax≥b}\max\{c^Tx \mid Ax \ge b\}max{cTx∣Ax≥b} rather than a program equivalent to (LP). The formal statement uses the correct computation, ξ+Aη−Aζ=−b\xi + A\eta - A\zeta = -bξ+Aη−Aζ=−b with x=ζ−ηx = \zeta - \etax=ζ−η.

Formalization scope

Vectors are Fin n → ℝ. Indices are 0-based, so the strict rows of (S)(\mathcal S)(S) are i < ms, and ms ≤ m is a hypothesis. Optimal values are never written as sInf/sSup, whose junk value 000 on empty or unbounded sets would make the equal-values clause trivially true. A lower bound is the predicate ∀x, Ax≥b⇒a≤cTx\forall x,\ Ax \ge b \Rightarrow a \le c^Tx∀x, Ax≥b⇒a≤cTx. "vvv is the optimal value" is IsGLB/IsLUB of the set of objective values, which no real satisfies for an infeasible or unbounded program. Item 1 of the goal is not formalized as True. It states the explicit feasible-set correspondence that "equivalent" means in the book's proof. The five properties are a List.TFAE.

In Bernstein's theorem the sup-norm inequality is stated as "every bound MMM on ∣f∣|f|∣f∣ over [0,2π][0, 2\pi][0,2π] gives the bound kMkMkM on ∣f′∣|f'|∣f′∣". Coefficients are complex, which covers the real case.

The book prints the trigonometric polynomial as a0+∑l=1k[a0cos⁡(lt)+b0sin⁡(lt)]a_0 + \sum_{l=1}^k[a_0\cos(lt) + b_0\sin(lt)]a0​+∑l=1k​[a0​cos(lt)+b0​sin(lt)], with the same two coefficients in every term. This is a subscript typo: the theorem is stated for every trigonometric polynomial of degree ≤k\le k≤k, and its own tightness example cos⁡(kt)\cos(kt)cos(kt) is not of the printed form for k≥2k \ge 2k≥2. The formal statement uses general coefficients al,bla_l, b_lal​,bl​.

A complete development needs only Mathlib's finite-dimensional linear algebra and convexity (convexHull, Convex). The definitions of the LP pair and of the alternative systems are reusable by any later mission that dualizes a linear inner problem.

Selected references

  • A. Ben-Tal, A. Nemirovski, Lectures on Modern Convex Optimization: Analysis, Algorithms, and Engineering Applications, MPS/SIAM Series on Optimization, SIAM, 2001. doi:10.1137/1.9780898718829
  • J. Farkas, Theorie der einfachen Ungleichungen, J. Reine Angew. Math. 124 (1902), 1–27. doi:10.1515/crll.1902.124.1
  • E. Helly, Über Mengen konvexer Körper mit gemeinschaftlichen Punkten, Jahresber. Dtsch. Math.-Ver. 32 (1923), 175–176. eudml:145659
  • J. Radon, Mengen konvexer Körper, die einen gemeinsamen Punkt enthalten, Math. Ann. 83 (1921), 113–115. doi:10.1007/BF01464231
  • A. Schrijver, Theory of Linear and Integer Programming, Wiley, 1986 (Ch. 7, the theorems on the alternative and LP duality). ISBN 978-0-471-98232-6
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🏆Completed
Complexity TheoryTheoretical Computer Science·Captain: marwahaha

Integer multiplication: κ = 1/2^129Open Problem

Motivation

Multiplying two binary integers is a basic task in computational complexity. The relevant resource here is the number of individual steps made by a machine whose tapes can only be accessed through moving heads. Harvey and van der Hoeven established an O(nlog⁡n)O(n\log n)O(nlogn) bound in this model. The OpenAI manuscript proposes a positive saving in the exponent of the logarithm. Subsequent constructions explore larger savings. The formalization target is the complete computation and its time bound, including the analytic and implementation arguments needed to connect a finite construction to every input length.

Setting

A deterministic multitape Turing machine has a fixed finite alphabet, a fixed finite state set, and a fixed finite number of tapes. Each tape extends in one direction and has one head. A step reads the symbols under the heads, changes state, writes at those positions, and moves each head by at most one cell. The alphabet contains distinct blank, start-marker, zero, one, and separator symbols. Tape zero is the read-only input tape; tape one is the output tape; further tapes are available for work. The halting state freezes the configuration.

An input consists of two bit strings x,yx,yx,y of the same positive length nnn, separated by #\##. The strings are read most significant bit first, with leading zeros permitted. If val⁡(x)\operatorname{val}(x)val(x) denotes the represented natural number, the required output is exactly the 2n2n2n-bit binary representation of val⁡(x)val⁡(y)\operatorname{val}(x)\operatorname{val}(y)val(x)val(y), padded with leading zeros and followed by blanks. All tapes begin with a preserved start marker. Define L(n)=max⁡(⌈log⁡2n⌉,1)L(n)=\max(\lceil\log_2 n\rceil,1)L(n)=max(⌈log2​n⌉,1).

Target

The full target is

IntMul.KappaBound(value).\mathrm{IntMul.KappaBound}({{value}}).IntMul.KappaBound(value).

This asserts the existence of one machine that computes the exact product correctly for every positive input length, together with constants c>0c>0c>0 and n0n_0n0​ such that every pair of nnn-bit inputs, for n≥n0n\ge n_0n≥n0​ and n≥1n\ge1n≥1, halts within

c n L(n)1−valuec\,n\,L(n)^{1-{{value}}}cnL(n)1−value

steps. Constants, alphabet, states, and tape count are independent of the input length. The number is an exact real value. Larger κ\kappaκ gives a stronger asymptotic saving because L(n)≥1L(n)\ge1L(n)≥1.

Each entry supplies its own exact numerical value and identifies the construction that motivates it. Historical and new entries use the same machine definition. A proposed value may be recorded while its complete proof is still open; it becomes a proved record only when the goal has a verified proof. Numerical certificates are supporting results with their own scope, and do not establish a complete machine time bound.

Significance

A proof for any positive value would give a strict asymptotic improvement over nlog⁡nn\log nnlogn. Such an improvement would contradict the proposed Ω(nlog⁡n)\Omega(n\log n)Ω(nlogn) lower bound, while remaining consistent with the known upper bound. The tracked value concerns asymptotic growth; it does not measure the runtime of a practical implementation. No claim about a currently fastest implementation follows from a larger saving.

Formalizing the full target connects exact finite calculations to a uniform algorithm. The community repository explicitly treats the original framework and remaining all-size interfaces as assumptions of its current evidence. In this mission those steps must be proved before the goal can be marked Proved. They are not added as hypotheses that would weaken the full target. Earlier published theorem statements and finite certificates may be reused with their original attribution and proof status.

Difficulty

A finite network certificate can establish a concrete role count or a rational margin, but does not itself supply a machine for every input length. A complete proof must establish correctness of the recursive construction, admissibility of its parameters, precision and error guarantees, and the cost of moving data on tapes. Counts of algebraic operations alone do not account for this last resource. The difficult connection is between these separate contracts and the single uniform machine quantified by the goal.

Formalization scope

The goal imports the existing public Definitions.Def_IntMul_MultitapeModel bundle and uses IntMul.KappaBound directly. No alternative machine or cost model is introduced. Natural numbers describe input lengths, head positions, and step counts; real numbers describe the asymptotic constant and exponent. The real power has base at least one. Correctness is required even below the asymptotic threshold. Inputs of length zero and malformed inputs are outside the specified task.

The input and output conventions exclude a machine that merely decides a predicate about the product. The entire output tape must contain the required product and then blanks. Neither failure to halt nor correctness on a finite collection of test inputs meets the target. The work tapes and final head positions are unconstrained. Reusable contributions include machine composition with explicit costs, exact encodings, analytic estimates, and proofs that the finite certificates imply the contracts required by the recursive algorithm. Every such contribution should state its own assumptions and conclusion explicitly.

Selected references

  • D. Harvey and J. van der Hoeven, Integer multiplication in time O(n log n), Annals of Mathematics 193(2), 563–617 (2021). Paper.
  • OpenAI, Integer multiplication below n log n, preprint (23 September 2026), pinned manuscript revision adc7f1241b42e322a6451854ab7e4b4c146bf78a. Source.
  • D. Colkitt and community contributors, A sharper exponent for integer multiplication, research repository (2026), revision 56b66d58297deca1d7dd130247d720e960f77a37. Checkpoint and attribution.
2 thms2 active usersReviewed
Quantum Information·Captain: Goku

Schwartz operatorsResearch Paper

Motivation

In this paper we introduce Schwartz operators as a non-commutative analog of Schwartz functions and provide a detailed discussion of their properties. We equip them in particular with a number of different (but equivalent) families of seminorms which turns the space of Schwartz operators into a Frechet space. The study of the topological dual leads to non-commutative tempered distributions which are discussed in detail as well. We show in particular that the latter can be identified with a certain class of quadratic forms, therefore making operations like products with bounded (and also some unbounded) operators and quantum harmonic analysis available to objects which are otherwise too singular for being a Hilbert space operator. Finally we show how the new methods can be applied by studying operator moment problems and convergence properties of fluctuation operators.

