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Linear algebra

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AlgebraCombinatoricsDiscrete Geometry·Captain: mikedeng1

Maximum Scattered Linear Sets and Complete Caps in Galois Spaces 1: Scattered 𝔽_q-Linear Sets of Rank rt/2 Exist in PG(r − 1, q^t) for t Even, in Three Families of (q, t)Research Paper

Motivation

Linear sets are the main tool for building point sets with few intersection sizes in finite projective spaces: sets meeting every hyperplane, two-intersection sets, translation ovoids, and the geometric side of finite semifields and rank-metric codes (Polverino, 2010). Among them, scattered linear sets are those whose points all carry the smallest possible weight, and a scattered linear set of the largest possible rank is called maximum scattered. By Blokhuis and Lavrauw (2000), a maximum scattered linear set of PG(r−1,qt)\mathrm{PG}(r-1,q^t)PG(r−1,qt) of rank rt/2rt/2rt/2 is a two-intersection set with respect to hyperplanes, so each one yields a two-weight code and a strongly regular graph.

Timeline.

  • 2000, Blokhuis–Lavrauw: the rank of a scattered Fq\mathbb F_qFq​-linear set of PG(r−1,qt)\mathrm{PG}(r-1,q^t)PG(r−1,qt) is at most rt/2rt/2rt/2, and for rrr even this bound is attained.
  • 2000, Ball–Blokhuis–Lavrauw: examples of rank 666 in PG(2,q4)\mathrm{PG}(2,q^4)PG(2,q4).
  • Classical: for r=3r=3r=3, t=2t=2t=2 the bound 333 is attained by Baer subplanes.
  • 2000, Blokhuis–Lavrauw, Thm 4.4: existence (without explicit examples) for r>3r>3r>3, t=2t=2t=2, q=2q=2q=2 and for r≥3r\ge3r≥3, (t−1)∣r(t-1)\mid r(t−1)∣r, ttt even, q>2q>2q>2.
  • 2015, Bartoli, Giulietti, Marino and Polverino (arXiv:1512.07467v1, Combinatorica 37 (2017)): three explicit families in PG(2,q2n)\mathrm{PG}(2,q^{2n})PG(2,q2n) and, by direct sums, maximum scattered linear sets in PG(r−1,qt)\mathrm{PG}(r-1,q^t)PG(r−1,qt) for ttt even in three families of (q,t)(q,t)(q,t). This mission formalizes that result; the companion mission formalizes the paper's application to complete caps.

Setting

Let qqq be a prime power, t≥1t\ge1t≥1, and let VVV be an rrr-dimensional vector space over Fqt\mathbb F_{q^t}Fqt​; PG(V,Fqt)=PG(r−1,qt)\mathrm{PG}(V,\mathbb F_{q^t})=\mathrm{PG}(r-1,q^t)PG(V,Fqt​)=PG(r−1,qt) has as points the spans ⟨v⟩Fqt\langle v\rangle_{\mathbb F_{q^t}}⟨v⟩Fqt​​ of nonzero v∈Vv\in Vv∈V. An Fq\mathbb F_qFq​-subspace U⊆VU\subseteq VU⊆V is a subset closed under addition and under multiplication by Fq\mathbb F_qFq​. It defines the Fq\mathbb F_qFq​-linear set

LU={⟨u⟩Fqt:u∈U∖{0}},L_U=\{\langle u\rangle_{\mathbb F_{q^t}} : u\in U\setminus\{0\}\},LU​={⟨u⟩Fqt​​:u∈U∖{0}},

whose rank is dim⁡FqU\dim_{\mathbb F_q}UdimFq​​U. A linear set comes paired with UUU, so every statement here is about UUU. The weight of a point ⟨v⟩\langle v\rangle⟨v⟩ is dim⁡Fq(⟨v⟩Fqt∩U)\dim_{\mathbb F_q}(\langle v\rangle_{\mathbb F_{q^t}}\cap U)dimFq​​(⟨v⟩Fqt​​∩U), and LUL_ULU​ is scattered when every point of LUL_ULU​ has weight 111; equivalently, for every nonzero u∈Uu\in Uu∈U,

λ∈Fqt, λu∈U ⟹ λ∈Fq.\lambda\in\mathbb F_{q^t},\ \lambda u\in U\ \Longrightarrow\ \lambda\in\mathbb F_q .λ∈Fqt​, λu∈U ⟹ λ∈Fq​.

The plane construction (§2). Fix n≥2n\ge2n≥2 and the field E=Fq6nE=\mathbb F_{q^{6n}}E=Fq6n​ with its subfields Fq⊆Fqn⊆Fq2n\mathbb F_q\subseteq\mathbb F_{q^n}\subseteq\mathbb F_{q^{2n}}Fq​⊆Fqn​⊆Fq2n​ and Fq3n\mathbb F_{q^{3n}}Fq3n​. As an Fq2n\mathbb F_{q^{2n}}Fq2n​-space EEE has dimension 333, so PG(E,Fq2n)=PG(2,q2n)\mathrm{PG}(E,\mathbb F_{q^{2n}})=\mathrm{PG}(2,q^{2n})PG(E,Fq2n​)=PG(2,q2n). For ω∈Fq2n∖Fqn\omega\in\mathbb F_{q^{2n}}\setminus\mathbb F_{q^n}ω∈Fq2n​∖Fqn​ and an Fq\mathbb F_qFq​-linear f:Fq3n→Fq3nf:\mathbb F_{q^{3n}}\to\mathbb F_{q^{3n}}f:Fq3n​→Fq3n​ the paper studies

Uf={f(x)+xω:x∈Fq3n},U_f=\{f(x)+x\omega : x\in\mathbb F_{q^{3n}}\},Uf​={f(x)+xω:x∈Fq3n​},

with fff a monomial axqiax^{q^i}axqi or a binomial fi,a,b(x)=axqi+bxq2n+if_{i,a,b}(x)=ax^{q^i}+bx^{q^{2n+i}}fi,a,b​(x)=axqi+bxq2n+i. The relative norms Nqm/qd(x)=∏j<m/dxqdjN_{q^m/q^d}(x)=\prod_{j<m/d}x^{q^{dj}}Nqm/qd​(x)=∏j<m/d​xqdj enter the hypotheses.

Formalization targets

Goal: Theorem 1.2 (p. 3)

For ttt even and r≥2r\ge2r≥2, in each of the cases (a) q=2q=2q=2, t≥4t\ge4t≥4; (b) t≢0(mod3)t\not\equiv0\pmod3t≡0(mod3); (c) q≡1(mod3)q\equiv1\pmod3q≡1(mod3), t≡0(mod3)t\equiv0\pmod3t≡0(mod3),

∃ U⊆Fqt r  Fq-subspace:dim⁡FqU=rt2,LU scattered.\exists\,U\subseteq\mathbb F_{q^t}^{\,r}\ \ \mathbb F_q\text{-subspace}:\qquad \dim_{\mathbb F_q}U=\frac{rt}{2},\quad L_U\ \text{scattered}.∃U⊆Fqtr​  Fq​-subspace:dimFq​​U=2rt​,LU​ scattered.

Milestones, in proof order

  • Proposition 2.1 (p. 5): UfU_fUf​ has rank 3n3n3n, and LUfL_{U_f}LUf​​ is scattered iff Qf∩Fq2n=FqQ_f\cap\mathbb F_{q^{2n}}=\mathbb F_qQf​∩Fq2n​=Fq​, where QfQ_fQf​ is the set of quotients f(x)+xωf(y)+yω\frac{f(x)+x\omega}{f(y)+y\omega}f(y)+yωf(x)+xω​, y≠0y\ne0y=0.
  • Proposition 2.2 (p. 6): the same criterion through the polynomial system (5)–(6).
  • Theorems 2.3, 2.4 (pp. 7, 9): the monomial families, for n≢0(mod3)n\not\equiv0\pmod 3n≡0(mod3) and for q≡1(mod3)q\equiv1\pmod3q≡1(mod3).
  • Theorem 2.5 (p. 10): existence in PG(2,q2n)\mathrm{PG}(2,q^{2n})PG(2,q2n) in those two regimes.
  • Lemma 2.6 (p. 11): φ(x)/x\varphi(x)/xφ(x)/x and φˉ(x)/x\bar\varphi(x)/xφˉ​(x)/x have the same image, where φˉ\bar\varphiφˉ​ is the trace adjoint.
  • Proposition 2.7, Lemma 2.8, Proposition 2.9, Theorem 2.10 (pp. 12–16): the binomial family for q=2q=2q=2.
  • Theorem 3.1 (p. 16): direct sums of scattered linear sets are scattered, of rank rt/2rt/2rt/2 iff each summand has rank sit/2s_it/2si​t/2.
  • The line example (p. 2, cited from Lavrauw's thesis) and the Baer-subplane case r=3r=3r=3, t=2t=2t=2 (p. 3).

Significance

Theorem 1.2 gives maximum scattered linear sets, and hence two-intersection sets, two-weight codes and strongly regular graphs, for infinitely many (q,t)(q,t)(q,t) with rrr odd, a regime where earlier existence results covered only a few values of ttt. The q=2q=2q=2 case feeds the paper's second main result: scattered F2\mathbb F_2F2​-linear sets of PG(2,2t)\mathrm{PG}(2,2^t)PG(2,2t) of rank 3t/23t/23t/2 are translation caps, from which complete caps of size 2q n−12\sqrt{q^{\,n-1}}2qn−1​ in AG(n,q)\mathrm{AG}(n,q)AG(n,q) are built.

All statements are proved in the preprint; none has a machine-checked proof. Formalizing them requires a usable theory of subfields of a finite field as Frobenius fixed fields, relative norms and their images, linearized polynomials and their trace adjoints, and the passage between Fq\mathbb F_qFq​-dimension, cardinality and weight. Each of these is reusable for later work on linear sets, MRD codes and semifields.

Difficulty

The criterion of Proposition 2.2 reduces scatteredness to a polynomial system, but the system has to be solved for a specific fff. For the monomials this rests on the solvability of zqi−1=cz^{q^i-1}=czqi−1=c in Fq3n\mathbb F_{q^{3n}}Fq3n​, a norm condition interacting with the gcd hypotheses. For the binomial with q=2q=2q=2, the existence of a suitable bbb (Lemma 2.8) needs a value-set bound for non-permutation polynomials (Turnwald, 1995) and a point count on a plane curve. The higher-dimensional statement then needs the elementary bound dim⁡U≤st/2\dim U\le st/2dimU≤st/2 for scattered UUU to obtain the rank equivalence in Theorem 3.1. A tempting shortcut, taking U=Fq rU=\mathbb F_q^{\,r}U=Fqr​ or any small subspace, is scattered but has the wrong rank; the content is in the rank rt/2rt/2rt/2.

Formalization scope

  • Citation basis. arXiv:1512.07467v1; page numbers equal PDF pages.
  • Fields. Fqm⊆E\mathbb F_{q^m}\subseteq EFqm​⊆E is the fixed field of x↦xqmx\mapsto x^{q^m}x↦xqm in a finite field EEE of characteristic ppp with ∣E∣=q6n|E|=q^{6n}∣E∣=q6n, q=phq=p^hq=ph. Norms and traces are explicit Frobenius products and sums.
  • Subspaces and rank. An Fq\mathbb F_qFq​-subspace is a carrier set with closure conditions. Rank kkk is ∣U∣=qk|U|=q^k∣U∣=qk; in Theorem 3.1 rank rt/2rt/2rt/2 is ∣W∣2=qrt|W|^2=q^{rt}∣W∣2=qrt.
  • Points. Scatteredness takes the spanning field as an argument: Fq2n\mathbb F_{q^{2n}}Fq2n​ in §2, the whole Fqt\mathbb F_{q^t}Fqt​ in Theorem 1.2 and §3. PG(r−1,qt)\mathrm{PG}(r-1,q^t)PG(r−1,qt) is modelled on Fin r → K; the plane of §2 on EEE itself.
  • Pinned readings.
    • Theorem 1.2 prints no range for rrr. The preceding sentence and the proof (p. 17) say r≥5r\ge5r≥5, and r=1r=1r=1 is false. The goal assumes r≥2r\ge2r≥2, covered by the line example (r=2r=2r=2), §2 with the Baer case (r=3r=3r=3) and Theorem 3.1 (r≥4r\ge4r≥4).
    • ω\omegaω is quantified over all of Fq2n∖Fqn\mathbb F_{q^{2n}}\setminus\mathbb F_{q^n}Fq2n​∖Fqn​.
    • The index ranges 1≤i≤3n−11\le i\le3n-11≤i≤3n−1 (monomial) and 2n+i≤3n−12n+i\le3n-12n+i≤3n−1 (binomial) come from the case headings on pp. 7 and 10.
    • Proposition 2.7's printed "wxwxwx" is ωx\omega xωx.
    • Theorem 2.10 keeps its printed hypothesis N23n/2n(b)≠1N_{2^{3n}/2^n}(b)\ne1N23n/2n​(b)=1.
    • Theorem 3.1's rank clause assumes t≥2t\ge2t≥2; for t=1t=1t=1 it is false.
  • Ruled out. Taking the span over EEE or over Fq\mathbb F_qFq​, or dropping the rank, would make the statements false or trivial; every existence statement fixes the rank, and the span field is explicit.
  • Contributions welcome. Frobenius-fixed-field cardinalities, norm surjectivity, the criteria of Propositions 2.1–2.2, the monomial and binomial families, and the direct-sum rank computation.