This mission is the statement-level formalization of Schwartz operators (arXiv:1503.04086v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

10 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is The form topology makes Schwartz operators a Frechet space (Proposition 3.3, PDF p. 11). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

51 results of the paper are not stated yet, because the library lacks an interface they need:

  • Proposition 2.3: Canonical Hermite basis in L2 and Schwartz space, and finite-subset expansions (hard)
  • Proposition 2.4: Schwartz algebraic tensor injection and its Hilbert tensor identification (hard)
  • Lemma 2.6: Hilbert structure on the actual Hilbert--Schmidt ideal, kernel unitary and Hermite matrix unitary (hard)
  • Lemma 2.7: HS-to-scaled-phase-L2 Weyl unitary with the U(id tensor F*)V kernel factorization (hard)
  • Lemma 3.5: Full singular-value decomposition interface and continuous adjoint/composition on the form topology (hard)
  • Proposition 3.7: Actual L2 kernels and Hermite coefficient maps with Schwartz onto homeomorphisms (hard)
  • Proposition 3.8: Hermite matrix units as Schwartz operators and unordered finite-subset expansions (hard)
  • Proposition 3.10: Canonical maximal Q/P and oscillator domains, Hermite weights and all three one-sided topologies (hard)
  • Proposition 3.11: Adjoints of natural right products, their bounded extensions, and right-range oscillator/matrix topologies (hard)
  • Proposition 3.13: Densely defined adjoints, graph closure and natural products with a Schwartz operator (hard)
  • Proposition 3.14: Closure of the ordered natural-domain product ATB* (hard)
  • Corollary 3.16: Actual singular-value sequences for compact operators and dyadic-power summability (hard)
  • Corollary 3.17: Complex trace pairing and closures of TA and AT for unbounded A (hard)
  • Proposition 3.18: Concrete full HS Weyl transform and its Schwartz restriction homeomorphism (hard)
  • Lemma 3.19: Ground-projection operator convolution as a Schwartz-valued map with dense range (hard)
  • Corollary 3.20: Both-sided oscillator relative boundedness and unbounded trace cycling (hard)
  • Proposition 3.21: Proposition 3.21 source-convention decision (source-ambiguity)
  • Proposition 3.24: Source O_MR/O_ML multiplier classes with canonical oscillator domains (hard)
  • Proposition 3.25: Proposition 3.25 source-convention decision (source-ambiguity)
  • Proposition 4.2: Analytic moments, arbitrary canonical words, and HS norms of R^A sqrt(T) (hard)
  • Proposition 4.3: Minimal purification, amplified canonical domains and analytic-vector span (hard)
  • Theorem 4.4: Actual canonical polynomial moment traces and independent analytic Schwartz predicate (hard)
  • Proposition 5.1: Complex-linear weak-* dual of the form Schwartz space and concrete transpose isomorphisms (hard)
  • Proposition 5.2: Weak-* coefficient reconstruction with the trace-pairing transposition correction (source-ambiguity)
  • Proposition 5.3: Weak-* dual precomposition operations for all listed source multipliers and derivatives (hard)
  • Proposition 5.4: Source-reflected transpose Fourier/Weyl/quantization transforms on weak duals (hard)
  • Proposition 5.6: Proposition 5.6 source-convention decision (source-ambiguity)
  • Proposition 5.7: Weak Weyl-translation derivative of parity and quantization of delta derivatives (hard)
  • Proposition 5.8: All four allowed distribution/Schwartz convolution maps and weak-* topologies (hard)
  • Proposition 5.9: All concrete reflected Fourier/Weyl distribution-convolution identities (hard)
  • Proposition 5.10: Weak-dual convolution by the actual oscillator ground projection (hard)
  • Proposition 5.12: Complex trace sandwich distributions and full HS regularity representation (hard)
  • Proposition 5.15: Sesquilinear kernel theorem with oscillator inverse powers and both weak-dual bijections (hard)
  • Theorem 5.16: Two-sided polynomially bounded operator distributions and finite derivative representation (hard)
  • Proposition 5.17: Fixed-weight Hermite-diagonal finite-rank cutoffs and weak-* precomposition limits (hard)
  • Proposition 6.1: Position spectral densities as distributions with actual kernel and normalized Wigner maps (hard)
  • Corollary 6.2: Complex spectral trace and diagonal of the actual Schwartz kernel (hard)
  • Proposition 6.3: Constructed symmetric-spin/Hermite canonical approximants and distribution traces (hard)
  • Proposition 6.4: Actual spectral measures of the embedded spin approximants and their complex trace measures (hard)
  • Corollary 6.5: Common shrinking-interval and positive-spin sequences for all Schwartz trace tests (hard)
  • SchattenSeminormTopology: Weighted-product trace norms and tuple-oscillator trace-class estimate (hard)
  • OscillatorSeminormTopology: Tuple and total-oscillator powers on their actual domains and two HS seminorm topologies (hard)
  • SchwartzConvolutionContinuity: Both classical/quantum Schwartz convolution maps with an arbitrary fixed Schwartz operator (hard)
  • WignerWeylCorrespondence: Full source-normalized Weyl quantization and Wigner homeomorphisms, traces and kernel (hard)
  • DifferentialConvolutionIdentities: DifferentialConvolutionIdentities source-convention decision (source-ambiguity)
  • OperatorsAsDistributions: Complex trace embeddings of all operator ideals and one-/two-sided unbounded Schwartz restrictions (hard)
  • DeltaWeylCorrespondence: All shifted-delta transpose transforms and parity/Weyl operator distributions (hard)
  • PositiveCorrespondence: Translation actions, weak-dual positivity and both positive convolution correspondences (hard)
  • Remark 5.13: Bounded-operator version of the full polynomial-sandwich distribution representation (hard)
  • DeltaParityApproximation: Actual quantized scaled Gaussian symbols and weak-dual parity approximation (hard)
  • Section 5.5.1, scaled approximate identity: Classical and operator weak-* approximate-identity convolution interfaces (hard)

Selected references

  • Schwartz operators, arXiv:1503.04086v1, https://arxiv.org/abs/1503.04086v1
13 thms2 active usersReviewed
Quantum Information·Captain: Goku

Relating quantum privacy and quantum coherence: an operational approachResearch Paper

Motivation

We describe how to achieve optimal entanglement generation and one-way entanglement distillation rates by coherent implementation of a class of secret key generation and secret key distillation protocols, respectively. This short paper is a high-level descrioption of our detailed papers [8] and [10].

This mission is the statement-level formalization of Relating quantum privacy and quantum coherence: an operational approach (arXiv:quant-ph/0307053v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

8 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Coherent information is achievable in all four resource conversions (Conclusion; scenarios 1–4, PDF p. 4). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

2 results of the paper are not stated yet, because the library lacks an interface they need:

  • Equation (2), PA sets; size assertion continues on p.3: A distinct uniform PA subset with the printed IID environmental reference, with its finite-size and typical-set conventions fixed. (source-ambiguity)
  • Every-l,t Fourier-code substitution claim and footnote [16]: A complete arbitrary-source l,t coherent code family with specified finite branch law and uniformly good ancillary decoupling, sufficient for any claimed real-message coherification premise. (source-ambiguity)

Selected references

  • Relating quantum privacy and quantum coherence: an operational approach, arXiv:quant-ph/0307053v1, https://arxiv.org/abs/quant-ph/0307053v1
17 thms2 active usersReviewed
🏆Completed
Quantum Information·Captain: Goku

Classical feedback for quantum channelsResearch Paper

Motivation

We investigate whether the use of a noiseless, classical feedback channel will increase the capacity of a quantum discrete memoryless channel to transmit classical information. This problem has been previously analyzed by Bowen and Nagarajan for the case of protocols restricted to product input states. They showed that feedback did not increase the information capacity. In this paper we introduce a quantum analogue of classical causality and prove a capacity theorem (in regularized form) for the transmission of classical information.

This mission is the statement-level formalization of Classical feedback for quantum channels (arXiv:quant-ph/0409207v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

1 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Whole-codeword Markov property of the executed feedback protocol (§2, paragraph continuing PDF p.5, PDF p. 6). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

6 results of the paper are not stated yet, because the library lacks an interface they need:

  • Theorem 2 (announced in Abstract): regularized classical-feedback capacity: An unambiguous corrected operational error, causal execution and capacity regularization (source-ambiguity)
  • Lemma 1: Directed Data Processing Inequality: A source-supported prefix sufficiency condition or a different directed-information object (source-ambiguity)
  • §3 and §5, unnumbered: double-block random-coding error and vanishing-error existence: A physical collective decoder, correct history probabilities and uniformly decaying error parameters (source-ambiguity)
  • §4, unnumbered: recovery of the usual unassisted classical-capacity formula: The exact no-feedback restriction and resulting entropic reduction (source-ambiguity)
  • Lemma 3: disturbance bound for the inserted collective measurements: A specified conditional disturbance theorem with valid postselection control and timing (source-ambiguity)
  • Lemma 4: the two printed typical-projector estimates: Corrected typical-projector conclusions and quantified constants (source-ambiguity)

Selected references

  • Classical feedback for quantum channels, arXiv:quant-ph/0409207v3, https://arxiv.org/abs/quant-ph/0409207v3
5 thms2 active usersReviewed
Quantum Information·Captain: Goku

Maximum likelihood estimation for a group of physical transformationsResearch Paper

Motivation

The maximum likelihood strategy to the estimation of group parameters allows to derive in a general fashion optimal measurements, optimal signal states, and their relations with other information theoretical quantities. These results provide a deep insight into the general structure underlying optimal quantum estimation strategies. The entanglement between representation spaces and multiplicity spaces of the group action appear to be the unique kind of entanglement which is really useful for the optimal estimation of group parameters.

This mission is the statement-level formalization of Maximum likelihood estimation for a group of physical transformations (arXiv:quant-ph/0507007v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

14 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Optimal input states and the likelihood ceiling (Theorem 3 (optimal input states), Eqs.(24)–(25); capstone selected from the p.1 abstract, PDF p. 10). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

10 results of the paper are not stated yet, because the library lacks an interface they need:

  • §2.5 Remark I: claimed uniqueness iff the orbit is spanning: §2.5 Remark I: claimed uniqueness iff the orbit is spanning — a valid source-supported domain or correction (source-ambiguity)
  • §4.1: general extension of the optimal-POVM theorem to infinite dimension: §4.1: general extension of the optimal-POVM theorem to infinite dimension — a valid source-supported domain or correction (source-ambiguity)
  • §4.2: blanket extension of Theorems 1, 2 and 3 via formal dimensions: §4.2: blanket extension of Theorems 1, 2 and 3 via formal dimensions — a valid source-supported domain or correction (source-ambiguity)
  • Proposition 1: noncompact discrete-series group average, Eqs.(35)–(36): Proposition 1: noncompact discrete-series group average, Eqs.(35)–(36) — a valid source-supported domain or correction (source-ambiguity)
  • §4.3.1, Eqs.(38)–(40): identical-displacement decomposition and formal dimension: Completed two-mode Fock Weyl action, corrected passive 50:50 rotation, invariant infinite-multiplicity subspaces, and coefficient-square Haar integrability. (hard)
  • §4.3.1: optimal POVMs and likelihood for two identical coherent states, Eqs.(41)–(43): Normalized positive-form POVMs, their integrated bounded operator measures, and links to the joint quadrature and heterodyne-average measurements. (hard)
  • §4.3.1 Remark: squeezing improves likelihood, Eqs.(44)–(45): Normalized full-Fock squeezed vectors and the weakly normalized optimal covariant diagonal-sum measurement on them. (hard)
  • §4.3.2, Eqs.(47)–(49): conjugate-displacement spectral decomposition: Concrete Weyl/Plancherel unitary from completed two-mode Fock space to L2(C,d^2beta/pi), with its action intertwining and full commutant characterization. (hard)
  • Proposition 2: direct-integral group average for conjugate displacements, Eq.(50): Proposition 2: direct-integral group average for conjugate displacements, Eq.(50) — a valid source-supported domain or correction (source-ambiguity)
  • §4.3.2: unique optimal covariant POVM and Gaussian law, Eqs.(52)–(56): Positive seed form for constant spectral wavefunction, its normalized integrated operator measure, full-support uniqueness and actual Born Gaussian law. (hard)

Selected references

  • Maximum likelihood estimation for a group of physical transformations, arXiv:quant-ph/0507007v1, https://arxiv.org/abs/quant-ph/0507007v1
19 thms2 active usersReviewed
Quantum Information·Captain: Goku

Optimal estimation of group transformations using entanglementResearch Paper

Motivation

We derive the optimal input states and the optimal quantum measurements for estimating the unitary action of a given symmetry group, showing how the optimal performance is obtained with a suitable use of entanglement. Optimality is defined in a Bayesian sense, as minimization of the average value of a given cost function. We introduce a class of cost functions that generalizes the Holevo class for phase estimation, and show that for states of the optimal form all functions in such a class lead to the same optimal measurement. A first application of the main result is the complete proof of the optimal efficiency in the transmission of a Cartesian reference frame. As a second application, we derive the optimal estimation of a completely unknown two-qubit maximally entangled state, provided that N copies of the state are available. In the limit of large N, the fidelity of the optimal estimation is shown to be 1-3/(4N).

This mission is the statement-level formalization of Optimal estimation of group transformations using entanglement (arXiv:quant-ph/0506267v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

13 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem 1: optimal canonical input states (Theorem 1, PDF p. 4). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

1 results of the paper are not stated yet, because the library lacks an interface they need:

  • §IV B final paragraph: A specified local parameter chart, locally unbiased estimator comparison class, and a theorem linking its local asymptotic risk to this particular covariant Bayes estimator. (source-ambiguity)

Selected references

  • Optimal estimation of group transformations using entanglement, arXiv:quant-ph/0506267v2, https://arxiv.org/abs/quant-ph/0506267v2
17 thms2 active usersReviewed
🏆Completed
Quantum Information·Captain: Goku

Noncommutative maximal ergodic theoremsResearch Paper

Motivation

This paper is devoted to the study of various maximal ergodic theorems in noncommutative LpL_pLp​-spaces. In particular, we prove the noncommutative analogue of the classical Dunford-Schwartz maximal ergodic inequality for positive contractions on LpL_pLp​ and the analogue of Stein's maximal inequality for symmetric positive contractions. We also obtain the corresponding individual ergodic theorems. We apply these results to a family of natural examples which frequently appear in theory of von Neumann algebras and in quantum probability.

This mission is the statement-level formalization of Noncommutative maximal ergodic theorems (arXiv:math/0505308v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

1 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Operator block matrix norm comparison (Lemma 3.2, PDF p. 13). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

62 results of the paper are not stated yet, because the library lacks an interface they need:

  • Theorem 0.1: positive Dunford–Schwartz and symmetric-power maximal inequalities: semifinite trace; tracial Lp; compatible Lp extensions; discrete Cesaro average; maximal factorization norm (hard)
  • Theorem 0.2: introductory c0 convergence assertion: Unambiguous corrected full source assertion: Theorem 0.2: introductory c0 convergence assertion (source-ambiguity)
  • Theorem 0.3: free-group Poisson maximal inequality and radial convergence: free group von Neumann algebra; word-length Poisson semigroup; tracial Lp; maximal factorization norm; tracial b.a.u. and a.u. convergence (hard)
  • Lemma 1.1: compatible positive contractive Lp extensions and normality: finite-trace support ideal; tracial Lp; normality; compatible Lp extensions (hard)
  • Proposition 2.1: decomposition, finite truncations, duality and Cauchy–Schwarz: maximal factorization norm; ell1 factorization space; finite truncation; conjugate exponent; trace pairing (hard)
  • Remark 2.2: attained factorization norms, c0 duality, and failure of modulus stability: attained factorization norm; finite factorization ell1^0; ell1 factorization space; c0 factorization space; Banach dual; coordinate modulus (hard)
  • Remark 2.3: trace-compatible subalgebra inclusions: trace-compatible subalgebra inclusion; ell1 factorization space; maximal factorization norm (hard)
  • Remark 2.4: arbitrary-index factorization, duality and Proposition 2.1: arbitrary-index maximal factorization space; arbitrary-index ell1 factorization space; finite-subset truncation; trace pairing (hard)
  • Proposition 2.5: complex interpolation isometries: ell1 factorization space; maximal factorization norm; Calderon complex interpolation space (hard)
  • Theorem 3.1: noncommutative Marcinkiewicz interpolation: positive-cone sum; subadditive operator-valued family; weak-type projection bound; strong-type positive majorant; conjugate interpolation parameter (hard)
  • Lemma 3.3: compressed strong bound from weak type: weak-type projection bound; compressed maximal norm (hard)
  • Lemma 3.4: mixed endpoint norm estimate: positive endpoint intersection; maximal factorization norm (hard)
  • Lemma 3.5: Lorentz Lp,1 estimate: noncommutative Lorentz Lp,q; generalized singular numbers; maximal factorization norm (hard)
  • Remark 3.6: positive-cone real J interpolation isometry: noncommutative Lorentz Lp,q; real J interpolation of cones; real J interpolation of Banach spaces (hard)
  • Lemma 3.8: quantitative J-method inclusion: noncommutative Lorentz Lp,q; real J interpolation of Banach spaces (hard)
  • Lemma 3.9: positive maximal cones interpolate: positive maximal cone; real J interpolation of cones; maximal factorization norm (hard)
  • Theorem 4.1: maximal Cesaro inequality with sharp growth: discrete Cesaro average; maximal factorization norm; optimal universal maximal constant (hard)
  • Corollary 4.3: column maximal Cesaro inequality: column maximal factorization space; discrete Cesaro average; maximal constant family (hard)
  • Corollary 4.4: ordered multiple Cesaro maximal inequalities: ordered multiple Cesaro averages; arbitrary-index maximal factorization space; column maximal factorization space (hard)
  • Theorem 4.5: one- and multiparameter continuous Cesaro maximal inequalities: weak-star continuous semigroup; continuous Cesaro average; ordered multiple continuous averages; arbitrary-index maximal factorization space; column maximal factorization space (hard)
  • Corollary 4.6: subordinated semigroup maximal inequalities: Unambiguous corrected full source assertion: Corollary 4.6: subordinated semigroup maximal inequalities (source-ambiguity)
  • Remark 4.7: continuous weak type (1,1) and subordination assertion: Unambiguous corrected full source assertion: Remark 4.7: continuous weak type (1,1) and subordination assertion (source-ambiguity)
  • Remark 4.7, continuous-average clause: continuous Cesaro average; weak-type projection bound (hard)
  • Theorem 5.1: symmetric discrete-power maximal inequality: symmetric tracial contraction; maximal factorization norm; powers of Lp extension (hard)
  • Theorem 5.2: fractional-average maximal inequality: fractional binomial coefficients; fractional averages; positive L2 operator; maximal factorization norm (hard)
  • Lemma 5.4: fractional averages in the right half-plane: fractional averages; maximal factorization norm (hard)
  • Lemma 5.5: discrete Littlewood–Paley square estimate: falling factorial coefficients; finite differences with zero past; discrete Littlewood-Paley square trace; positive L2 operator (hard)
  • Lemma 5.6: maximal finite-difference estimate: finite differences with zero past; positive L2 operator; maximal factorization norm (hard)
  • Lemma 5.7: scalar matrix action on maximal families: maximal factorization norm; absolutely summable scalar rows (hard)
  • Lemma 5.8: L2 fractional averages on negative half-integer lines: fractional averages; positive L2 operator; maximal factorization norm (hard)
  • Corollary 5.9: column maximal powers: column maximal factorization space; maximal constant family (hard)
  • Corollary 5.10: ordered multiple symmetric-power maximal inequalities: ordered multiple powers; arbitrary-index maximal factorization space; column maximal factorization space (hard)
  • Corollary 5.11: continuous symmetric-semigroup maximal inequalities: weak-star continuous semigroup; ordered multiple semigroup powers; arbitrary-index maximal factorization space; column maximal factorization space (hard)
  • Theorem 6.3: Cesaro errors belong to c0: discrete Cesaro average; mean-ergodic projection; c0 factorization space; column c0 factorization space (hard)
  • Corollary 6.4: individual discrete Cesaro theorem: discrete Cesaro average; mean-ergodic projection; tracial b.a.u. and a.u. convergence (hard)
  • Remark 6.5: a.u. convergence at p=2: discrete Cesaro average; tracial a.u. convergence (hard)
  • Theorem 6.6: ordered multiple individual Cesaro theorem: ordered multiple Cesaro averages; mean-ergodic projection; filter-tail c0 factorization spaces; tracial b.a.u. and a.u. convergence (hard)
  • Theorem 6.7: symmetric nonnegative-power individual theorem: positive L2 operator; powers of Lp extension; c0 factorization space; column c0 factorization space; tracial b.a.u. and a.u. convergence (hard)
  • Unnumbered remark after Theorem 6.7: even and odd power limits: even and odd powers; mean-ergodic projection; tracial b.a.u. convergence (hard)
  • Theorem 6.8: local and global continuous individual theorem: continuous Cesaro average; weak-star continuous semigroup; mean-ergodic projection; filter-tail c0 factorization spaces; tracial b.a.u. and a.u. convergence (hard)
  • Unnumbered remarks after Theorem 6.8: endpoints, multiple versions and subordination: Unambiguous corrected full source assertion: Unnumbered remarks after Theorem 6.8: endpoints, multiple versions and subordination (source-ambiguity)
  • Remark 7.2: independence of Haagerup injection parameter: Haagerup Lp; modular automorphism group; Haagerup density sandwiches; compatible Haagerup Lp extensions; modular analytic elements; maximal factorization norm; ell1 factorization space; column maximal factorization space; c0 factorization space; Calderon complex interpolation space; normal state-preserving conditional expectation (hard)
  • Remark 7.3: fixed points form a subalgebra under state preservation: normal faithful state; fixed point subalgebra; normal state-preserving conditional expectation; mean-ergodic projection (hard)
  • Theorem 7.4: nontracial maximal Cesaro and symmetric-power inequalities: Haagerup Lp; compatible Haagerup Lp extensions; discrete Cesaro average; arbitrary-index maximal factorization space; maximal constant family (hard)
  • Corollary 7.5: nontracial column maximal estimates: Haagerup Lp; compatible Haagerup Lp extensions; column maximal factorization space; maximal constant family (hard)
  • Corollary 7.6: continuous-index Haagerup maximal inequalities: Haagerup Lp; compatible Haagerup Lp extensions; weak-star continuous semigroup; continuous Cesaro average; arbitrary-index maximal factorization space; column maximal factorization space; Haagerup density sandwiches (hard)
  • Section 7.2 semigroup extension assertion: p=infinity contraction endpoint: weak-star continuous semigroup; continuous Cesaro average; bounded-family L-infinity norm; compatible Haagerup Lp extensions (hard)
  • Theorem 7.11: Haagerup c0 convergence of ordered averages and powers: Haagerup Lp; compatible Haagerup Lp extensions; ordered multiple Cesaro averages; ordered multiple powers; mean-ergodic projection; filter-tail c0 factorization spaces; positive L2 operator (hard)
  • Corollary 7.12: Jajte individual ergodic convergence: Haagerup Lp; Haagerup density sandwiches; Jajte bilateral almost-sure convergence; Jajte almost-sure convergence; ordered multiple Cesaro averages; ordered multiple powers; mean-ergodic projection (hard)
  • Unnumbered remarks after Corollary 7.12: semigroup and L1 extensions: Haagerup Lp; continuous Cesaro average; Jajte bilateral almost-sure convergence; Jajte almost-sure convergence; L1 endpoint individual limit (hard)
  • Lemma 7.13: transfer from density-injected c0 to Lance convergence: Unambiguous corrected full source assertion: Lemma 7.13: transfer from density-injected c0 to Lance convergence (source-ambiguity)
  • Corollary 7.14: bounded-input averages and powers convergence: Unambiguous corrected full source assertion: Corollary 7.14: bounded-input averages and powers convergence (source-ambiguity)
  • Corollary 7.14(i): Lance a.u. convergence for bounded-input averages: Lance a.u. and b.a.u. convergence; ordered multiple Cesaro averages; mean-ergodic projection (hard)
  • Unnumbered semigroup analogue after Corollary 7.14: weak-star continuous semigroup; continuous Cesaro average; ordered multiple continuous averages; Jajte bilateral almost-sure convergence; Jajte almost-sure convergence; Lance a.u. and b.a.u. convergence (hard)
  • Section 8.1: modular-action maximal averages and fixed-point centralizer: modular automorphism group; continuous Cesaro average; state centralizer; Haagerup Lp; arbitrary-index maximal factorization space (hard)
  • Section 8.1: asserted modular-action pointwise convergence: Unambiguous corrected full source assertion: Section 8.1: asserted modular-action pointwise convergence (source-ambiguity)
  • Section 8.2: operator-valued Poisson maximal and weak-type estimates: spatial von Neumann tensor product; operator-valued Bochner Lp identification; tensor-extended semigroup; classical Poisson semigroup; weak-type projection bound; classical Ornstein-Uhlenbeck subordination (hard)
  • Section 8.3: Gaussian and Poisson Schur multiplier semigroups: Schatten classes; Schur multiplier semigroup; isonormal Gaussian process; classical Poisson subordination; maximal factorization norm (hard)
  • Section 8.4: Hamiltonian Gaussian and Poisson semigroups: selfadjoint affiliated spectral calculus; Hamiltonian Gaussian conjugation semigroup; unbounded commutator generator; classical Poisson subordination; Schur multiplier semigroup (hard)
  • Section 8.5: free-product semigroups and free Poisson convergence: reduced free product of state algebras; free-product semigroup; centered reduced words; free Poisson semigroup; Haagerup Lp; Lance a.u. and b.a.u. convergence; Jajte bilateral almost-sure convergence; Jajte almost-sure convergence (hard)
  • Section 8.6: group length multipliers and fractional powers: group von Neumann algebra; tree-type length function; group Fourier multiplier semigroup; fractional length multiplier; reduced free product of groups (hard)
  • Section 8.7: q-Ornstein–Uhlenbeck construction and properties: q-Fock space; q-Gaussian algebra; vacuum tracial state; Wick product; second quantization; q-Ornstein-Uhlenbeck semigroup; number operator (hard)