Selected references

  • D. Bartoli, M. Giulietti, G. Marino, O. Polverino, Maximum scattered linear sets and complete caps in Galois spaces, arXiv:1512.07467v1 (2015); Combinatorica 37 (2017). https://arxiv.org/abs/1512.07467, https://doi.org/10.1007/s00493-016-3531-6
  • A. Blokhuis, M. Lavrauw, Scattered spaces with respect to a spread in PG(n, q), Geom. Dedicata 81 (2000), 231–243. https://doi.org/10.1023/A:1005283806897
  • O. Polverino, Linear sets in finite projective spaces, Discrete Math. 310 (2010), 3096–3107. https://doi.org/10.1016/j.disc.2010.04.007
  • S. Ball, A. Blokhuis, M. Lavrauw, Linear (q + 1)-fold blocking sets in PG(2, q⁴), Finite Fields Appl. 6 (2000), 294–301.
  • M. Lavrauw, Scattered Spaces with respect to Spreads and Eggs in Finite Projective Spaces, Ph.D. thesis, TU Eindhoven, 2001.
  • G. Turnwald, A new criterion for permutation polynomials, Finite Fields Appl. 1 (1995), 64–82.
15 thms1 active userReviewed
Complexity TheoryGraph TheoryOptimization+1·Captain: mikedeng1

Most Tensor Problems Are NP-Hard 5: The Stability Number Is Read Off the Largest Eigenvalue of an Explicit Symmetric 3-TensorResearch Paper

Motivation

For a real symmetric matrix, the largest eigenvalue is the maximum of the quadratic form x⊤Ax\mathbf x^\top A\mathbf xx⊤Ax on the unit sphere, and it is computable to any accuracy in polynomial time. Tensor eigenvalues, introduced independently by Lim (2005) and Qi (2005), extend this picture to higher order: they are the stationary values of the cubic form A(x,x,x)\mathcal A(\mathbf x,\mathbf x,\mathbf x)A(x,x,x) on the unit sphere. They appear in multilinear statistics, signal processing, hypergraph theory and polynomial optimization, and for these applications the symmetric case is the natural one.

Hillar and Lim, in Most Tensor Problems Are NP-Hard (J. ACM 2013), show that the eigenvalue problem stays NP-hard when the tensor is required to be symmetric (their Theorem 9.3). The proof is short once one ingredient is available: a theorem of Nesterov (2003), in a form corrected by Hillar and Lim, that expresses the stability number of a graph as the maximum of an explicit cubic polynomial over a sphere. This mission formalizes that chain.

Setting

Let G=(V,E)G=(V,E)G=(V,E) be a simple graph on V={1,…,v}V=\{1,\dots,v\}V={1,…,v}, v≥1v\ge1v≥1. A set of vertices is stable if no two of its members are adjacent; the stability number α(G)\alpha(G)α(G) is the size of a largest stable set, so 1≤α(G)≤v1\le\alpha(G)\le v1≤α(G)≤v.

Put n=v+v(v−1)/2n=v+v(v-1)/2n=v+v(v−1)/2 and write a vector of Rn\mathbb R^nRn as z=(x,y)\mathbf z=(\mathbf x,\mathbf y)z=(x,y), with x=(x1,…,xv)\mathbf x=(x_1,\dots,x_v)x=(x1​,…,xv​) indexed by vertices and y=(yij)i<j\mathbf y=(y_{ij})_{i<j}y=(yij​)i<j​ indexed by pairs of vertices. The tensor SG=[ ⁣[sabc] ⁣]∈Rn×n×n\mathcal S_G=[\![s_{abc}]\!]\in\mathbb R^{n\times n\times n}SG​=[[sabc​]]∈Rn×n×n has entry 111 at the six orderings of the triple of coordinates (xi,xj,yij)(x_i,x_j,y_{ij})(xi​,xj​,yij​) for every non-adjacent pair i<ji<ji<j, and 000 elsewhere. It is symmetric: its entries do not change under any permutation of the three indices.

For a real 3-tensor A=[ ⁣[aabc] ⁣]\mathcal A=[\![a_{abc}]\!]A=[[aabc​]] the cubic form is A(z,z,z)=∑a,b,caabczazbzc\mathcal A(\mathbf z,\mathbf z,\mathbf z)=\sum_{a,b,c}a_{abc}z_az_bz_cA(z,z,z)=∑a,b,c​aabc​za​zb​zc​, and a real λ\lambdaλ is a unit ℓ2\ell^2ℓ2-eigenvalue of A\mathcal AA if

∑a,baabczazb=λzcfor all c,for some z with ∥z∥2=1.\sum_{a,b}a_{abc}z_az_b=\lambda z_c\quad\text{for all }c,\qquad\text{for some }\mathbf z\text{ with }\|\mathbf z\|_2=1 .a,b∑​aabc​za​zb​=λzc​for all c,for some z with ∥z∥2​=1.

Finally, λl=223(1−1l)\lambda_l=2\sqrt{\tfrac23\left(1-\tfrac1l\right)}λl​=232​(1−l1​)​ for l≥1l\ge1l≥1. In Lean these are TensorNP.SymEigen.stabTensor, cubicForm, IsUnitL2Eigenvalue and lambdaL, and α(G)\alpha(G)α(G) is Mathlib's SimpleGraph.indepNum.

Formalization targets

Goal: Theorem 9.3, core

α(G)=max⁡{ l∈{1,…,v}: λl is a unit ℓ2-eigenvalue of SG }.\alpha(G)=\max\{\,l\in\{1,\dots,v\}:\ \lambda_l\text{ is a unit }\ell^2\text{-eigenvalue of }\mathcal S_G\,\}.α(G)=max{l∈{1,…,v}: λl​ is a unit ℓ2-eigenvalue of SG​}.

That is, λα(G)\lambda_{\alpha(G)}λα(G)​ is an eigenvalue of SG\mathcal S_GSG​, and no λl\lambda_lλl​ with α(G)<l≤v\alpha(G)<l\le vα(G)<l≤v is. This is the statement on which the paper's vvv-query reduction rests; nothing is claimed about l<α(G)l<\alpha(G)l<α(G).

Milestones, in the paper's order

  1. Theorem 9.2 (Nesterov). With Sn−1={(x,y):∥x∥22+∥y∥22=1}\mathbb S^{n-1}=\{(\mathbf x,\mathbf y):\|\mathbf x\|_2^2+\|\mathbf y\|_2^2=1\}Sn−1={(x,y):∥x∥22​+∥y∥22​=1},
1−1α(G)=332⋅max⁡(x,y)∈Sn−1 ∑i<j, {i,j}∉Exixjyij.\sqrt{1-\frac1{\alpha(G)}}=3\sqrt{\frac32}\cdot\max_{(\mathbf x,\mathbf y)\in\mathbb S^{n-1}}\ \sum_{i<j,\ \{i,j\}\notin E}x_ix_jy_{ij}.1−α(G)1​​=323​​⋅(x,y)∈Sn−1max​ i<j, {i,j}∈/E∑​xi​xj​yij​.
  1. The tensor. SG\mathcal S_GSG​ is symmetric and SG(z,z,z)=6∑i<j,{i,j}∉Exixjyij\mathcal S_G(\mathbf z,\mathbf z,\mathbf z)=6\sum_{i<j,\{i,j\}\notin E}x_ix_jy_{ij}SG​(z,z,z)=6∑i<j,{i,j}∈/E​xi​xj​yij​.
  2. The maximum is an eigenvalue. max⁡∥z∥2=1SG(z,z,z)\max_{\|\mathbf z\|_2=1}\mathcal S_G(\mathbf z,\mathbf z,\mathbf z)max∥z∥2​=1​SG​(z,z,z) is attained and is a unit ℓ2\ell^2ℓ2-eigenvalue of SG\mathcal S_GSG​.
  3. Its value. max⁡∥z∥2=1SG(z,z,z)=λα(G)\max_{\|\mathbf z\|_2=1}\mathcal S_G(\mathbf z,\mathbf z,\mathbf z)=\lambda_{\alpha(G)}max∥z∥2​=1​SG​(z,z,z)=λα(G)​.
  4. Further result: Theorem 6.9 (Banach), (23). For every symmetric S∈Rn×n×n\mathcal S\in\mathbb R^{n\times n\times n}S∈Rn×n×n,
sup⁡x,y,z≠0∣S(x,y,z)∣∥x∥2∥y∥2∥z∥2=sup⁡x≠0∣S(x,x,x)∣∥x∥23,\sup_{\mathbf x,\mathbf y,\mathbf z\ne\mathbf 0}\frac{|\mathcal S(\mathbf x,\mathbf y,\mathbf z)|}{\|\mathbf x\|_2\|\mathbf y\|_2\|\mathbf z\|_2}=\sup_{\mathbf x\ne\mathbf 0}\frac{|\mathcal S(\mathbf x,\mathbf x,\mathbf x)|}{\|\mathbf x\|_2^3},x,y,z=0sup​∥x∥2​∥y∥2​∥z∥2​∣S(x,y,z)∣​=x=0sup​∥x∥23​∣S(x,x,x)∣​,

both sides finite. The paper uses it in §10 to transfer Theorem 9.3 to the spectral norm and the best rank-one approximation of symmetric tensors.

Significance

The result. Theorem 9.3 places symmetric tensor eigenvalue among the NP-hard problems of Hillar and Lim's Table I, and through Banach's theorem (Theorem 10.2 of the paper) the same holds for the largest singular value, the spectral norm and the best rank-one approximation of a symmetric 3-tensor. These are the quantities computed by higher-order power methods and by moment-based estimators, so the result marks where the matrix theory stops transferring.

Formalizing it. All results here are proved in the literature; none is machine-checked. Nesterov's theorem, which rests on the Motzkin–Straus theorem for the complement graph, is not on the platform or in Mathlib, and its formal statement settles the constant that the original paper got wrong by a factor 1/21/\sqrt21/2​ (Hillar–Lim, footnote 12). Banach's theorem on symmetric multilinear forms is likewise absent from Mathlib and is useful well beyond this mission.

Difficulty

The tensor identity (milestone 2) is bookkeeping. The analytic content sits in two places. First, Nesterov's theorem: the obvious route, fixing x\mathbf xx and maximizing over y\mathbf yy by Cauchy–Schwarz, reduces the cubic problem to a quartic one in x\mathbf xx, whose value still has to be identified with α(G)\alpha(G)α(G); that identification is the Motzkin–Straus theorem, which is not available in Lean and is itself a nontrivial optimization over the simplex. Second, the passage from a maximum to an eigenvalue needs a Lagrange multiplier argument on the sphere, and the symmetry of SG\mathcal S_GSG​ is what makes the gradient of the cubic form match the eigen-equation. Part (b) of the goal needs a further, unprinted observation relating every unit eigenpair to the cubic form. Banach's theorem has no short proof; the classical arguments go through polarization estimates or a variational argument specific to symmetric forms.