Selected references

  • Noncommutative maximal ergodic theorems, arXiv:math/0505308v2, https://arxiv.org/abs/math/0505308v2
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On the Weyl Representation of Metaplectic OperatorsResearch Paper

Motivation

We study the Weyl representation of metaplectic operators associated to a symplectic matrix having no non-trivial fixed point, and justify a formula suggested in earlier work of Mehlig and Wilkinson. We give precise calculations of the associated Maslov-type indices; these indices intervene in a crucial way in Gutzwiller's formula of semiclassical mechanics, and are simply related to an index defined by Conley and Zehnder.

This mission is the statement-level formalization of On the Weyl Representation of Metaplectic Operators (arXiv:math/0503708v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

3 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Symplectic Cayley transform and its inverse (§3.1, unnumbered, PDF p. 6). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

9 results of the paper are not stated yet, because the library lacks an interface they need:

  • §4, paper-level conclusion: Concrete metaplectic group, its projection, source-normalized quadratic Fourier generators and weak MW operator (hard)
  • Lemma 1, (16)–(18): Three concrete weak oscillatory MW expressions (16)–(18) (hard)
  • Corollary 3: Unitary realization of the concrete MW map and actual metaplectic lifts (hard)
  • Proposition 6, (22)–(23): Concrete quadratic Fourier/MW equality with phase normalization (hard)
  • §3.2, equation (26): A genuine integer classical Conley–Zehnder index for symplectic paths (hard)
  • §3.2, equation (27): Consistent source statement for the printed Maslov–CZ equation (27) (source-ambiguity)
  • Lemma 8, (29): Source-normalized quadratic Fourier generators as actual Schwartz and canonical L2 operators (hard)
  • Proposition 9, (i)–(ii): Concrete Mp subgroup with admissible nonfixed free MW generators (hard)
  • Proposition 10, (32): Composition of actual MW operators and their metaplectic projection (hard)

Selected references

  • On the Weyl Representation of Metaplectic Operators, arXiv:math/0503708v1, https://arxiv.org/abs/math/0503708v1
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Pro-Lie groups which are infinite-dimensional Lie groupsResearch Paper

Motivation

A pro-Lie group is a projective limit of a family of finite-dimensional Lie groups. In this note we show that a pro-Lie group GGG is a Lie group in the sense that its topology is compatible with a smooth manifold structure for which the group operations are smooth if and only if GGG is locally contractible. We also characterize the corresponding pro-Lie algebras in various ways. Furthermore, we characterize those pro-Lie groups which are locally exponential, that is, they are Lie groups with a smooth exponential function which maps a zero neighborhood in the Lie algebra diffeomorphically onto an open identity neighborhood of the group.

This mission is the statement-level formalization of Pro-Lie groups which are infinite-dimensional Lie groups (arXiv:math/0609684v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

7 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Pro-Lie groups admit compatible Lie structures exactly when locally contractible (Theorem 1.1, PDF p. 3). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

31 results of the paper are not stated yet, because the library lacks an interface they need:

  • Theorem 1.2: The actual pro-Lie Lie functor, universal integration Gamma, prosolvable radical and Levi product, and smooth exponential/tangent Lie algebra interface (hard)
  • Theorem 1.3: Canonical Gamma integration and its regular Lie structure; tangent Lie algebra, smooth path evolution, and central discrete quotient classification (hard)
  • Theorem 1.5: Tangent and one-parameter Lie algebras, locally exponential local multiplication, and the actual quotientwise Maurer–Cartan operator/spectrum (hard)
  • Theorem 3.7: The canonical Gamma(L(G)) group, discrete central quotients and the corresponding arbitrary-product homeomorphism (hard)
  • Remark 4.4: Globally evaluated pronilpotent BCH Lie series and the actual Gamma integration (hard)
  • Theorem 4.5: Canonical Gamma, its ambient contraction predicate, and the prosolvable radical/semisimple product quotient (hard)
  • Proposition 4.7: Pro-compact adjoint module presentations and maximal compactly embedded subalgebras; Gamma-defined algebra smoothness (hard)
  • Proposition 5.1: The actual radical integration Gamma(r) and the Phi chart built from the closed commutator ideal and exponential evaluation (hard)
  • Theorem 5.2: Canonical Gamma integration and smoothness defined by ambient contractibility of that group (hard)
  • Proposition 5.7: Construction-specific Lie atlas on Gamma(g) and Milnor regularity with the smooth path-space topology (hard)
  • Theorem 5.8: Tangent Lie algebra of a general locally convex Lie group and its smooth exponential; Gamma-based smoothness of g (hard)
  • Corollary 5.9: Milnor regularity, tangent Lie algebra, actual Gamma and its discrete central Lie-group quotients (hard)
  • Lemma 5.11: The actual center of Gamma(g) for smooth g and the subgroup generated by all compact subgroups (hard)
  • Theorem 5.13: Actual center of Gamma(g) and Gamma-defined smoothness of g (hard)
  • Remark 6.5: Quotientwise adjoint flow and pointwise kappa integral on a pro-Lie algebra before local exponentiality is known (hard)
  • Remark 6.6: A comparison between the actual tangent Lie algebra and compact-open one-parameter Lie algebra, plus locally exponential canonical quotients (hard)
  • Theorem 7.1: E1–E4 global exponential Lie algebra, the actual Gamma group, and quotientwise complex adjoint spectrum (hard)
  • Example 7.2: The coefficient-topological formal current Lie algebra, its adjoint spectrum, and exponential/pronilpotent predicates (hard)
  • Proposition 7.3: Locally exponential algebra via E1–E4, exponential closed ideals, and the actual prosolvable radical (hard)
  • Remark 7.4: Exponential finite-codimensional ideal, actual prosolvable radical and regular canonical Gamma structure (hard)
  • Example 7.5: Pointwise averaging in arbitrary complete locally convex spaces, actual semidirect exponential and smooth inverse predicates (hard)
  • Lemma 7.7: Topological complexification, closed ideal subquotient roots, and complex spectrum of pro-Lie adjoint operators (hard)
  • Proposition 7.9: Canonical Gamma and exponential evaluation, topological root weights, and their natural integrated additive characters (hard)
  • Proposition 7.10: Milnor regularity and tangent Lie algebras for arbitrary locally convex Lie groups (hard)
  • Theorem 7.11: Independent E1–E4 local exponential algebra, pointwise kappa exp-regularity and actual Gamma integration (hard)
  • Corollary 7.12: Actual identity-component universal cover, one-parameter algebra and Gamma, and locally exponential group/algebra predicates (hard)
  • Remark 7.13: Closed-ideal root weights and the actual semidirect generator/adjoint regularity in n ⋊ R (hard)
  • Example 7.14: The actual infinite semidirect Lie algebra and bounded dual-module-types representation, spectral exp-regularity and local exponentiality (hard)
  • Remark 8.1: The canonical regular Gamma(g), its exponential and the local-diffeomorphism property of the specified product-of-exponentials chart (hard)
  • Remark 8.2: Canonical Gamma realization with actual integrated finite-quotient projections and its construction-specific regular atlas (hard)
  • Remark 8.3: Canonical Gamma(g) and its actual quotient projections, regular canonical atlas, locally exponential source groups (hard)

Selected references

  • Pro-Lie groups which are infinite-dimensional Lie groups, arXiv:math/0609684v1, https://arxiv.org/abs/math/0609684v1
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Decoherence rates for Galilean covariant dynamicsResearch Paper

Motivation

We introduce a measure of decoherence for a class of density operators. For Gaussian density operators in dimension one it coincides with an index used by Morikawa (1990). Spatial decoherence rates are derived for three large classes of the Galilean covariant quantum semigroups introduced by Holevo. We also characterize the relaxation to a Gaussian state for these dynamics and give a theorem for the convergence of the Wigner function to the probability distribution of the classical analog of the process.