Formalization scope

  • Tensors and indices. A 3-tensor is a function ι → ι → ι → ℝ on a finite index type. For SG\mathcal S_GSG​ the index type is the disjoint union of the vertices Fin v and the pairs {(i,j):i<j}\{(i,j): i<j\}{(i,j):i<j}; this is Rn\mathbb R^nRn with coordinates labelled by name instead of by the paper's enumeration φ(i,j)=(i−1)v−i(i−1)/2+j−i\varphi(i,j)=(i-1)v-i(i-1)/2+j-iφ(i,j)=(i−1)v−i(i−1)/2+j−i. Vertices are 0,…,v−10,\dots,v-10,…,v−1.
  • Normalization. Eigenvalues are taken with a unit eigenvector. The paper's Problem 9.1 and Definition 5.1 say only x≠0\mathbf x\ne\mathbf 0x=0; since (λ,x)↦(tλ,tx)(\lambda,\mathbf x)\mapsto(t\lambda,t\mathbf x)(λ,x)↦(tλ,tx) preserves the eigen-equation, that reading would make every nonzero real an eigenvalue of SG\mathcal S_GSG​ and the goal false. The unit sphere (13) is where the paper derives the notion.
  • Explicit readings. The paper's index range "1≤i<j<k≤v1\le i<j<k\le v1≤i<j<k≤v" in the definition of sijks_{ijk}sijk​ is read as k≤nk\le nk≤n (taken literally it gives SG=0\mathcal S_G=0SG​=0). Every "max" is stated as a greatest element, so attainment is claimed. In (23) the suprema are real suprema over nonzero vectors with boundedness part of the conclusion. v≥1v\ge1v≥1 is assumed wherever the paper uses α(G)∈{1,…,v}\alpha(G)\in\{1,\dots,v\}α(G)∈{1,…,v}.
  • Not formalized. The oracle procedure of the proof of Theorem 9.3, the polynomial size of SG\mathcal S_GSG​, the input model of Problem 9.1 with quadratic irrationalities (Remark 9.4), and the NP-completeness of the stability number (Karp 1972, via α(G)=ω(G‾)\alpha(G)=\omega(\overline G)α(G)=ω(G)). The goal is the mathematical core of the Turing reduction, not a complexity statement.
  • Trivializations ruled out. Without the unit normalization the eigenvalue statements are trivial or false; a goal stating only (a), or only an inequality between the maximum and λα(G)\lambda_{\alpha(G)}λα(G)​, would not determine α(G)\alpha(G)α(G); both are excluded by the statements above.
  • Infrastructure. Everything rests on Mathlib (SimpleGraph.indepNum, real analysis on finite-dimensional spaces, Lagrange multipliers). A Motzkin–Straus theorem for SimpleGraph and Banach's theorem for symmetric trilinear forms are both reusable beyond this mission; contributions of either, or of a general "maximum of a symmetric cubic form on the sphere is an eigenvalue" lemma, are welcome.

Selected references

  • C. J. Hillar, L.-H. Lim, Most Tensor Problems Are NP-Hard, Journal of the ACM 60(6), Article 45, 2013. https://doi.org/10.1145/2512329 (arXiv:0911.1393v5: https://arxiv.org/abs/0911.1393)
  • Yu. Nesterov, Random walk in a simplex and quadratic optimization over convex polytopes, CORE Discussion Paper 2003/71, 2003. http://edoc.bib.ucl.ac.be:83/archive/00000238/01/dp2003-71.pdf
  • E. de Klerk, The complexity of optimizing over a simplex, hypercube or sphere: a short survey, Central European Journal of Operations Research 16, 111–125, 2008. https://doi.org/10.1007/s10100-007-0052-9
  • T. S. Motzkin, E. G. Straus, Maxima for graphs and a new proof of a theorem of Turán, Canadian Journal of Mathematics 17, 533–540, 1965. https://doi.org/10.4153/CJM-1965-053-6
  • S. Banach, Über homogene Polynome in (L2L^2L2), Studia Mathematica 7(1), 36–44, 1938 (reference [Banach 1938] of Hillar–Lim).
  • L.-H. Lim, Singular values and eigenvalues of tensors: a variational approach, Proc. IEEE CAMSAP 1, 129–132, 2005. https://arxiv.org/abs/math/0607648
  • L. Qi, Eigenvalues of a real supersymmetric tensor, Journal of Symbolic Computation 40, 1302–1324, 2005. https://doi.org/10.1016/j.jsc.2005.05.007
  • R. M. Karp, Reducibility among combinatorial problems, in Complexity of Computer Computations, 85–103, 1972. https://doi.org/10.1007/978-1-4684-2001-2_9
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Complexity TheoryGraph TheoryOptimization+1·Captain: mikedeng1

Most Tensor Problems Are NP-Hard 3: The Clique Number Is the Unique l for Which an Explicit Graph Tensor Has Spectral Norm 1Research Paper

Motivation

The spectral norm of a matrix, its largest singular value, is computable in polynomial time to any accuracy. Its analogue for 3-tensors appears in the analysis of multilinear systems, in the best rank-1 approximation of a data array, in quantum information (the geometric measure of entanglement), and in the injective norm of tensor products. Hillar and Lim, Most Tensor Problems Are NP-Hard (J. ACM 60(6), 2013, Article 45; final version arXiv:0911.1393v5), show that, in contrast with matrices, deciding whether a fixed nonzero rational number is a singular value or the spectral norm of a rational 3-tensor is NP-hard (their Theorems 6.5 and 1.10).

The proof is a reduction from the clique number ω(G)\omega(G)ω(G) of a graph. It combines three classical ingredients: the theorem of Motzkin and Straus (1965), which expresses ω(G)\omega(G)ω(G) as the value of a quadratic program over the simplex; a theorem of Banach (1938) on the spectral norm of symmetric tensors; and an observation from He, Li and Zhang (2010) on maxima of sums of squared bilinear forms. Deciding ω(G)≥l\omega(G)\ge lω(G)≥l is one of Karp's (1972) NP-complete problems.

Setting

A real 3-tensor is an array A=[ ⁣[aijk] ⁣]∈Rl×m×n\mathcal A=[\![a_{ijk}]\!]\in\mathbb R^{l\times m\times n}A=[[aijk​]]∈Rl×m×n with trilinear form A(x,y,z)=∑i,j,kaijkxiyjzk\mathcal A(\mathbf x,\mathbf y,\mathbf z)=\sum_{i,j,k}a_{ijk}x_iy_jz_kA(x,y,z)=∑i,j,k​aijk​xi​yj​zk​. With the Euclidean norm ∥⋅∥2\|\cdot\|_2∥⋅∥2​, its spectral norm is

∥A∥2,2,2=sup⁡x,y,z≠0∣A(x,y,z)∣∥x∥2∥y∥2∥z∥2.\|\mathcal A\|_{2,2,2}=\sup_{\mathbf x,\mathbf y,\mathbf z\ne\mathbf 0}\frac{|\mathcal A(\mathbf x,\mathbf y,\mathbf z)|}{\|\mathbf x\|_2\|\mathbf y\|_2\|\mathbf z\|_2}.∥A∥2,2,2​=x,y,z=0sup​∥x∥2​∥y∥2​∥z∥2​∣A(x,y,z)∣​.

A real σ\sigmaσ is a unit ℓ2\ell^2ℓ2-singular value of A\mathcal AA if there are unit vectors u,v,w\mathbf u,\mathbf v,\mathbf wu,v,w with

∑j,kaijkvjwk=σui,∑i,kaijkuiwk=σvj,∑i,jaijkuivj=σwk\textstyle\sum_{j,k}a_{ijk}v_jw_k=\sigma u_i,\quad \sum_{i,k}a_{ijk}u_iw_k=\sigma v_j,\quad \sum_{i,j}a_{ijk}u_iv_j=\sigma w_k∑j,k​aijk​vj​wk​=σui​,∑i,k​aijk​ui​wk​=σvj​,∑i,j​aijk​ui​vj​=σwk​

for all i,j,ki,j,ki,j,k: the stationarity conditions of A(u,v,w)\mathcal A(\mathbf u,\mathbf v,\mathbf w)A(u,v,w) on a product of unit spheres.

Let G=(V,E)G=(V,E)G=(V,E) be a simple graph on V={1,…,v}V=\{1,\dots,v\}V={1,…,v}, v≥1v\ge1v≥1, with eee edges {ik,jk}\{i_k,j_k\}{ik​,jk​}, k=1,…,ek=1,\dots,ek=1,…,e, and clique number ω\omegaω. Let Δv\Delta_vΔv​ be the standard simplex, AGA_GAG​ the adjacency matrix and JJJ the all-ones matrix. For a positive integer lll set Ql=AG+1lJQ_l=A_G+\frac1lJQl​=AG​+l1​J and Ml=max⁡x∈Δvx⊤QlxM_l=\max_{\mathbf x\in\Delta_v}\mathbf x^\top Q_l\mathbf xMl​=maxx∈Δv​​x⊤Ql​x. Let Ek=12Eikjk+12EjkikE_k=\frac12E_{i_kj_k}+\frac12E_{j_ki_k}Ek​=21​Eik​jk​​+21​Ejk​ik​​, and let TlT_lTl​ be the maximum over unit u,v∈Rv\mathbf u,\mathbf v\in\mathbb R^vu,v∈Rv, w∈Rl+2e\mathbf w\in\mathbb R^{l+2e}w∈Rl+2e of the multilinear form

∑i=1l(u⊤1lIv)wi+∑k=1e(u⊤Ekv)wl+k+∑k=1e(u⊤Ekv)we+l+k.(26)\sum_{i=1}^l\Big(\mathbf u^\top\tfrac1lI\mathbf v\Big)w_i+\sum_{k=1}^e(\mathbf u^\top E_k\mathbf v)w_{l+k}+\sum_{k=1}^e(\mathbf u^\top E_k\mathbf v)w_{e+l+k}. \tag{26}i=1∑l​(u⊤l1​Iv)wi​+k=1∑e​(u⊤Ek​v)wl+k​+k=1∑e​(u⊤Ek​v)we+l+k​.(26)

The graph tensor Al∈Qv×v×(l+2e)\mathcal A_l\in\mathbb Q^{v\times v\times(l+2e)}Al​∈Qv×v×(l+2e) has as entry aijka_{ijk}aijk​ the coefficient of uivjwku_iv_jw_kui​vj​wk​ in (26).

Formalization targets

Goal: Theorems 6.5 and 1.10, encoding-free core

For every graph GGG on v≥1v\ge1v≥1 vertices and every enumeration of its edges:

∀l≥1: ∥Al∥2,2,2=1  ⟺  l=ω;1 is a unit singular value of Aω;∀l>ω: 1 is not one of Al,\forall l\ge1:\ \|\mathcal A_l\|_{2,2,2}=1\iff l=\omega;\qquad 1\text{ is a unit singular value of }\mathcal A_\omega;\qquad \forall l>\omega:\ 1\text{ is not one of }\mathcal A_l,∀l≥1: ∥Al​∥2,2,2​=1⟺l=ω;1 is a unit singular value of Aω​;∀l>ω: 1 is not one of Al​,

so ω\omegaω is the largest l∈{1,…,v}l\in\{1,\dots,v\}l∈{1,…,v} for which 111 is a unit singular value of Al\mathcal A_lAl​. The paper's vvv-query Turing reductions rest on exactly this.