This mission is the statement-level formalization of Decoherence rates for Galilean covariant dynamics (arXiv:0710.1344v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

13 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem 4.3, cases 1 and 3: leading spatial decoherence rates (seed from abstract) (Theorem 4.3, cases 1 and 3: leading spatial decoherence rates (seed from abstract), PDF p. 18). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

9 results of the paper are not stated yet, because the library lacks an interface they need:

  • Proposition 4.1, case 2: position-only Gaussian noise: A source-consistent complete statement for Proposition 4.1, case 2: position-only Gaussian noise (source-ambiguity)
  • Theorem 4.3, case 2: position-only Lévy noise: A source-consistent complete statement for Theorem 4.3, case 2: position-only Lévy noise (source-ambiguity)
  • Theorem 4.4: relative Hilbert–Schmidt Gaussian relaxation: A source-consistent complete statement for Theorem 4.4: relative Hilbert–Schmidt Gaussian relaxation (source-ambiguity)
  • Theorem 4.5: Wigner/classical relative L² convergence: A source-consistent complete statement for Theorem 4.5: Wigner/classical relative L² convergence (source-ambiguity)
  • Proposition 2.5: commutator and anticommutator characteristic formulas: A source-consistent complete statement for Proposition 2.5: commutator and anticommutator characteristic formulas (source-ambiguity)
  • Lemma 4.2: regularity and quadratic estimates of a Lévy exponent: A source-consistent complete statement for Lemma 4.2: regularity and quadratic estimates of a Lévy exponent (source-ambiguity)
  • Lemma A.1: differentiating Weyl translations in trace norm: A source-consistent complete statement for Lemma A.1: differentiating Weyl translations in trace norm (source-ambiguity)
  • Lemma A.2, moreover: directional derivative identity: A source-consistent complete statement for Lemma A.2, moreover: directional derivative identity (source-ambiguity)
  • Appendix A, (A.1)–(A.2) and Fourier/kernel identities: Partial and full angular-frequency L² Fourier transforms tied to actual Schrödinger HS kernels and the Wigner definition (hard)

Selected references

  • Decoherence rates for Galilean covariant dynamics, arXiv:0710.1344v2, https://arxiv.org/abs/0710.1344v2
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Constructing algebraic Lie algebrasResearch Paper

Motivation

We give an algorithm for constructing the algebraic hull of a given matrix Lie algebra in characteristic zero. It is based on an algorithm for finding integral linear dependencies of the roots of a polynomial, that is probably of independent interest.

This mission is the statement-level formalization of Constructing algebraic Lie algebras (arXiv:math/0611414v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

3 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Trivial permutation component and power traces (Lemma 5: trivial permutation component and trace, PDF p. 5). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

18 results of the paper are not stated yet, because the library lacks an interface they need:

  • Abstract / §§2–3: construction of the algebraic hull: Algebraic subgroups of GL(n) over arbitrary characteristic-zero F, their tangent Lie subalgebras, and the intrinsic algebraic hull; effective exact number-field computations and a terminating executable construction (hard)
  • §2: algebraicity criterion using a basis: Algebraic subgroups of GL(n) over arbitrary characteristic-zero F, their tangent Lie subalgebras, and the intrinsic algebraic hull (hard)
  • Lemma 2: coefficient-space description of a semisimple hull: Algebraic subgroups of GL(n) over arbitrary characteristic-zero F, their tangent Lie subalgebras, and the intrinsic algebraic hull (hard)
  • Algorithm 3: exact splitting-field hull construction: Algebraic subgroups of GL(n) over arbitrary characteristic-zero F, their tangent Lie subalgebras, and the intrinsic algebraic hull; effective exact number-field computations and a terminating executable construction (hard)
  • Example 4: even quartic minimal polynomial: Algebraic subgroups of GL(n) over arbitrary characteristic-zero F, their tangent Lie subalgebras, and the intrinsic algebraic hull (hard)
  • Lemma 6: irreducible augmentation component: A valid scope for the irreducible augmentation lemma when the characteristic polynomial is reducible and n=2 (source-ambiguity)
  • Corollary 7: 2-transitive or prime-degree hull: Algebraic subgroups of GL(n) over arbitrary characteristic-zero F, their tangent Lie subalgebras, and the intrinsic algebraic hull (hard)
  • Proposition 8: all four non-S4/non-A4 quartic cases: Algebraic subgroups of GL(n) over arbitrary characteristic-zero F, their tangent Lie subalgebras, and the intrinsic algebraic hull (hard)
  • Proposition 9: sextic Magma-group formula: Proposition 9: sextic Magma-group formula with corrected source precision, scope or output contract (source-ambiguity)
  • §6: the two integral-dependency tasks: §6: the two integral-dependency tasks with corrected source precision, scope or output contract (source-ambiguity)
  • Algorithm 10: certified zero test: Algorithm 10: certified zero test with corrected source precision, scope or output contract (source-ambiguity)
  • Theorem 11: small integral relation basis: Theorem 11: small integral relation basis with corrected source precision, scope or output contract (source-ambiguity)
  • Algorithm 13: LLL relation-lattice algorithm: Algorithm 13: LLL relation-lattice algorithm with corrected source precision, scope or output contract (source-ambiguity)
  • §6: reduced-precision retry variant of Algorithm 13: §6: reduced-precision retry variant of Algorithm 13 with corrected source precision, scope or output contract (source-ambiguity)
  • Algorithm 14: Galois-assisted relation reconstruction: Algorithm 14: Galois-assisted relation reconstruction with corrected source precision, scope or output contract (source-ambiguity)
  • §6: extension to relations over number-field orders: §6: extension to relations over number-field orders with corrected source precision, scope or output contract (source-ambiguity)
  • §6 Remark: component-testing algorithm: §6 Remark: component-testing algorithm with corrected source precision, scope or output contract (source-ambiguity)
  • §7: hull construction avoiding exact splitting fields: §7: hull construction avoiding exact splitting fields with corrected source precision, scope or output contract (source-ambiguity)

Selected references

  • Constructing algebraic Lie algebras, arXiv:math/0611414v1, https://arxiv.org/abs/math/0611414v1
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Quantum communication using a bounded-size quantum reference frameResearch Paper

Motivation

Typical quantum communication schemes are such that to achieve perfect decoding the receiver must share a reference frame with the sender. Indeed, if the receiver only possesses a bounded-size quantum token of the sender's reference frame, then the decoding is imperfect, and we can describe this effect as a noisy quantum channel. We seek here to characterize the performance of such schemes, or equivalently, to determine the effective decoherence induced by having a bounded-size reference frame. We assume that the token is prepared in a special state that has particularly nice group-theoretic properties and that is near-optimal for transmitting information about the sender's frame. We present a decoding operation, which can be proven to be near-optimal in this case, and we demonstrate that there are two distinct ways of implementing it (corresponding to two distinct Kraus decompositions). In one, the receiver measures the orientation of the reference frame token and reorients the system appropriately. In the other, the receiver extracts the encoded information from the virtual subsystems that describe the relational degrees of freedom of the system and token. Finally, we provide explicit characterizations of these decoding schemes when the system is a single qubit and for three standard kinds of reference frame: a phase reference, a Cartesian frame (representing an orthogonal triad of spatial directions), and a reference direction (representing a single spatial direction).

This mission is the statement-level formalization of Quantum communication using a bounded-size quantum reference frame (arXiv:0812.5040v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

18 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Canonical-token effective channel (Paper result: canonical-token effective channel, Eqs.(1)–(3), (38)–(40), PDF p. 1). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

3 results of the paper are not stated yet, because the library lacks an interface they need:

  • §V.B, Eqs.(73)–(92), continuing PDF p.14: The based joint multiplicity decomposition and explicit reciprocal Cartesian A_J of Eqs.(75),(79),(81),(84),(87), tied to the actual symmetric-tensor spin representation and paired canonical memory. (hard)
  • §III, sentence following the no-prior-information claim: A source-supported average-input restriction compatible with the fixed recovery D_R E†. (source-ambiguity)
  • §III.D continuation, first column: A purification or a changed encoding that could make the whole successful composite pure. (source-ambiguity)

Selected references

  • Quantum communication using a bounded-size quantum reference frame, arXiv:0812.5040v2, https://arxiv.org/abs/0812.5040v2
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A non-smooth continuous unitary representation of a Banach-Lie groupResearch Paper

Motivation

In this note we show that the representation of the additive group of the Hilbert space L2([0,1],R)L^2([0,1],\R)L2([0,1],R) on L2([0,1],\C)L^2([0,1],\C)L2([0,1],\C) given by the multiplication operators π(f):=eif\pi(f) := e^{if}π(f):=eif is continuous but its space of smooth vectors is trivial. This example shows that a continuous unitary representation of an infinite dimensional Lie group need not be smooth.

This mission is the statement-level formalization of A non-smooth continuous unitary representation of a Banach-Lie group (arXiv:0811.4234v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

3 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is The phase representation is continuous and has only the zero smooth vector (Theorem 2.3, PDF p. 4). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Selected references

  • A non-smooth continuous unitary representation of a Banach-Lie group, arXiv:0811.4234v1, https://arxiv.org/abs/0811.4234v1
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Towards a Lie theory for locally convex groupsResearch Paper

Motivation

In this survey, we report on the state of the art of some of the fundamental problems in the Lie theory of Lie groups modeled on locally convex spaces, such as integrability of Lie algebras, integrability of Lie subalgebras to Lie subgroups, and integrability of Lie algebra extensions to Lie group extensions. We further describe how regularity or local exponentiality of a Lie group can be used to obtain quite satisfying answers to some of the fundamental problems. These results are illustrated by specialization to some specific classes of Lie groups, such as direct limit groups, linear Lie groups, groups of smooth maps and groups of diffeomorphisms.