Milestones (in attack order)

  1. Theorem 6.7 (Motzkin–Straus): 1−1/ω=2max⁡x∈Δv∑{i,j}∈Exixj1-1/\omega=2\max_{\mathbf x\in\Delta_v}\sum_{\{i,j\}\in E}x_ix_j1−1/ω=2maxx∈Δv​​∑{i,j}∈E​xi​xj​.
  2. (22): Ml=1+ω−llωM_l=1+\frac{\omega-l}{l\omega}Ml​=1+lωω−l​; so Mω=1M_\omega=1Mω​=1, Ml>1M_l>1Ml​>1 for l<ωl<\omegal<ω, Ml<1M_l<1Ml​<1 for l>ωl>\omegal>ω.
  3. Lemma 6.8: Ml=NlM_l=N_lMl​=Nl​, where Nl=max⁡∥u∥2=1{∑i=1l(u⊤1lIu)2+2∑k(u⊤Eku)2}N_l=\max_{\|\mathbf u\|_2=1}\{\sum_{i=1}^l(\mathbf u^\top\frac1lI\mathbf u)^2+2\sum_k(\mathbf u^\top E_k\mathbf u)^2\}Nl​=max∥u∥2​=1​{∑i=1l​(u⊤l1​Iu)2+2∑k​(u⊤Ek​u)2}.
  4. Theorem 6.9 (Banach), (24): for a symmetric 4-tensor, ∥S∥2,2,2,2=sup⁡x≠0∣S(x,x,x,x)∣/∥x∥24\|\mathcal S\|_{2,2,2,2}=\sup_{\mathbf x\neq\mathbf 0}|\mathcal S(\mathbf x,\mathbf x,\mathbf x,\mathbf x)|/\|\mathbf x\|_2^4∥S∥2,2,2,2​=supx=0​∣S(x,x,x,x)∣/∥x∥24​.
  5. Proposition 6.10 (He–Li–Zhang): for symmetric AkA_kAk​, max⁡∥u∥=∥v∥=1∑k(u⊤Akv)2=max⁡∥v∥=1∑k(v⊤Akv)2\max_{\|\mathbf u\|=\|\mathbf v\|=1}\sum_k(\mathbf u^\top A_k\mathbf v)^2=\max_{\|\mathbf v\|=1}\sum_k(\mathbf v^\top A_k\mathbf v)^2max∥u∥=∥v∥=1​∑k​(u⊤Ak​v)2=max∥v∥=1​∑k​(v⊤Ak​v)2.
  6. Lemma 6.11: Tl=Ml1/2T_l=M_l^{1/2}Tl​=Ml1/2​, hence Tl=1T_l=1Tl​=1 iff l=ωl=\omegal=ω, Tl>1T_l>1Tl​>1 iff l<ωl<\omegal<ω, Tl<1T_l<1Tl​<1 iff l>ωl>\omegal>ω.
  7. Proof of Theorem 6.5: ∥Al∥2,2,2=Tl\|\mathcal A_l\|_{2,2,2}=T_l∥Al​∥2,2,2​=Tl​, TlT_lTl​ is a unit singular value of Al\mathcal A_lAl​, and every unit singular value has absolute value at most TlT_lTl​.
  8. §7 (content of Theorem 1.13): min⁡σ≥0, unit u,v,w∥A−σ u⊗v⊗w∥F2=∥A∥F2−∥A∥2,2,22\min_{\sigma\ge0,\ \text{unit }\mathbf u,\mathbf v,\mathbf w}\|\mathcal A-\sigma\,\mathbf u\otimes\mathbf v\otimes\mathbf w\|_F^2=\|\mathcal A\|_F^2-\|\mathcal A\|_{2,2,2}^2minσ≥0, unit u,v,w​∥A−σu⊗v⊗w∥F2​=∥A∥F2​−∥A∥2,2,22​, attained only with σ=∥A∥2,2,2\sigma=\|\mathcal A\|_{2,2,2}σ=∥A∥2,2,2​.

Significance

The result. The goal shows that a single comparison with 111 of the spectral norm, or of the singular-value spectrum, of an explicit rational tensor of size v×v×(l+2e)v\times v\times(l+2e)v×v×(l+2e) encodes whether l=ω(G)l=\omega(G)l=ω(G). It is the step that makes the spectral norm, the largest singular value, and (through §7) the best rank-1 approximation of a 3-tensor NP-hard, whereas all three are polynomial-time for matrices. It explains why the higher-order power method and its relatives carry no global guarantees, and it is the starting point for inapproximability results such as the paper's Theorem 1.11.

Formalizing it. The results are proved on paper; none of them is formalized. Motzkin–Straus, Banach's polarization theorem for symmetric 4-tensors, and the He–Li–Zhang identity are classical results that are not in Mathlib and not on the platform; each is reusable well beyond this mission (Turán-type bounds, polynomial optimization over spheres, injective norms). The mission also checks the paper's construction at the level of indices and constants.

Difficulty

The construction of Al\mathcal A_lAl​ is explicit, and the comparison with 111 is arithmetic once Tl=Ml1/2T_l=M_l^{1/2}Tl​=Ml1/2​ is known. Everything rests on the three cited theorems. Motzkin–Straus is an optimization statement over the simplex whose maximizers may lie on the boundary and need not be unique, so a first-order computation at an interior critical point does not settle it. Banach's theorem asserts equality, not equality up to a constant: the standard polarization identity bounds the 4-linear form by its diagonal values only up to a factor. Proposition 6.10 is where the paper's own argument is loose: the 4-linear form it introduces is not symmetric, so (24) does not apply as printed. Finally, the singular-value clauses require that the maximum of a trilinear form on a product of spheres is a stationary value. This must be proved, not assumed.

Formalization scope

Tensors are arrays Fin l → Fin m → Fin n → ℝ with 0-based indices: the paper's aijka_{ijk}aijk​ is A (i-1) (j-1) (k-1). The Euclidean norm is Real.sqrt (∑ i, x i ^ 2). Suprema and maxima are sSup of sets that are nonempty and bounded under the stated hypotheses; where the paper's "max" carries content (Motzkin–Straus, (22), §7), attainment is stated with IsGreatest/IsLeast. The graph is a SimpleGraph (Fin v) with v≥1v\ge1v≥1, clique number Mathlib's SimpleGraph.cliqueNum, and its edges are enumerated by an arbitrary Fin e ≃ G.edgeSet. Every statement holds for each enumeration, so the tensor depends on the choice and the conclusions do not. Al\mathcal A_lAl​ is a rational tensor, read over R\mathbb RR by casting.

Explicit readings of the paper:

  • Definition 6.1 has no norm constraint. Since (σ,u,v,w)↦(tσ,tu,tv,tw)(\sigma,\mathbf u,\mathbf v,\mathbf w)\mapsto(t\sigma,t\mathbf u,t\mathbf v,t\mathbf w)(σ,u,v,w)↦(tσ,tu,tv,tw) preserves (20), unnormalized singular values make every nonzero real a singular value of Al\mathcal A_lAl​, so the clause "not for l>ωl>\omegal>ω" would be false. Singular vectors are therefore unit vectors, as in the paper's derivation on p. 0:21.
  • The statement of Lemma 6.11 prints wm+l+kw_{m+l+k}wm+l+k​. There is no mmm in §6, and the proof uses we+l+kw_{e+l+k}we+l+k​, which is formalized.
  • EkE_kEk​ is written entrywise as 12[{i,j}={ik,jk}]\frac12[\{i,j\}=\{i_k,j_k\}]21​[{i,j}={ik​,jk​}], which equals 12Eikjk+12Ejkik\frac12E_{i_kj_k}+\frac12E_{j_ki_k}21​Eik​jk​​+21​Ejk​ik​​ for a loopless edge.
  • "TlT_lTl​ is just the maximum ℓ2\ell^2ℓ2-singular value of Al\mathcal A_lAl​" is made explicit as milestone 7.
  • The goal does not claim that 111 fails to be a singular value of Al\mathcal A_lAl​ for l<ωl<\omegal<ω; the paper neither claims nor uses this.

This is the mathematical core of a polynomial-time Turing reduction, not an NP-hardness theorem. The polynomial size of Al\mathcal A_lAl​, the vvv-query procedure, the scaling to a general fixed 0≠σ∈Q0\ne\sigma\in\mathbb Q0=σ∈Q, and the NP-completeness of CLIQUE (Karp 1972, cited) are not formalized. Theorem 1.11 and Corollary 1.12 are out of scope.

Two formalizations would make the goal trivial, and both are excluded. One is dropping the unit-norm constraint, which makes every nonzero number a singular value. The other is a spectral norm taken as a supremum over all vectors without normalization, which makes it unbounded and junk-valued; here the quotients are normalized.

Contributions are welcome on each milestone. Motzkin–Straus, Banach (24) and He–Li–Zhang are self-contained and reusable. Lemma 6.11 and milestone 7 need Cauchy–Schwarz and a Lagrange-type stationarity argument on spheres, which Mathlib supports through IsLocalExtrOn and the Lagrange multiplier files.

Selected references

  • C. J. Hillar, L.-H. Lim, Most Tensor Problems Are NP-Hard, J. ACM 60(6), Article 45, 2013. https://doi.org/10.1145/2512329 (final version arXiv:0911.1393v5, https://arxiv.org/abs/0911.1393v5)
  • T. S. Motzkin, E. G. Straus, Maxima for graphs and a new proof of a theorem of Turán, Canadian J. Math. 17, 533–540, 1965. https://doi.org/10.4153/CJM-1965-053-6
  • S. Banach, Über homogene Polynome in (L²), Studia Math. 7, 36–44, 1938. https://doi.org/10.4064/sm-7-1-36-44
  • S. He, Z. Li, S. Zhang, Approximation algorithms for homogeneous polynomial optimization with quadratic constraints, Math. Program. Ser. B 125(2), 353–383, 2010. https://doi.org/10.1007/s10107-010-0409-z
  • R. M. Karp, Reducibility among combinatorial problems, in Complexity of Computer Computations, Plenum, 85–103, 1972. https://doi.org/10.1007/978-1-4684-2001-2_9
11 thms1 active userReviewed
ProbabilityRandom Matrix Theory·Captain: mikedeng1

User-Friendly Tail Bounds for Sums of Random Matrices III: The Matrix Chernoff Inequality for Sums of Independent Positive-Semidefinite Random MatricesResearch Paper

Motivation

The classical Chernoff bound controls the probability that a sum of independent, nonnegative, uniformly bounded random variables deviates from its mean, with exponentially small tails governed by the Kullback–Leibler divergence between two Bernoulli laws. Many problems in numerical linear algebra, graph sparsification, compressed sensing and randomized algorithms instead require control of a sum of independent random matrices: the smallest singular value of a random matrix with independent columns, the spectrum of a sampled Laplacian, or the conditioning of a random submatrix. For these, what matters is not a scalar sum but the extreme eigenvalues of a random positive-semidefinite matrix.

Ahlswede and Winter (2002) introduced a matrix version of the Laplace transform method and proved a matrix Chernoff bound for identically distributed summands. Tropp's paper (arXiv:1004.4389, Found. Comput. Math. 2012) replaced the Golden–Thompson step of their argument with Lieb's concavity theorem, obtaining a master tail bound for independent sums, and derived from it matrix Chernoff, Bernstein and Azuma inequalities that require no identical distribution and lose only a dimensional factor. This mission formalizes the matrix Chernoff inequalities of §5 of that paper.

Timeline:

  • 2002, Ahlswede–Winter: matrix Laplace transform method; matrix Chernoff bound for i.i.d. summands via Golden–Thompson.
  • 2010, Oliveira: a variant of the Laplace transform method used in Proposition 3.1 of the paper.
  • 2010–2012, Tropp: master tail bound via Lieb's theorem (Theorem 3.6), and Theorem 5.1 / Corollary 5.2 for independent, non-identical psd summands.

Setting

All matrices are d×dd\times dd×d complex matrices with d≥1d\ge1d≥1. For a self-adjoint (Hermitian) matrix AAA, λmax⁡(A)\lambda_{\max}(A)λmax​(A) and λmin⁡(A)\lambda_{\min}(A)λmin​(A) are its algebraically largest and smallest eigenvalues. The semidefinite order A≼BA\preccurlyeq BA≼B means that B−AB-AB−A is positive semidefinite (psd). Functions of a self-adjoint matrix are defined spectrally: if A=QΛQ∗A = Q\Lambda Q^*A=QΛQ∗ then f(A)=Qf(Λ)Q∗f(A) = Qf(\Lambda)Q^*f(A)=Qf(Λ)Q∗; this gives the matrix exponential eAe^AeA and, on positive-definite matrices, the matrix logarithm log⁡A\log AlogA.

A random matrix is a measurable map X:Ω→Cd×dX:\Omega\to\mathbb C^{d\times d}X:Ω→Cd×d on a probability space (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P), and its expectation EX\mathbb E XEX is taken entrywise. The matrix moment generating function of XXX is θ↦E eθX\theta\mapsto\mathbb E\,e^{\theta X}θ↦EeθX.

The objects of the mission are independent random Hermitian matrices X1,…,XnX_1,\dots,X_nX1​,…,Xn​ that are almost surely psd contractions: Xk≽0X_k\succcurlyeq0Xk​≽0 and λmax⁡(Xk)≤1\lambda_{\max}(X_k)\le1λmax​(Xk​)≤1. Their average expectation has extreme eigenvalues

μˉmin⁡=λmin⁡(1n∑k=1nEXk),μˉmax⁡=λmax⁡(1n∑k=1nEXk),\bar\mu_{\min} = \lambda_{\min}\Big(\frac1n\sum_{k=1}^n\mathbb E X_k\Big),\qquad \bar\mu_{\max}=\lambda_{\max}\Big(\frac1n\sum_{k=1}^n\mathbb E X_k\Big),μˉ​min​=λmin​(n1​k=1∑n​EXk​),μˉ​max​=λmax​(n1​k=1∑n​EXk​),

and the binary information divergence is

D(a ∥ u)=a(log⁡a−log⁡u)+(1−a)(log⁡(1−a)−log⁡(1−u)),a,u∈[0,1].\mathrm D(a\,\|\,u) = a(\log a-\log u)+(1-a)(\log(1-a)-\log(1-u)),\qquad a,u\in[0,1].D(a∥u)=a(loga−logu)+(1−a)(log(1−a)−log(1−u)),a,u∈[0,1].

In Lean these are lambdaMax, lambdaMin, mexp, mlog, mean and binDiv in the namespace MatrixTail.Chernoff.

Formalization targets

Goal: Theorem 5.1 (Matrix Chernoff I)

P{λmin⁡(1n∑kXk)≤α}≤d e−n D(α∥μˉmin⁡)(0≤α≤μˉmin⁡),\mathbb P\Big\{\lambda_{\min}\Big(\tfrac1n\textstyle\sum_k X_k\Big)\le\alpha\Big\}\le d\,e^{-n\,\mathrm D(\alpha\|\bar\mu_{\min})}\quad(0\le\alpha\le\bar\mu_{\min}),P{λmin​(n1​∑k​Xk​)≤α}≤de−nD(α∥μˉ​min​)(0≤α≤μˉ​min​), P{λmax⁡(1n∑kXk)≥α}≤d e−n D(α∥μˉmax⁡)(μˉmax⁡≤α≤1).\mathbb P\Big\{\lambda_{\max}\Big(\tfrac1n\textstyle\sum_k X_k\Big)\ge\alpha\Big\}\le d\,e^{-n\,\mathrm D(\alpha\|\bar\mu_{\max})}\quad(\bar\mu_{\max}\le\alpha\le1).P{λmax​(n1​∑k​Xk​)≥α}≤de−nD(α∥μˉ​max​)(μˉ​max​≤α≤1).

Milestones

  1. Theorem 3.6 (master tail bound): for every θ>0\theta>0θ>0 at which the mgfs exist, P{λmax⁡(∑kXk)≥t}≤e−θttr⁡exp⁡(∑klog⁡E eθXk)\mathbb P\{\lambda_{\max}(\sum_kX_k)\ge t\}\le e^{-\theta t}\operatorname{tr}\exp(\sum_k\log\mathbb E\,e^{\theta X_k})P{λmax​(∑k​Xk​)≥t}≤e−θttrexp(∑k​logEeθXk​).
  2. Corollary 3.9: the same with the mgfs under one logarithm, d⋅exp⁡(−θt+nlog⁡λmax⁡(1n∑kE eθXk))d\cdot\exp(-\theta t+n\log\lambda_{\max}(\frac1n\sum_k\mathbb E\,e^{\theta X_k}))d⋅exp(−θt+nlogλmax​(n1​∑k​EeθXk​)).
  3. Lemma 5.8 (Chernoff mgf): E eθX≼I+(eθ−1)EX\mathbb E\,e^{\theta X}\preccurlyeq\mathbf I+(e^\theta-1)\mathbb E XEeθX≼I+(eθ−1)EX for a random psd contraction XXX.
  4. Display (5.1): P{λmax⁡(∑kXk)≥t}≤dexp⁡(−θt+nlog⁡(1+(eθ−1)μˉmax⁡))\mathbb P\{\lambda_{\max}(\sum_kX_k)\ge t\}\le d\exp(-\theta t+n\log(1+(e^\theta-1)\bar\mu_{\max}))P{λmax​(∑k​Xk​)≥t}≤dexp(−θt+nlog(1+(eθ−1)μˉ​max​)).
  5. Display (5.2): P{λmin⁡(∑kXk)≤t}≤dexp⁡(θt+nlog⁡(1−(1−e−θ)μˉmin⁡))\mathbb P\{\lambda_{\min}(\sum_kX_k)\le t\}\le d\exp(\theta t+n\log(1-(1-e^{-\theta})\bar\mu_{\min}))P{λmin​(∑k​Xk​)≤t}≤dexp(θt+nlog(1−(1−e−θ)μˉ​min​)).

Further statement

Corollary 5.2 (Matrix Chernoff II), the form usually quoted: with λmax⁡(Xk)≤R\lambda_{\max}(X_k)\le Rλmax​(Xk​)≤R, μmin⁡,μmax⁡\mu_{\min},\mu_{\max}μmin​,μmax​ the extreme eigenvalues of ∑kEXk\sum_k\mathbb E X_k∑k​EXk​,

P{λmin⁡(∑kXk)≤(1−δ)μmin⁡}≤d[e−δ(1−δ)1−δ]μmin⁡/R,P{λmax⁡(∑kXk)≥(1+δ)μmax⁡}≤d[eδ(1+δ)1+δ]μmax⁡/R.\mathbb P\{\lambda_{\min}(\textstyle\sum_kX_k)\le(1-\delta)\mu_{\min}\}\le d\Big[\tfrac{e^{-\delta}}{(1-\delta)^{1-\delta}}\Big]^{\mu_{\min}/R},\quad \mathbb P\{\lambda_{\max}(\textstyle\sum_kX_k)\ge(1+\delta)\mu_{\max}\}\le d\Big[\tfrac{e^{\delta}}{(1+\delta)^{1+\delta}}\Big]^{\mu_{\max}/R}.P{λmin​(∑k​Xk​)≤(1−δ)μmin​}≤d[(1−δ)1−δe−δ​]μmin​/R,P{λmax​(∑k​Xk​)≥(1+δ)μmax​}≤d[(1+δ)1+δeδ​]μmax​/R.

Significance

Theorem 5.1 matches the strongest scalar Chernoff bound for independent, non-identical Bernoulli trials, up to the factor ddd, which cannot be removed (coupon collector, Remark 5.6). Corollary 5.2 is the version used in applications: lower bounds on the smallest singular value of matrices with independent columns (Remark 5.4), spectral sparsification, column subset selection and random sampling of matrices. Remark 5.5 derives from it the expectation bound Eλmax⁡(∑kXk)≤Cmax⁡{μmax⁡,Rlog⁡d}\mathbb E\lambda_{\max}(\sum_kX_k)\le C\max\{\mu_{\max},R\log d\}Eλmax​(∑k​Xk​)≤Cmax{μmax​,Rlogd}.

The results are proved in the paper, from Lieb's concavity theorem. As far as is known, no machine-checked proof of a matrix Chernoff inequality exists in Lean or Mathlib. A formalization yields a reusable statement for the random-matrix and randomized-numerical-linear-algebra literature, and the milestones (the master bound, the single-logarithm corollary and the semidefinite mgf bound) are reusable beyond this mission.

Difficulty

The scalar Chernoff argument uses E eθ(X+Y)=E eθX E eθY\mathbb E\,e^{\theta(X+Y)}=\mathbb E\,e^{\theta X}\,\mathbb E\,e^{\theta Y}Eeθ(X+Y)=EeθXEeθY for independent X,YX,YX,Y. For matrices eA+B≠eAeBe^{A+B}\neq e^Ae^BeA+B=eAeB unless AAA and BBB commute, so the trace of the mgf of a sum does not factor. The Golden–Thompson inequality handles two summands but does not extend to three, which is why the Ahlswede–Winter bound needed identical distributions. The master bound (Theorem 3.6) requires Lieb's concavity theorem, which has no counterpart in Mathlib. Corollary 3.9 in addition needs operator concavity of the matrix logarithm, and Lemma 5.8 needs the transfer of a scalar inequality to the semidefinite order through the spectral calculus.

Formalization scope

Matrices are Matrix (Fin d) (Fin d) ℂ with [NeZero d]; the semidefinite order is Mathlib's MatrixOrder (A ≤ B ↔ (B − A).PosSemidef). exp and log of a matrix are the continuous functional calculus cfc. λmax⁡\lambda_{\max}λmax​, λmin⁡\lambda_{\min}λmin​ are sSup/sInf of the real spectrum. Expectation is entrywise. Random matrices are measurable with respect to the Borel σ-algebra on matrices, independence is iIndepFun, and the probability measure is a probability measure. The summands are Hermitian for every outcome; "psd" and "λmax⁡≤1\lambda_{\max}\le1λmax​≤1" hold almost surely. The sequence has n≥1n\ge1n≥1 terms wherever an average 1/n1/n1/n appears. An infimum over θ>0\theta>0θ>0 is stated as a bound for every admissible θ>0\theta>0θ>0; integrability of eθXke^{\theta X_k}eθXk​ is a hypothesis only in Theorem 3.6 and Corollary 3.9, where the summands are unbounded. In Lean log⁡0=0\log 0=0log0=0, so at the boundary values μˉ∈{0,1}\bar\mu\in\{0,1\}μˉ​∈{0,1} the divergence is finite where the paper's is +∞+\infty+∞; this only weakens the stated bound.

A formalization in which d=0d=0d=0 (empty spectrum, λmax⁡=0\lambda_{\max}=0λmax​=0) or n=0n=0n=0 (the average 1/0=01/0=01/0=0) were allowed, or in which the range of α\alphaα were dropped, would state a different, partly false theorem; these cases are excluded.

A complete development needs Lieb's theorem or another route to the master bound, operator concavity of the logarithm, the spectral mapping theorem and the transfer rule for the functional calculus on Hermitian matrices, monotonicity of the trace exponential, and the scalar optimization in θ\thetaθ. Contributions of any of these as stand-alone lemmas are welcome.

Selected references

  • J. A. Tropp, User-Friendly Tail Bounds for Sums of Random Matrices, arXiv:1004.4389v7 (2011); Found. Comput. Math. 12 (2012) 389–434. https://arxiv.org/abs/1004.4389, https://doi.org/10.1007/s10208-011-9099-z
  • R. Ahlswede, A. Winter, Strong converse for identification via quantum channels, IEEE Trans. Inform. Theory 48 (2002) 569–579. https://doi.org/10.1109/18.985947
  • E. H. Lieb, Convex trace functions and the Wigner–Yanase–Dyson conjecture, Adv. Math. 11 (1973) 267–288. https://doi.org/10.1016/0001-8708(73)90011-X
  • R. I. Oliveira, Sums of random Hermitian matrices and an inequality by Rudelson, Electron. Commun. Probab. 15 (2010) 203–212. https://arxiv.org/abs/1004.3821
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Graph TheoryTheoretical Computer Science·Captain: mikedeng1

Spectral Sparsification of Graphs 3: Sparsifying the Contraction and Pulling It Back Approximates a Graph with Heavy Intra-Part Edges to Within (1+ε)(1+1/c)²Research Paper

Motivation

A spectral sparsifier of a weighted graph GGG is a graph G~\widetilde GG on the same vertices, with few edges, whose Laplacian quadratic form is within a factor σ\sigmaσ of that of GGG on every vector. Spielman and Teng introduced the notion in their work on nearly-linear-time solvers for symmetric diagonally dominant linear systems (Spielman–Teng 2004; arXiv:0808.4134): a sparsifier can replace a dense graph as a preconditioner, and it preserves every cut value up to the same factor, strengthening the cut sparsifiers of Benczúr and Karger (BK96).

Their construction first handles graphs whose edge weights lie in a bounded range. Arbitrary weights need an extra idea, which §10.2 of Spectral Sparsification of Graphs formalizes as Lemma 10.2 (Pullback): when a graph's vertex classes are held together by edges far heavier than those between them, one may contract each class to a single vertex, sparsify the much smaller contracted graph, and pull the result back to the original vertices. The approximation factor degrades only by (1+1/c)2(1+1/c)^2(1+1/c)2, where ccc measures the gap between heavy and light weights. The same contraction idea goes back to Benczúr and Karger's treatment of weighted cut sparsifiers.