This mission is the statement-level formalization of Towards a Lie theory for locally convex groups (arXiv:1501.06269v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

5 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Fundamental results of locally convex differential calculus (Proposition I.2.3, PDF p. 12). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

99 results of the paper are not stated yet, because the library lacks an interface they need:

  • Proposition I.4.3: Graded differential forms on the actual curve tangent bundle; exterior derivative, contraction, and Lie derivative constructed from I.4.1–2, with the degree-zero contraction convention. (hard)
  • Theorem II.2.1: A type of Hausdorff Bastiani Lie structures on a fixed abstract group, with equality of smooth structures rather than equality of chosen chart presentations; local group multiplication on U before any global topology exists. (hard)
  • Corollary II.2.2: The actual locally defined product and injective local homomorphism; Lie structures on the subgroup generated by its image, with the entire image open and the source manifold structure preserved. (hard)
  • Corollary II.2.3: Lie structures extending the supplied normal-subgroup structure as an open subgroup; smooth conjugation automorphisms defined independently on that subgroup. (hard)
  • Corollary II.2.4: A topology-compatible Bastiani Lie structure transported along a covering homomorphism, with local smooth inverses and uniqueness on the receiving group. (hard)
  • Theorem II.2.8: Finite-order mapping spaces on compact manifolds with boundary; compact-open C^r topology and the locally convex direct-limit topology on compact-support maps; tangent Lie algebra identification with pointwise bracket. (hard)
  • Lemma II.3.3: Diffeomorphisms of a general locally convex manifold; joint smooth evaluation and inverse evaluation; left logarithmic derivative from the actual tangent map, and Ad as pushforward. (hard)
  • Lemma II.3.5: The same independently constructed diffeomorphism-valued differential as II.3.3, so equality of logarithmic derivatives is not a freely supplied relation; connectedness and the conditional common-value uniqueness conclusion. (hard)
  • Lemma II.3.10: Smooth diffeomorphism-valued evolution on arbitrary real intervals, its actual right logarithmic derivative and curve tangents, including the endpoint derivative convention; no general locally convex ODE uniqueness assumption. (hard)
  • Proposition II.4.1: The actual tangent-at-identity Lie functor, left Maurer–Cartan form and pullback logarithmic derivative; all three clauses, including connected uniqueness and the homomorphism criterion. (hard)
  • Corollary II.4.2: Ad(g) computed by differentiating conjugation at the identity; a freely chosen representation cannot encode the asserted equality with the group center. (hard)
  • Proposition II.4.3: The tangent-at-identity Lie algebra with bracket obtained from left invariant vector fields, rather than an unrelated Lie algebra parameter attached to a connected group. (hard)
  • Theorem II.4.4: The computed tangent Lie algebra and its lower central and derived series; both nilpotence and solvability must be compared with the corresponding group series. (hard)
  • Proposition II.5.6: Smooth curves on the closed interval with their compact-open C-infinity locally convex topology; regularity defined by the actual endpoint evolution map, including smooth dependence, and Mackey completeness by existence of antiderivatives. (hard)
  • Proposition II.5.7: An exponential supplied as a smooth one-parameter-group evolution; delta(exp) computed by inverse left translation of its differential and Ad by differentiated conjugation; represented pointwise weak integral with the minus sign. (hard)
  • Proposition II.5.11: The independent exponential, adjoint flow and kappa operator; fibers and isolated points, all C1 curves in the restricted kernel, and finite-dimensional discreteness; all five clauses including the conditional reverse centrality implication. (hard)
  • Lemma II.6.2: Initial Lie subgroup structures with injective differential and the universal finite-C^k lifting property for every source manifold; uniqueness of the induced intrinsic smooth structure. (hard)
  • Proposition II.6.3: The set of actual right derivatives of based C1 arcs [0,1] into H, defined before proving bracket closure; compatibility with the image of the actual initial inclusion differential. (hard)
  • Theorem III.1.2: Lie-algebra-valued forms, Maurer–Cartan equation, actual local primitives and their gluing; based piecewise smooth loop classes and the normalized lift gamma(0)=1 determining the period homomorphism. (hard)
  • Corollary III.1.6: Regularity as smooth endpoint evolution and a smooth Lie group isomorphism whose differential is the given topological Lie algebra isomorphism; 1-connectedness includes connectedness. (hard)
  • Corollary III.1.7: Closed topological Lie ideals and the quotient topology; actual adjoint invariance and integration of a quotient to a regular Bastiani Lie group. (hard)
  • Theorem III.4.1: Unresolved printed source statement: Theorem III.4.1 (source-ambiguity)
  • Proposition IV.1.2: The actual smooth exponential of a general Banach Lie group and a local diffeomorphism in its given manifold structure; an arbitrary function called exponential would be circular. (hard)
  • Theorem IV.1.8: Locally convex analyticity via complexification and continuous homogeneous polynomials, actual local exponential charts with analytic inverse, and Dynkin BCH convergence; smooth inverse alone is insufficient. (hard)
  • Corollary IV.1.10: A topology-compatible analytic Lie structure and analytic exponential chart for arbitrary Banach Lie groups, using the actual BCH criterion rather than a Boolean label. (hard)
  • Theorem IV.1.11: Continuous inverse algebras without imposed normability; unit-group analytic charts, actual exponential, Mackey completeness, and smooth evolution regularity with sequential completeness only in the second clause. (hard)
  • Theorem IV.1.12: Compactly supported gauge transformations of the actual principal bundle, support on the base, equivariant adjoint-bundle sections and their LF topology; local exponentiality, regularity and BCH inheritance. (hard)
  • Lemma IV.1.17: The actual tangent Lie bracket and group exponential, local exponential charts, and convergence in the given group topology of the positive-index Trotter and four-factor commutator sequences. (hard)
  • Theorem IV.1.18: Both the smooth locally exponential category and the analytic BCH category over possibly nonnormable model spaces; actual maps retain their prescribed continuous homomorphism. (hard)
  • Theorem IV.1.19: Lie group morphisms and their computed differential, smooth target exponential without regularity, and the locally exponential 1-connected source; uniqueness is for the supplied algebra morphism. (hard)
  • Corollary IV.1.20: Actual locally exponential group structures and tangent Lie algebra isomorphisms; a smooth group isomorphism, not merely an abstract group equivalence. (hard)
  • Theorem IV.1.24: The compact-open space Hom_c(R,G), with scalar rescaling and operations defined by the specified Trotter/commutator limits; all Lie and continuity laws without a manifold assumption. (hard)
  • Lemma IV.2.2: Local Lie products on convex balanced open subsets of the tangent algebra with guarded domains, radial one-parameter groups, and second derivative equal to the given bracket. (hard)
  • Theorem IV.2.6: Polynomial nilpotent BCH multiplication, actual exponential as a covering Lie morphism, the discrete central kernel and its fundamental-group identification, plus regularity and local exponentiality. (hard)
  • Proposition IV.2.7: The actual polynomial BCH group on the computed tangent Lie algebra, with no completeness hypothesis; a smooth group isomorphism for the 1-connected exponential nilpotent source. (hard)
  • Theorem IV.2.8: Formal homogeneous Dynkin BCH polynomials and Taylor coefficients of the independently specified local product; no unsupported assertion of convergence in a non-BCH algebra. (hard)
  • Theorem IV.2.9: Topological Lie quotient and local products; integrable adjoint flows and pointwise represented kappa; stability for every x and neighborhood equality kappa(x)n=n, plus the kernel factorization consequence. (hard)
  • Lemma IV.3.1: The differential tangent set from actual C1 arcs and the exponential tangent set from all real multiples, with their equality and closed Lie-subalgebra structure. (hard)
  • Theorem IV.3.3: Locally exponential structures on the actual closed subgroup inducing its subspace topology, an exponential slice chart, and the source closed-subspace notion of submanifold without a complement assumption. (hard)
  • Proposition IV.3.4: Actual subgroup Lie structures and preimage structure with subspace topology; the supplied smooth homomorphism and its differential cannot be treated as unrelated data. (hard)
  • Theorem IV.3.5: Quotient Lie structures inducing quotient topology, subgroup structures inducing subspace topology, and the quotient algebra and kappa neighborhood condition in the full three-way equivalence. (hard)
  • Corollary IV.3.6: BCH analytic structures on subgroups with subspace topology and group quotients with quotient topology; cannot assert only an algebraic quotient or only local exponentiality. (hard)
  • Theorem IV.3.8: The concrete subgroup generated by integrated adjoint automorphisms, an independently defined smooth structure with model g/z(g), and exponential of quotient classes; no ambient topology on Aut(g) is given. (hard)
  • Corollary IV.3.9: The intrinsic locally exponential structure on the actual group center with its subspace topology, plus its identification as the kernel of the computed Ad. (hard)
  • Corollary IV.3.12: The natural Banach manifold structure on GL(E), and a possibly nonsplit closed-subspace stabilizer as a Banach Lie submanifold with the induced topology. (hard)
  • Corollary IV.3.13: The natural Banach manifold structure on GL(E) and the actual vector stabilizer as a Banach Lie subgroup, with v=0 permitted. (hard)
  • Corollary IV.3.14: The Banach Lie group GL(E), the subgroup preserving the supplied continuous bilinear operation, and its tangent Lie algebra identified with exactly the continuous derivations. (hard)
  • Corollary IV.3.15: Unresolved printed source statement: Corollary IV.3.15 (source-ambiguity)
  • Lemma IV.4.2: Independent tangent Lie functor and exponential/adjoint flows on both groups, so stability of image and kernel is a conclusion, not a field in a morphism structure. (hard)
  • Lemma IV.4.3: Integrable adjoint operators and their smooth flows in the actual possibly different subalgebra and ambient topologies; BCH analyticity, finite (co)dimension, and all three clauses. (hard)
  • Theorem IV.4.9: Locally exponential topological Lie algebras, the actual smooth group exponential and derived injection; the discrete central preimage is a hypothesis, and the integral subgroup must have the prescribed derivative. (hard)
  • Corollary IV.4.10: The same prescribed-derivative integral subgroup construction without assuming closed range; the two alternative sufficient hypotheses must remain alternatives. (hard)
  • Theorem IV.4.14: Actual integral inclusion and differential, exponential tangent set, local exponential injectivity and separable source algebra; the stronger initiality conclusion requires locally exponential ambient G and closed differential range. (hard)
  • Theorem IV.4.16: An initial Lie topology on the closed subgroup that may be finer than the subspace topology; its identity component, tangent algebra, and prescribed integral inclusion. (hard)
  • Theorem IV.4.17: The actual finest required intrinsic initial Lie topology making the maximal contained vector subspace open; its identity component and equality with both actual tangent sets, rather than the original subgroup topology. (hard)
  • Theorem V.1.4: Locally smooth outer actions and their C2/C3 equations, actual twisted multiplication and unique local-product-compatible Lie atlas, extension equivalence classes, and abelian Baer sum as a fiber-product quotient. (hard)
  • Theorem V.1.8: Smooth locally trivial principal-bundle extensions and smooth endpoint evolution on all three groups; algebraic exactness alone does not define the extension category. (hard)
  • Theorem V.2.8: Normalized locally smooth cochains, coboundary quotient H_s^2, equivalence classes of principal-bundle extensions with the prescribed action, and the Baer group law; the isomorphism is the cocycle extension map. (hard)
  • Proposition V.2.10: Continuous alternating Lie cochains for the supplied joint continuous action, their differential and quotient, topologically split abelian extensions with the fixed action, and the computed twisted bracket. (hard)
  • Corollary V.3.2: Unresolved printed source statement: Corollary V.3.2 (source-ambiguity)
  • Theorem VI.1.8: Actual adjoint group, its pi2 period map for the central extension, period image in the topological center and enlargeability to a locally exponential group; no arbitrary subgroup labeled period group. (hard)
  • Proposition VI.1.9: The actual period subgroup and its inherited topology, for separable locally exponential algebras; closedness/discreteness equivalence requires the additional complete metrizable locally convex topology. (hard)
  • Theorem VI.1.10: Concrete Z(G,n), its normal locally exponential structure and computed algebra, normalized-loop period via represented weak integration, and generated exp(n) subgroup before closedness; retain all three equivalences without adding completeness. (hard)
  • Proposition VI.1.12: Canonical universal coverings of the adjoint groups, integration of the induced algebra map there, pi2 transport by covering isomorphisms, and naturality of the actual period maps and images. (hard)
  • Corollary VI.1.13: The actual period constructions on both topological Lie algebras and their product, with the canonical product identification of the centers. (hard)
  • Proposition VI.1.15: The actual central exponential kernel in a 1-connected locally exponential Frechet Lie group and an actual group isomorphism with pi1 of the center. (hard)
  • Theorem VI.1.17: Continuous based paths with the compact-open topology and pointwise bracket, local multiplication on that topology, enlargeability and the evaluation-at-1 quotient consequence. (hard)
  • Theorem VI.1.27: Completed projective tensor quotient cyclic homology, universal cyclic cocycle, stable K3 period map, and the actual topological Steinberg Lie algebras of all positive matrix sizes over the complete CIA. (hard)
  • Corollary VI.2.2: Stable ideals using actual integrated adjoint groups and the analytic locally convex Lie category with an analytic exponential, rather than ruling out every smooth integration. (hard)
  • Theorem VI.2.7: The actual semidirect topological Lie algebra with bracket (tDv-prime minus t-prime Dv,0), smooth joint R-actions and generator defined by directional differentiation, and integrability to arbitrary locally convex Lie groups. (hard)
  • Lemma VII.2.3: Compact-support diffeomorphism Lie structures, locally finite compact covers and the locally convex restricted direct-product topology; finite-support factorization with an existential terminal index for each input. (hard)
  • Theorem VIII.2: Unresolved printed source statement: Theorem VIII.2 (source-ambiguity)
  • Corollary IX.1.2: The natural LF manifold structure on compactly supported diffeomorphisms; continuity of the supplied homomorphism refers to that topology and smoothness refers to its actual charts. (hard)
  • Corollary IX.1.7: Unresolved printed source statement: Corollary IX.1.7 (source-ambiguity)
  • Theorem IX.1.9: Unresolved printed source statement: Theorem IX.1.9 (source-ambiguity)
  • Remark I.5.3 (explicit unnumbered result): The actual smooth vector-field space with the topology induced by all iterated tangent maps; finite-dimensional bracket continuity and the affine-field restriction proving failure on every nonempty open subset of an infinite-dimensional model. (hard)
  • Example II.1.4 (explicit unnumbered result): Continuous inverse algebra unit manifold as an open subset, smooth multiplication and inversion and the computed inversion derivative without imposing Mackey completeness or assuming an exponential. (hard)
  • Remark II.1.6 (explicit unnumbered result): The actual tangent bundle of a locally convex Lie group and tangent maps of multiplication and inversion, the zero identity vector, and zero-section/projection morphisms. (hard)
  • Remark II.3.7 (explicit unnumbered result): Smooth joint group actions and representations, actual infinitesimal derivatives with the left-action minus sign and linear-representation plus sign, and uniqueness of each action for a connected group. (hard)
  • Examples II.5.9 (explicit unnumbered result): Actual semidirect exponential and represented weak beta integral with beta(0)=id, the local-injectivity/surjectivity criteria, and both infinite diagonal-product examples in their product topologies. (hard)
  • Remark II.5.10 (explicit unnumbered result): Actual exponential of a Mackey-complete CIA unit group, tangent identification with A, and the differential represented by the integral of exp((1-t)x)y exp(tx) in precisely that noncommuting order. (hard)
  • Remark II.6.6 (explicit unnumbered result): The locally embedded subgroup definition via the smooth arc component of an identity neighborhood and its intrinsic Lie structure, and initiality for all finite orders. (hard)
  • Example IV.1.6 (explicit unnumbered result): The genuine homogeneous Dynkin BCH terms, finite polynomial sum for a nilpotent locally convex algebra, and its resulting group structure and identity exponential; H1 and H2 must not be counted twice. (hard)
  • Example IV.1.13 (explicit unnumbered result): Arbitrary projective systems of nilpotent topological Lie algebras with no uniform nilpotency bound, actual coordinatewise BCH products, and the induced smooth exponential group with exp=id. (hard)
  • Example IV.1.16 (explicit unnumbered result): The real sequence-space semidirect group, analytic structure and actual exp/log, smooth but nonanalytic inverse and exponential-coordinate multiplication; normed analyticity cannot be substituted on R^N. (hard)
  • Remark IV.2.5 (explicit unnumbered result): Independently chosen guarded local Lie products satisfying radial and second-order conditions, preservation by every continuous Lie algebra morphism near zero, and equality of their germs. (hard)
  • Example IV.4.5 (explicit unnumbered result): The Frechet smooth-function translation semidirect group, actual support-restricted subalgebra, generated subgroup C_c-infinity(R) semidirect R, and the exclusion of every exponential integration of the inclusion. (hard)
  • Example IV.4.6 (explicit unnumbered result): Unresolved printed source statement: Example IV.4.6 (explicit unnumbered result) (source-ambiguity)
  • Remark V.2.7 (explicit unnumbered result): Nonabelian group and Lie crossed cocycles with their actual infinitesimal differentiation map; normalized equivariant forms, injectivity for connected G, regular target integration and pointed-set exactness of the period sequence. (hard)
  • Remark V.2.9 (explicit unnumbered result): The stronger local cocycle smoothness at each g, H_ss^2 as the quotient by locally smooth coboundaries, and its actual extension-classification homomorphism without connectedness. (hard)
  • Remark V.2.16 (explicit unnumbered result): Unresolved printed source statement: Remark V.2.16 (explicit unnumbered result) (source-ambiguity)
  • Example V.3.5 (explicit unnumbered result): The actual torus area form, vector-field cocycle, period and flux maps, and the disconnected gauge kernel and principal circle bundle; the abelian extension must differentiate to that particular cocycle. (hard)
  • Remark VI.1.14 (explicit unnumbered result): Unresolved printed source statement: Remark VI.1.14 (explicit unnumbered result) (source-ambiguity)
  • Remark VI.1.22 (explicit unnumbered result): Unresolved printed source statement: Remark VI.1.22 (explicit unnumbered result) (source-ambiguity)
  • Example VI.2.8 (explicit unnumbered result): Formal vector fields with arbitrary constant term and coefficientwise Frechet topology, the formal derivative bracket and integrability to groups with exponential; the false split-sequence sentence is not an assumption. (hard)
  • Mapping groups as projective limits (unnumbered): Compact manifold-with-boundary exhaustion cofinal among all compact subsets, C^r mapping groups with the actual compact-open derivative topology and restriction bonding maps, and the topological-group limit universal property. (hard)
  • Lie algebra of the projective mapping group (unnumbered): The compact-open one-parameter-group Lie algebra of the projective mapping group, canonical identification with C^r(M,L(K)), and its actual pointwise exponential; no manifold structure on the noncompact full mapping group. (hard)
  • Holomorphic mapping-group projective limit (unnumbered): Unresolved printed source statement: Holomorphic mapping-group projective limit (unnumbered) (source-ambiguity)
  • Smooth structure from the pro-solvable coordinate chart (unnumbered): The actual pro-Lie integration functor and pro-solvable radical, closed commutator algebra and complemented weakly complete topology, and the specified exponential-product homeomorphism as a smooth group chart. (hard)