Setting

A weighted graph G=(V,E,w)G=(V,E,w)G=(V,E,w) on a finite set VVV, n=∣V∣n=|V|n=∣V∣, is a symmetric function w:V×V→R≥0w:V\times V\to\mathbb R_{\ge 0}w:V×V→R≥0​ with w(v,v)=0w(v,v)=0w(v,v)=0; its edges are the pairs with w(u,v)≠0w(u,v)\ne 0w(u,v)=0. Its Laplacian quadratic form is

xTLGx=∑(u,v)∈Ew(u,v) (x(u)−x(v))2,x∈RV.x^TL_Gx=\sum_{(u,v)\in E}w(u,v)\,(x(u)-x(v))^2,\qquad x\in\mathbb R^V .xTLG​x=(u,v)∈E∑​w(u,v)(x(u)−x(v))2,x∈RV.

A graph G~\widetilde GG is a σ\sigmaσ-approximation of GGG if 1σxTLG~x≤xTLGx≤σ xTLG~x\frac1\sigma x^TL_{\widetilde G}x\le x^TL_Gx\le\sigma\, x^TL_{\widetilde G}xσ1​xTLG​x≤xTLG​x≤σxTLG​x for all xxx. We write G≼G′G\preccurlyeq G'G≼G′ when xTLGx≤xTLG′xx^TL_Gx\le x^TL_{G'}xxTLG​x≤xTLG′​x for all xxx, G+G′G+G'G+G′ for the graph whose weights are the sums, and (u,v)(u,v)(u,v) for the single edge {u,v}\{u,v\}{u,v} of weight 111.

Let V1,…,VkV_1,\dots,V_kV1​,…,Vk​ be a partition of VVV with map π:V→{1,…,k}\pi:V\to\{1,\dots,k\}π:V→{1,…,k}. Write E0=∂(V1,…,Vk)E_0=\partial(V_1,\dots,V_k)E0​=∂(V1​,…,Vk​) for the edges between different parts, E1=E−E0E_1=E-E_0E1​=E−E0​, and G0=(V,E0,w)G_0=(V,E_0,w)G0​=(V,E0​,w), G1=(V,E1,w)G_1=(V,E_1,w)G1​=(V,E1​,w). The contraction of GGG under π\piπ is the graph HHH on {1,…,k}\{1,\dots,k\}{1,…,k} with weight z(i,j)=∑π(u)=i, π(v)=jw(u,v)z(i,j)=\sum_{\pi(u)=i,\,\pi(v)=j}w(u,v)z(i,j)=∑π(u)=i,π(v)=j​w(u,v) for i≠ji\ne ji=j and no self-loops. Given a graph H~\widetilde HH on {1,…,k}\{1,\dots,k\}{1,…,k}, a graph G~\widetilde GG on VVV is a pullback of H~\widetilde HH under π\piπ if every edge of G~\widetilde GG joins different parts, H~\widetilde HH is the contraction of G~\widetilde GG, and for every edge (i,j)(i,j)(i,j) of H~\widetilde HH exactly one edge (u,v)(u,v)(u,v) of G~\widetilde GG has π(u)=i\pi(u)=iπ(u)=i, π(v)=j\pi(v)=jπ(v)=j. A pullback thus has as many edges as H~\widetilde HH.

Formalization targets

Goal: Lemma 10.2 (Pullback), pp. 36–37

Let 0≤ϵ<1/20\le\epsilon<1/20≤ϵ<1/2, c≥3c\ge3c≥3, let H~\widetilde HH be a (1+ϵ)(1+\epsilon)(1+ϵ)-approximation of the contraction of G0G_0G0​ under π\piπ, and let G~0\widetilde G_0G0​ be a pullback of H~\widetilde HH. Assume (1) each ViV_iVi​ is connected by edges in E1E_1E1​, (2) every edge in E1E_1E1​ has weight at least c2n3c^2n^3c2n3, (3) every edge in E0E_0E0​ has weight 111. Then

G~0+G1  is an  α-approximation of G,α=(1+ϵ)(1+1c)2.\widetilde G_0+G_1\ \text{ is an }\ \alpha\text{-approximation of } G,\qquad \alpha=(1+\epsilon)\Big(1+\frac1c\Big)^2 .G0​+G1​  is an  α-approximation of G,α=(1+ϵ)(1+c1​)2.

Milestones (proof of Lemma 10.2, pp. 37–38)

Choose representatives vi∈Viv_i\in V_ivi​∈Vi​; let FFF, F~\widetilde FF be the copies of HHH, H~\widetilde HH on {v1,…,vk}\{v_1,\dots,v_k\}{v1​,…,vk​}, and I=F+G1I=F+G_1I=F+G1​, I~=F~+G1\widetilde I=\widetilde F+G_1I=F+G1​.

  • Lemma 10.3 (path inequality): for a path from uuu to vvv with edge weights w1,…,wk>0w_1,\dots,w_k>0w1​,…,wk​>0, (u,v)≼(1/w1+⋯+1/wk)F(u,v)\preccurlyeq(1/w_1+\dots+1/w_k)F(u,v)≼(1/w1​+⋯+1/wk​)F.
  • (20), (21): for a,ba,ba,b in different parts and fff the unit edge between vπ(a),vπ(b)v_{\pi(a)},v_{\pi(b)}vπ(a)​,vπ(b)​,
(a,b)≼(1+1c)(f+1cn2G1),f≼(1+1c)((a,b)+1cn2G1).(a,b)\preccurlyeq\Big(1+\frac1c\Big)\Big(f+\frac{1}{cn^2}G_1\Big),\qquad f\preccurlyeq\Big(1+\frac1c\Big)\Big((a,b)+\frac{1}{cn^2}G_1\Big).(a,b)≼(1+c1​)(f+cn21​G1​),f≼(1+c1​)((a,b)+cn21​G1​).
  • Summed bound: G0≼(1+1/c) [F+12cG1]G_0\preccurlyeq(1+1/c)\,[F+\tfrac1{2c}G_1]G0​≼(1+1/c)[F+2c1​G1​].
  • Claim (a): III is a (1+1/c)(1+1/c)(1+1/c)-approximation of GGG.
  • Claim (b): I~\widetilde II is a (1+ϵ)(1+\epsilon)(1+ϵ)-approximation of III.
  • Claim (c): I~\widetilde II is a (1+1/c)(1+1/c)(1+1/c)-approximation of G~0+G1\widetilde G_0+G_1G0​+G1​.

The constants are the paper's; the goal is the lemma as printed.

Significance

Lemma 10.2 is the reduction from arbitrary weights to bounded weights in Spielman and Teng's sparsification algorithm (Sparsify, §10.2): the edges of each weight scale are sparsified on a graph in which all much heavier edges have been contracted, so the number of vertices handled at each scale stays small, and the total size of the sparsifier is only a logarithmic factor larger than in the bounded-weight case. The statement itself is purely about quadratic forms and holds for any approximation H~\widetilde HH of the contraction, however it was obtained; it applies equally to later sparsification methods such as sampling by effective resistances.

The lemma is proved in the paper. As far as is known, none of these statements has a machine-checked proof: Mathlib has the Laplacian of a simple graph (SimpleGraph.lapMatrix) but no weighted Laplacian order, no contraction of weighted graphs and no notion of spectral approximation. The mission produces those objects and a complete formal proof of the lemma and its intermediate claims.

Difficulty

The individual steps are elementary, but the proof combines three kinds of bookkeeping. Lemma 10.3 is a Cauchy–Schwarz inequality along a path, which must be applied to a path assembled from two walks inside parts and one edge between representatives; obtaining a simple path of length at most nnn from the connectivity hypothesis requires shortening walks. The summed bounds require recognising that the copies of the unit edges between representatives add up exactly to FFF, which uses hypothesis 3 and the fact that contraction counts each edge between two parts once. Claim (c) needs, in addition, that the total weight of F~\widetilde FF is at most (1+ϵ)(1+\epsilon)(1+ϵ) times that of FFF and that each pullback edge has the weight of its image edge. The constants are tight in one place: (1+1/c)(1+ϵ)≤2(1+1/c)(1+\epsilon)\le 2(1+1/c)(1+ϵ)≤2 requires both c≥3c\ge3c≥3 and ϵ≤1/2\epsilon\le 1/2ϵ≤1/2.

A natural shortcut, comparing G~0\widetilde G_0G0​ with G0G_0G0​ directly, fails: G~0\widetilde G_0G0​ and G0G_0G0​ have different edges, and their Laplacians are only comparable through the heavy intra-part edges.

Formalization scope

A weighted graph is a function w : V → V → ℝ on a Fintype V with IsWGraph w (symmetric, nonnegative, zero diagonal); sums and scalar multiples are pointwise. lapForm w x is 12∑u,vw(u,v)(x(u)−x(v))2\frac12\sum_{u,v}w(u,v)(x(u)-x(v))^221​∑u,v​w(u,v)(x(u)−x(v))2, IsApprox σ w̃ w keeps both inequalities of the definition, and GraphLE is ≼\preccurlyeq≼. The partition is a surjective map π : V → Fin k (nonempty parts). G0G_0G0​, G1G_1G1​ are crossPart w π, intraPart w π; hypothesis 1 is reachability, between any two vertices of the same part, in the simple graph of E1E_1E1​-edges. Representatives are any r : Fin k → V with π (r i) = i, and liftAlong r z places a graph on Fin k on them; the goal does not mention representatives. nnn is Fintype.card V.

Two hypotheses implicit in the paper are explicit: ϵ≥0\epsilon\ge0ϵ≥0 (with ϵ<0\epsilon<0ϵ<0 the lemma is false), and that every edge of a pullback joins two different parts (contraction cannot see an edge inside a part, so without this a pullback could carry an arbitrary heavy edge and the lemma would be false). In Lemma 10.3 the edge weights are positive and the path has at least one edge.

A trivializing formalization is ruled out: dropping hypothesis 2 or 3, allowing ϵ<0\epsilon<0ϵ<0 or intra-part pullback edges, or letting the pullback forget the uniqueness of the edge over each (i,j)(i,j)(i,j) makes the statement false or weaker, and stating only one of the two inequalities of σ\sigmaσ-approximation is a different theorem. Every statement here keeps both.

The algorithm Sparsify and its analysis (Lemma 10.4, Theorem 10.5, Proposition 10.6, Theorem 10.7, Lemmas 10.8–10.9) and all running-time claims are out of scope. The weighted Laplacian form, its additivity and nonnegativity, and the transport of a quadratic form along an injective vertex map are reusable beyond this mission; contributions of such general lemmas, and a proof of Lemma 10.3 by Cauchy–Schwarz, are welcome.

Selected references

  • D. A. Spielman, S.-H. Teng, Spectral Sparsification of Graphs, arXiv:0808.4134v3, 2010; SIAM J. Comput. 40(4), 2011. https://arxiv.org/abs/0808.4134
  • D. A. Spielman, S.-H. Teng, Nearly-Linear Time Algorithms for Graph Partitioning, Graph Sparsification, and Solving Linear Systems, STOC 2004. https://arxiv.org/abs/cs/0310051
  • A. A. Benczúr, D. R. Karger, Approximating s-t Minimum Cuts in Õ(n²) Time, STOC 1996; Randomized Approximation Schemes for Cuts and Flows in Capacitated Graphs, arXiv:cs/0207078. https://arxiv.org/abs/cs/0207078
  • P. Diaconis, D. Stroock, Geometric Bounds for Eigenvalues of Markov Chains, Ann. Appl. Probab. 1(1), 1991. https://doi.org/10.1214/aoap/1177005980
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Convex OptimizationOperations ResearchOptimization·Captain: mikedeng1

On the Rank of Extreme Matrices in Semidefinite Programs and the Multiplicity of Optimal Eigenvalues: If m > k(n − k), Extreme Optima of Affine EV_k Have λ_k = λ_{k+1} with Multiplicity ≥ n − τResearch Paper

Motivation

Minimizing the sum of the kkk largest eigenvalues of a symmetric matrix that depends affinely on parameters is a basic problem of eigenvalue optimization (survey: A. S. Lewis and M. L. Overton, Eigenvalue optimization, Acta Numerica 5, 1996, doi:10.1017/S0962492900002646). Its objective is convex, and fkf_kfk​ is differentiable at BBB exactly when λk(B)>λk+1(B)\lambda_k(B)>\lambda_{k+1}(B)λk​(B)>λk+1​(B); at optimal solutions the eigenvalues tend to coalesce, which makes the problem a model problem of nonsmooth optimization. G. Pataki, On the rank of extreme matrices in semidefinite programs and the multiplicity of optimal eigenvalues (Math. Oper. Res. 23(2), 1998, doi:10.1287/moor.23.2.339), gives a quantitative explanation in terms of the number of free parameters.