Selected references

  • Towards a Lie theory for locally convex groups, arXiv:1501.06269v1, https://arxiv.org/abs/1501.06269v1
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🏆Completed
Quantum Information·Captain: Goku

The weighted hook length formulaResearch Paper

Motivation

Based on the ideas in [CKP], we introduce the weighted analogue of the branching rule for the classical hook length formula, and give two proofs of this result. The first proof is completely bijective, and in a special case gives a new short combinatorial proof of the hook length formula. Our second proof is probabilistic, generalizing the (usual) hook walk proof of Green-Nijenhuis-Wilf, as well as the q-walk of Kerov. Further applications are also presented.

This mission is the statement-level formalization of The weighted hook length formula (arXiv:1006.0043v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

10 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Four weighted branching identities (Theorem 2(a)–(d), PDF p. 6). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

3 results of the paper are not stated yet, because the library lacks an interface they need:

  • §6.4, first new summation formula: An authoritative corrected first §6.4 summation formula with consistent coordinate and boundary conventions. (source-ambiguity)
  • §6.4, second new summation formula: An authoritative corrected second §6.4 summation formula with consistent coordinate and boundary conventions. (source-ambiguity)
  • §6.4, third new summation formula: An authoritative corrected third §6.4 summation formula with consistent coordinate and boundary conventions. (source-ambiguity)

Selected references

  • The weighted hook length formula, arXiv:1006.0043v1, https://arxiv.org/abs/1006.0043v1
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Quantum Information·Captain: Goku

Unbounded generators of dynamical semigroupsResearch Paper

Motivation

Dynamical semigroups have become the key structure for describing open system dynamics in all of physics. Bounded generators are known to be of a standard form, due to Gorini, Kossakowski, Sudarshan and Lindblad. This form is often used also in the unbounded case, but rather little is known about the general form of unbounded generators. In this paper we first give a precise description of the standard form in the unbounded case, emphasizing intuition, and collecting and even proving the basic results around it. We also give a cautionary example showing that the standard form must not be read too naively. Further examples are given of semigroups, which appear to be probability preserving to first order, but are not for finite times. Based on these, we construct examples of generators which are not of standard form.