The paper also proves a bound on the rank of extreme points of semidefinite programs, now often called the Pataki bound (also obtained by Barvinok, 1995): an extreme point XXX of {X⪰0:Ai∙X=bi, i≤m}\{X\succeq0: A_i\bullet X=b_i,\ i\le m\}{X⪰0:Ai​∙X=bi​, i≤m} satisfies rank⁡X(rank⁡X+1)/2≤m\operatorname{rank}X(\operatorname{rank}X+1)/2\le mrankX(rankX+1)/2≤m. This bound is used throughout low-rank semidefinite optimization, for instance in the Burer–Monteiro approach.

Setting

Sn\mathcal S^nSn is the space of real symmetric n×nn\times nn×n matrices, X⪰0X\succeq0X⪰0 means XXX is symmetric positive semidefinite, and A∙B=∑i,jaijbijA\bullet B=\sum_{i,j}a_{ij}b_{ij}A∙B=∑i,j​aij​bij​. For B∈SnB\in\mathcal S^nB∈Sn, λ1(B)≥⋯≥λn(B)\lambda_1(B)\ge\dots\ge\lambda_n(B)λ1​(B)≥⋯≥λn​(B) are its eigenvalues and, for k∈{1,…,n}k\in\{1,\dots,n\}k∈{1,…,n},

fk(B)=λ1(B)+⋯+λk(B).f_k(B)=\lambda_1(B)+\dots+\lambda_k(B).fk​(B)=λ1​(B)+⋯+λk​(B).

The multiplicity mult⁡(λi(B))\operatorname{mult}(\lambda_i(B))mult(λi​(B)) is the largest p≥1p\ge1p≥1 with λj(B)=⋯=λj+p−1(B)\lambda_j(B)=\dots=\lambda_{j+p-1}(B)λj​(B)=⋯=λj+p−1​(B) for some j≤i≤j+p−1j\le i\le j+p-1j≤i≤j+p−1.

A face of a convex set SSS is a convex F⊆SF\subseteq SF⊆S such that x∈Fx\in Fx∈F, y,z∈Sy,z\in Sy,z∈S, x=12(y+z)x=\tfrac12(y+z)x=21​(y+z) imply y,z∈Fy,z\in Fy,z∈F; an extreme point is a one-point face; dim⁡S\dim SdimS is the maximal number of affinely independent points of SSS, minus one. Write t(i)=i(i+1)/2t(i)=i(i+1)/2t(i)=i(i+1)/2 and

τ(l,r,s)=max⁡{ i+j: t(i)+t(j)≤l, i≤r, j≤s }.\tau(l,r,s)=\max\{\,i+j:\ t(i)+t(j)\le l,\ i\le r,\ j\le s\,\}.τ(l,r,s)=max{i+j: t(i)+t(j)≤l, i≤r, j≤s}.

Let A0,A1,…,Am∈SnA_0,A_1,\dots,A_m\in\mathcal S^nA0​,A1​,…,Am​∈Sn be linearly independent, A(x)=A0+∑i=1mxiAiA(x)=A_0+\sum_{i=1}^mx_iA_iA(x)=A0​+∑i=1m​xi​Ai​, and assume m≥1m\ge1m≥1 and k<nk<nk<n (the standing assumptions of §4). The affine eigenvalue problem is

(EVk)min⁡{fk(A(x)): x∈Rm},(EV_k)\qquad\min\{f_k(A(x)):\ x\in\mathbb R^m\},(EVk​)min{fk​(A(x)): x∈Rm},

and Θ\ThetaΘ denotes its set of optimal solutions, a closed convex set. For B∈SnB\in\mathcal S^nB∈Sn the semidefinite program

min⁡ kz+I∙Vs.t.V,W⪰0,zI+V−W=B(3.14)\min\ kz+I\bullet V\quad\text{s.t.}\quad V,W\succeq0,\quad zI+V-W=B \tag{3.14}min kz+I∙Vs.t.V,W⪰0,zI+V−W=B(3.14)

has optimal value fk(B)f_k(B)fk​(B); Ωk(B)\Omega_k(B)Ωk​(B) is its set of optimal solutions (z,V,W)(z,V,W)(z,V,W).

Formalization targets

Goal: Theorem 4.3

If x∗x^*x∗ is an extreme point of Θ\ThetaΘ and m>k(n−k)m>k(n-k)m>k(n−k), then

λk(A(x∗))=λk+1(A(x∗))andmult⁡(λk(A(x∗))) ≥ n−τ(t(n)−m−1, k−1, n−k−1).\lambda_k(A(x^*))=\lambda_{k+1}(A(x^*))\qquad\text{and}\qquad \operatorname{mult}(\lambda_k(A(x^*)))\ \ge\ n-\tau\big(t(n)-m-1,\,k-1,\,n-k-1\big).λk​(A(x∗))=λk+1​(A(x∗))andmult(λk​(A(x∗))) ≥ n−τ(t(n)−m−1,k−1,n−k−1).

Milestones

  1. Theorem 2.1: on a face FFF of the primal feasible set, t(rank⁡X)≤m+dim⁡Ft(\operatorname{rank}X)\le m+\dim Ft(rankX)≤m+dimF; on a face GGG of the dual feasible set, t(rank⁡Z)≤t(n)−m+dim⁡Gt(\operatorname{rank}Z)\le t(n)-m+\dim Gt(rankZ)≤t(n)−m+dimG.
  2. Theorem 2.2: the multi-block version ∑jt(rank⁡Xj)≤m−q+dim⁡G\sum_jt(\operatorname{rank}X_j)\le m-q+\dim G∑j​t(rankXj​)≤m−q+dimG for programs with ppp semidefinite blocks and qqq free variables.
  3. Lemmas 3.1, 3.2 and Theorem 3.3: the optimal value of (3.14) and an explicit description of Ωk(B)\Omega_k(B)Ωk​(B) through an eigendecomposition B=QDiag⁡(λ)QTB=Q\operatorname{Diag}(\lambda)Q^TB=QDiag(λ)QT.
  4. The rank identity of §3: rank⁡V+rank⁡W+mult⁡(λk(B))=n\operatorname{rank}V+\operatorname{rank}W+\operatorname{mult}(\lambda_k(B))=nrankV+rankW+mult(λk​(B))=n on Ωk(B)\Omega_k(B)Ωk​(B) when λk(B)=λk+1(B)\lambda_k(B)=\lambda_{k+1}(B)λk​(B)=λk+1​(B).
  5. Lemma 4.2 and (4.31): {x∗}×Ωk(A(x∗))\{x^*\}\times\Omega_k(A(x^*)){x∗}×Ωk​(A(x∗)) is a face of the feasible set of the lifted SDP (4.26), of dimension 111 or 000 according as λk>λk+1\lambda_k>\lambda_{k+1}λk​>λk+1​ or λk=λk+1\lambda_k=\lambda_{k+1}λk​=λk+1​.
  6. Lemma 4.1: Θ\ThetaΘ contains no line, so it has extreme points whenever it is nonempty.

Significance

The theorem says that once the number of free parameters mmm exceeds k(n−k)k(n-k)k(n−k), the kkk-th and (k+1)(k+1)(k+1)-st eigenvalues necessarily coincide at extreme optimal solutions, so fk∘Af_k\circ Afk​∘A is typically nonsmooth at its minimizers, and it bounds from below the dimension of the subdifferential ∂fk(A(x∗))\partial f_k(A(x^*))∂fk​(A(x∗)), which is t(mult⁡(λk))t(\operatorname{mult}(\lambda_k))t(mult(λk​)). The intermediate rank bounds of §2 are reusable on their own for any semidefinite program.

The results are proved in the paper. As far as is known, none of them (neither the Pataki rank bound, nor the semidefinite characterization of fkf_kfk​, nor Theorem 4.3) has a machine-checked proof. Formalizing them produces a library of faces and dimensions of spectrahedra, the SDP representation of the Ky Fan sum fkf_kfk​, and the multiplicity bound itself.

Difficulty

Extremality of x∗x^*x∗ in Θ\ThetaΘ is a statement in the parameter space Rm\mathbb R^mRm and gives no direct information on the spectrum of A(x∗)A(x^*)A(x∗): perturbation arguments on the eigenvalues alone break down precisely at the coalesced eigenvalues the theorem is about, where fkf_kfk​ is not differentiable. The quantitative bound (4.30) also needs more than the optimal value fk(A(x∗))f_k(A(x^*))fk​(A(x∗)): it depends on the whole optimal set Ωk(A(x∗))\Omega_k(A(x^*))Ωk​(A(x∗)), on the dimension of faces of spectrahedra, and on an exact count relating the ranks of the optimal V,WV,WV,W to the multiplicity of λk\lambda_kλk​. None of these (faces and dimension of spectrahedra, the semidefinite representation of fkf_kfk​, eigenvalue run lengths) is in Mathlib.

Formalization scope

Matrices are Matrix (Fin n) (Fin n) ℝ; A∙BA\bullet BA∙B is the published BurerMonteiro.RankIncrease.frob, the primal and dual feasible sets are the published IsPrimalFeasible/IsDualFeasible, and λi(B)\lambda_i(B)λi​(B) is the published ProjLikeRetr.Spectral.eig B ⟨i-1,_⟩ (Mathlib's nonincreasing eigenvalues, 0-based). Every matrix whose eigenvalues are taken is assumed symmetric. Faces, extreme points and dimension are defined as on p. 341; dimension is integer valued with dim⁡∅=−1\dim\emptyset=-1dim∅=−1. All rank bounds are compared in Z\mathbb ZZ. Θ\ThetaΘ is the argmin set {x:fk(A(x))≤fk(A(y)) ∀y}\{x: f_k(A(x))\le f_k(A(y))\ \forall y\}{x:fk​(A(x))≤fk​(A(y)) ∀y} and Ωk(B)\Omega_k(B)Ωk​(B) is the set of feasible points no worse than every feasible point; no infimum is used. Optimal values are stated as least elements of the set of feasible objective values.

Hypotheses added relative to the page, each disclosed in its item: 1≤k<n1\le k<n1≤k<n in the statements of §3, which mention λk+1\lambda_{k+1}λk+1​; k≥1k\ge1k≥1 (p. 340) in every §4 statement; one common matrix order in Theorem 2.2; and λk(B)=λk+1(B)\lambda_k(B)=\lambda_{k+1}(B)λk​(B)=λk+1​(B) in the rank identity of p. 348, which is false as printed when λk(B)>λk+1(B)\lambda_k(B)>\lambda_{k+1}(B)λk​(B)>λk+1​(B) (n=2n=2n=2, k=1k=1k=1, B=diag⁡(2,0)B=\operatorname{diag}(2,0)B=diag(2,0) gives 3≠23\ne23=2) and is used in the paper only in the equal case. The linear independence of A0,…,AmA_0,\dots,A_mA0​,…,Am​ is kept with A0A_0A0​ included, as on p. 348.

Trivializing formalizations are ruled out: Θ\ThetaΘ is not defined through a possibly junk infimum, a face must be convex and contained in the set, the dimension is not a junk 000, mult⁡\operatorname{mult}mult is the run length of equal eigenvalues and not a constant or an index, and the eigenvalues are only ever taken of symmetric matrices.

A complete development needs: the rank–dimension bound for faces of spectrahedra (reusable for any SDP), the semidefinite characterization of fkf_kfk​ with its optimal set, and convexity facts on Θ\ThetaΘ. Proofs of any milestone, alternative proofs of the rank bounds, and the general smooth case of §5 are welcome.