This mission is the statement-level formalization of Unbounded generators of dynamical semigroups (arXiv:1707.02266v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

6 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is No-event semigroups admit a C0 contraction implementation (Definition II.1, asserted realization of no-event semigroups, PDF p. 3). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

19 results of the paper are not stated yet, because the library lacks an interface they need:

  • Abstract / Section IV: two concrete conservative non-standard generators: Concrete birth/diffusion models and standardness over all contraction generators (hard)
  • Section II.B, event expansion is the minimal semigroup: Completed event tensor powers, pathwise detection iterates, and trace-class partial traces (hard)
  • Proposition II.3: equivalent standard-form data: Exit rank-one lift, graph-continuous extension, Kraus and transit-basis correspondences (hard)
  • Section II.C, claimed converse resolvent characterization: Nondegeneracy of an abstract resolvent family (source-ambiguity)
  • Lemma II.6: gauge transformation: Corrected gauge data and equality of actual minimal standard semigroups (hard)
  • Proposition II.7: no additional nonzero rank-one factors: Standard jump realization with actual densely defined adjoints and forward equation (hard)
  • Section III.A: non-closable jump operators in a standard generator: Half-line H1 boundary trace and actual shift-generator jump composition (hard)
  • Section III.B.1: explicit quantum birth resolvent (32)–(33): Constructed quantum-birth standard semigroup and its actual Laplace resolvent (hard)
  • Lemma III.1: full birth-generator domain from matrix elements: Actual birth generator versus formal matrix-element action (hard)
  • Section III.B.2: conservativity and arrival transform: Quantum-birth arrival distribution and independent exponential waiting-time sum (hard)
  • Section III.B.3: boundary functionals and strict domain increase: Birth boundary coefficient functionals and constructed trace-class sigma (hard)
  • Proposition III.2: moderately growing rates support coherent escape: Moderately growing birth rates and trace-class coherent-shift operators (hard)
  • Section III.B.3, asserted stretched-exponential examples: A consistent quantitative moderate-growth condition (source-ambiguity)
  • Section III.B.3, Example: Exponentially growing rates: Exponential-rate birth generator and off-diagonal boundary functionals (hard)
  • Proposition III.3: no new rank-one operators for quantum birth: Computed actual birth and no-event domains on rank-one operators (hard)
  • Section III.C: diagonal-diffusion semigroup and resolvent kernels: Absorbing H2 half-line realization and a.e. trace-class kernel evolution (hard)
  • Section III.C: boundary regularity and normalization loss: Nuclear trace density, diffusion-domain regularity and boundary derivative (hard)
  • Section III.C: no new rank-one operators for diagonal diffusion: Actual Dirichlet adjoint realization and minimal diffusion rank-one domains (hard)
  • Section IV, conservative rank-one reset perturbation (52): Actual reset semigroups for both concrete nonconservative models (hard)

Selected references

  • Unbounded generators of dynamical semigroups, arXiv:1707.02266v1, https://arxiv.org/abs/1707.02266v1
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On Analytic Vectors for Unitary Representations of Infinite Dimensional Lie GroupsResearch Paper

Motivation

Let GGG be a 1-connected Banach-Lie group or, more generally, a BCH--Lie group. On the complex enveloping algebra U\C(\g)U_\C(\g)U\C​(\g) of its Lie algebra \g\g\g we define the concept of an analytic functional and show that every positive analytic functional λ\lambdaλ is integrable in the sense that it is of the form λ(D)=\la\ddπ(D)v,v\ra\lambda(D) = \la \dd\pi(D)v, v\raλ(D)=\la\ddπ(D)v,v\ra for an analytic vector vvv of a unitary representation of GGG. On the way to this result we derive criteria for the integrability of *-representations of infinite dimensional Lie algebras of unbounded operators to unitary group representations. For the matrix coefficient πv,v(g)=\laπ(g)v,v\ra\pi^{v,v}(g) = \la \pi(g)v,v\raπv,v(g)=\laπ(g)v,v\ra of a vector vvv in a unitary representation of an analytic Fr'echet-Lie group GGG we show that vvv is an analytic vector if and only if πv,v\pi^{v,v}πv,v is analytic in an identity neighborhood. Combining this insight with the results on positive analytic functionals, we derive that every local positive definite analytic function on a 1-connected Fr'echet--BCH--Lie group GGG extends to a global analytic function.

This mission is the statement-level formalization of On Analytic Vectors for Unitary Representations of Infinite Dimensional Lie Groups (arXiv:1002.4792v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

9 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Analytic functionals: seminorm and Banach norm criteria (Proposition 3.4, PDF p. 9). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

17 results of the paper are not stated yet, because the library lacks an interface they need:

  • Proposition 4.6: The actual smooth locally convex Lie group and its tangent Lie algebra, the smooth-vector subspace of the given continuous action on the same locally convex space V, and its computed tangent-derived action with values in that subspace. (hard)
  • Theorem 5.1: A paper-local locally convex analytic manifold interface: complexifications, continuous iterated directional derivatives, local holomorphic extension, actual tangent spaces and chart transitions. (hard)
  • Theorem 5.2: Analytic Frechet Lie groups in the source's locally convex calculus, continuous unitary actions on arbitrary complex Hilbert spaces, analytic full orbit maps, and their computed diagonal coefficients. No BCH hypothesis or derived-action interface is needed to state this criterion. (hard)
  • Corollary 5.3: Real analyticity of scalar functions on analytic Frechet Lie groups, local analyticity at the identity, and positive definiteness of the computed group kernel. No BCH, connectedness, tangent-derived action, or given Hilbert realization is needed to state the corollary. (hard)
  • Proposition 6.3: The canonical complexified enveloping algebra with its antilinear anti-automorphism x*=−x, canonical complex-linear extension of the given action, and positive coefficient functionals. (hard)
  • Proposition 6.5: The canonical complexified enveloping algebra with its antilinear anti-automorphism x*=−x, canonical complex-linear extension of the given action, and positive coefficient functionals. The canonical GNS construction from the supplied positive functional: null-space quotient, pre-Hilbert completion H_lambda, dense cyclic invariant domain D_lambda, and computed right regular action rho_lambda. (hard)
  • Lemma 6.7: A convergent BCH Lie algebra interface in the locally convex holomorphic calculus, linked to actual unitary Stone flows with full graph-closure generators. (hard)
  • Theorem 6.8: Actual BCH/analytic Lie group structure and tangent Lie algebra identification, exponential curves, smooth and analytic orbit maps, and derived actions computed from the same continuous representation on the same Hilbert space. A convergent BCH Lie algebra interface in the locally convex holomorphic calculus, linked to actual unitary Stone flows with full graph-closure generators. (hard)
  • Lemma 6.9: The canonical complexified enveloping algebra with its antilinear anti-automorphism x*=−x, canonical complex-linear extension of the given action, and positive coefficient functionals. The canonical GNS construction from the supplied positive functional: null-space quotient, pre-Hilbert completion H_lambda, dense cyclic invariant domain D_lambda, and computed right regular action rho_lambda. (hard)
  • Unnumbered assertion before Theorem 6.10: An analytic locally convex Lie group with its actual tangent Lie algebra, smooth and analytic orbit maps for the same continuous unitary action on the same Hilbert space, and the canonical complex enveloping extension of its derived action with antilinear anti-automorphism x*=−x. No BCH or connectedness hypothesis is required. (hard)
  • Theorem 6.10: Actual BCH/analytic Lie group structure and tangent Lie algebra identification, exponential curves, smooth and analytic orbit maps, and derived actions computed from the same continuous representation on the same Hilbert space. The canonical complexified enveloping algebra with its antilinear anti-automorphism x*=−x, canonical complex-linear extension of the given action, and positive coefficient functionals. The canonical GNS construction from the supplied positive functional: null-space quotient, pre-Hilbert completion H_lambda, dense cyclic invariant domain D_lambda, and computed right regular action rho_lambda. (hard)
  • Corollary 6.11: Actual BCH/analytic Lie group structure and tangent Lie algebra identification, exponential curves, smooth and analytic orbit maps, and derived actions computed from the same continuous representation on the same Hilbert space. The canonical complexified enveloping algebra with its antilinear anti-automorphism x*=−x, canonical complex-linear extension of the given action, and positive coefficient functionals. The canonical GNS construction from the supplied positive functional: null-space quotient, pre-Hilbert completion H_lambda, dense cyclic invariant domain D_lambda, and computed right regular action rho_lambda. (hard)
  • Theorem 6.12: Actual BCH/analytic Lie group structure and tangent Lie algebra identification, exponential curves, smooth and analytic orbit maps, and derived actions computed from the same continuous representation on the same Hilbert space. A convergent BCH Lie algebra interface in the locally convex holomorphic calculus, linked to actual unitary Stone flows with full graph-closure generators. (hard)
  • Example 6.14: A source-consistent real multiplication representation and a probability-space assumption forcing nondiscreteness. (source-ambiguity)
  • Remark 6.15: An abelian Banach Lie group with actual exponential curves, a continuous unitary action with dense analytic full orbit vectors, and its computed closed kernel and exponential Lie algebra {x : for all real t, pi(exp(t*x))=1}. The kernel is not assumed an embedded Lie subgroup. (hard)
  • Lemma 7.2: A paper-local locally convex analytic manifold interface: complexifications, continuous iterated directional derivatives, local holomorphic extension, actual tangent spaces and chart transitions. (hard)
  • Theorem 7.3: Analytic Frechet BCH Lie groups and scalar analyticity in the source's locally convex calculus; a connected open identity neighborhood V, the full domain V*V-inverse, its local positive definite kernel, and global positive definite analytic extension. A group representation or derived action is not part of the data needed to state the result. (hard)

Selected references

  • On Analytic Vectors for Unitary Representations of Infinite Dimensional Lie Groups, arXiv:1002.4792v2, https://arxiv.org/abs/1002.4792v2
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