Selected references

  • G. Pataki, On the rank of extreme matrices in semidefinite programs and the multiplicity of optimal eigenvalues, Mathematics of Operations Research 23(2), 339–358, 1998. https://doi.org/10.1287/moor.23.2.339
  • A. I. Barvinok, Problems of distance geometry and convex properties of quadratic maps, Discrete & Computational Geometry 13, 189–202, 1995. https://doi.org/10.1007/BF02574037
  • M. L. Overton and R. S. Womersley, Optimality conditions and duality theory for minimizing sums of the largest eigenvalues of symmetric matrices, Mathematical Programming 62, 321–357, 1993. https://doi.org/10.1007/BF01585173
  • F. Alizadeh, Interior point methods in semidefinite programming with applications to combinatorial optimization, SIAM Journal on Optimization 5(1), 13–51, 1995. https://doi.org/10.1137/0805002
  • A. S. Lewis and M. L. Overton, Eigenvalue optimization, Acta Numerica 5, 149–190, 1996. https://doi.org/10.1017/S0962492900002646
  • R. T. Rockafellar, Convex Analysis, Princeton University Press, 1970.
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Theoretical Computer Science·Captain: marwahaha

Complex Matrix Multiplication Below 2.258 and Rectangular BoundsOpen Problem

Motivation

Rectangular matrix products arise when the two outer dimensions are much larger than the inner dimension. The dual exponent records the largest inner growth rate compatible with arithmetic exponent two. The source manuscript presents the surrounding research claim.

Setting

For k∈[0,1], ω_ℂ(1,k,1) is the infimum of exponents for multiplying an n×⌈nᵏ⌉ matrix by a ⌈nᵏ⌉×n matrix over ℂ. The dual exponent α is the supremum of k for which this infimum equals two.

Formalization target

Prove the strict bound

αC>93200=0.465.\alpha_{\mathbb C}>\frac{93}{200}=0.465.αC​>20093​=0.465.

The additional published rectangular endpoint asserts ω_ℂ(1,709/1000,1)<523/250=2.092.

The selected formal target is OAI.MatrixMultiplication.complex_alpha_gt_93_div_200.

Significance and status

Strictness is part of both statements. The supplied goal concerns the complex dual exponent; the manuscript title’s square bound and broader field claims are not attached formal targets. The published target is currently Open; the manuscript's argument and a checked Lean proof are separate deliverables.

Difficulty

An algorithm for one size does not establish an asymptotic exponent. The definition quantifies over every positive slack and all positive sizes with one bound constant for each slack.

Formalization scope

Algorithms are division-free arithmetic programs with constants and input gates of cost zero and addition, subtraction and multiplication of cost one. Correctness is quantified over all input matrices. The dual exponent is a real supremum of exact exponent-two shapes, using the prescribed inner-dimension ceiling.

Selected references

  • OpenAI, Complex Matrix Multiplication Below 2.258 and Rectangular Bounds, preprint, 2026. Pinned manuscript.
  • OpenAI, accompanying formal statements, commit adc7f1241b42. Goal source.
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Complexity TheoryTheoretical Computer Science·Captain: wurtle

Finite tensor savings and exact Fourier circuitsResearch Paper

Motivation

The discrete Fourier transform of length nnn is computed by the fast Fourier transform with O(nlog⁡n)O(n\log n)O(nlogn) arithmetic operations, and this has been the benchmark since Cooley and Tukey (1965). Whether Ω(nlog⁡n)\Omega(n\log n)Ω(nlogn) operations are necessary is one of the basic open questions of algebraic complexity theory. Lower bounds of order nlog⁡nn\log nnlogn are known only under restrictions on the algorithm: bounded coefficients, unitary 2×22\times22×2 gates on exactly nnn registers, or bounded conditioning of intermediate maps. In the unrestricted model of linear circuits, where coefficients are arbitrary complex numbers and only arithmetic operations are counted, the question remained open. This mission concerns that unrestricted question.

Timeline

  • 1958. Good gives the multidimensional (coprime-factor) form of the Fourier transform (doi:10.1111/j.2517-6161.1958.tb00300.x).
  • 1965. Cooley and Tukey publish the fast Fourier transform (doi:10.1090/S0025-5718-1965-0178586-1).
  • 1969–1970. Rabiner, Schafer and Rader (chirp zzz-transform) and Bluestein reduce arbitrary lengths to convolution (doi:10.1109/TAU.1969.1162034, doi:10.1109/TAU.1970.1162132).
  • 1973. Morgenstern proves an Ω(nlog⁡n)\Omega(n\log n)Ω(nlogn) lower bound for linear circuits with bounded coefficients (doi:10.1145/321752.321761).
  • 2013–2014. Ailon proves lower bounds for 2×22\times22×2 unitary gate models and for well-conditioned computations (arXiv:1305.4745, arXiv:1403.1307).
  • 2023. Alman and Rao improve the leading constants for power-of-two transforms via matrix non-rigidity (doi:10.1145/3564246.3585188).
  • 2025. Alman and Li characterize asymptotic sizes of depth-two circuits for Kronecker powers (arXiv:2509.14489).

The source of this mission, an OpenAI preprint dated September 25, 2026, claims that the Ω(nlog⁡n)\Omega(n\log n)Ω(nlogn) lower bound fails in the unrestricted complex linear-circuit model.

Setting

For n≥2n\ge2n≥2 let ζn=e2πi/n\zeta_n=e^{2\pi i/n}ζn​=e2πi/n and Fn=(ζnjk)0≤j,k<nF_n=(\zeta_n^{jk})_{0\le j,k<n}Fn​=(ζnjk​)0≤j,k<n​. A linear circuit of length nnn has inputs x0,…,xn−1x_0,\dots,x_{n-1}x0​,…,xn−1​ and the constant 000, followed by a finite sequence of gates. Each gate computes u+vu+vu+v, u−vu-vu−v or λu\lambda uλu from previously available values u,vu,vu,v, where λ∈C\lambda\in\mathbb Cλ∈C is a fixed coefficient; each gate costs one. Values may be reused arbitrarily, and the nnn outputs are designated available values. The circuit computes FnF_nFn​ if its outputs equal FnxF_nxFn​x for every x∈Cnx\in\mathbb C^nx∈Cn. Coefficients may depend on nnn and have no bound on size or description; depth, storage and conditioning are unrestricted. Let L(n)L(n)L(n) be the minimum number of gates.

Formalization targets

Goal: Theorem 1.1

lim inf⁡n→∞L(n)nlog⁡2n=0,\liminf_{n\to\infty}\frac{L(n)}{n\log_2 n}=0,n→∞liminf​nlog2​nL(n)​=0,

equivalently: for every c>0c>0c>0 and every N0≥2N_0\ge2N0​≥2 there are n≥N0n\ge N_0n≥N0​ and an exact circuit for FnF_nFn​ with fewer than c nlog⁡2nc\,n\log_2 ncnlog2​n gates. The Lean statement OAI.ExactFourier.main_theorem is this second form and is open on the platform.

The statement does not assert an upper bound for every length, a uniform construction, or anything about numerical stability. A companion OpenAI preprint gives a quantitative all-length bound in a model that also charges coefficient preparation; that result is not part of this mission.

Significance

The theorem refutes the assertion that L(n)≥c nlog⁡2nL(n)\ge c\,n\log_2nL(n)≥cnlog2​n for some fixed c>0c>0c>0 and all large nnn in the unrestricted linear model. It shows that the known lower bounds necessarily depend on their restrictions (bounded coefficients, conditioning, unitary gates). The mechanism, a single finite tensor saving amplified through tensor powers, is a general tool: one strict improvement over the standard axis-by-axis algorithm for one tensor power of one nonmonomial matrix yields an exponent improvement for all tensor powers.

The result is claimed in an OpenAI preprint; it has not been peer reviewed and no machine-checked proof exists. The existence part of the argument is non-constructive (it proceeds by contradiction through price functions and compactness), so a formal proof is a meaningful check.

Difficulty

Leading-constant improvements of the FFT do not change the nlog⁡nn\log nnlogn scale, and every classical structural algorithm (Cooley–Tukey, Good–Thomas, chirp) has that scale. A gain in the exponent of the logarithm needs a saving that compounds across many tensor factors; but a saving for one tensor power of a small matrix does not obviously transfer to Fourier matrices of growing length, because Fourier factorizations introduce diagonal twiddle factors and change the coordinate set. In addition, the existence of a single finite saving is itself not exhibited explicitly and must be proved.

Formalization scope

  • Gate w is add i j, sub i j or scale c i with c : ℂ, referencing the www values available so far.
  • Program n k is a list of kkk gates in topological order; values 0,…,n−10,\dots,n-10,…,n−1 are the inputs and value nnn is the constant 000 (via Fin.snoc x 0).
  • Circuit n has size, a program of that size, and outputs : Fin n → Fin (n+1+size); output selection is free.
  • fourierMatrix n j k = zeta n ^ (j*k) with zeta n = exp(2πi/n); Computes is equality with mulVec for every input.
  • MainStatement: for every real c>0c>0c>0 and N0≥2N_0\ge2N0​≥2 there are n≥N0n\ge N_0n≥N0​ and a computing circuit with size < c * n * logb 2 n.

A complete development needs tensor products of matrices and circuits, the Chinese Remainder (Good–Thomas) identification of FrsF_{rs}Frs​ with Fr⊗FsF_r\otimes F_sFr​⊗Fs​ for coprime r,sr,sr,s, a Toeplitz/Vandermonde factorization of FrF_rFr​ on its own coordinates, and the price-function existence argument (separation, compactness, feedback). Contributions formalizing Lemma 2.3 (tensor amplification) and Proposition 3.4 (transfer of a finite win to Fourier circuits) are natural first steps.

Selected references

  • OpenAI, Finite tensor savings and exact Fourier circuits, preprint, September 25, 2026. https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/Finite-tensor-savings-and-exact-Fourier-circuits-September-25-2026/main.pdf
  • J. W. Cooley, J. W. Tukey, An algorithm for the machine calculation of complex Fourier series, Math. Comp., 1965. https://doi.org/10.1090/S0025-5718-1965-0178586-1
  • J. Morgenstern, Note on a lower bound on the linear complexity of the fast Fourier transform, J. ACM, 1973. https://doi.org/10.1145/321752.321761
  • N. Ailon, A lower bound for Fourier transform computation in a linear model over 2×2 unitary gates, preprint, 2013. https://arxiv.org/abs/1305.4745
  • N. Ailon, An Ω((nlog⁡n)/R)\Omega((n\log n)/R)Ω((nlogn)/R) lower bound for Fourier transform computation in the RRR-well conditioned model, preprint, 2014. https://arxiv.org/abs/1403.1307
  • J. Alman, K. Rao, Faster Walsh–Hadamard and discrete Fourier transforms from matrix non-rigidity, STOC 2023. https://doi.org/10.1145/3564246.3585188
  • I. J. Good, The interaction algorithm and practical Fourier analysis, J. R. Stat. Soc. B, 1958. https://doi.org/10.1111/j.2517-6161.1958.tb00300.x
  • J. Alman, B. Li, Kronecker powers, orthogonal vectors, and the asymptotic spectrum, preprint, 2025. https://arxiv.org/abs/2509.14489
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Complexity TheoryTheoretical Computer Science·Captain: wurtle

Staggered extraction for exact matrix multiplication over every fieldResearch Paper

Motivation: the matrix-multiplication exponent

Multiplying two n×nn\times nn×n matrices by the schoolbook method costs about n3n^3n3 operations. The matrix-multiplication exponent ωF\omega_FωF​ of a field FFF is the infimum of exponents τ\tauτ such that n×nn\times nn×n matrices over FFF can be multiplied with O(nτ+o(1))O(n^{\tau+o(1)})O(nτ+o(1)) additions, subtractions and multiplications. It governs the asymptotic cost of a central bilinear operation and of the many algorithms built from it (determinants, inversion, linear systems). Bounding ω\omegaω has driven algebraic complexity theory since 1969. In recent years the bounds have moved in the third and fourth decimal place, with each improvement coming from a finer analysis of the same tensor-power framework.

Background

  • 1969 — Strassen's seven-product algorithm gives ω≤log⁡27\omega\le\log_27ω≤log2​7 (Strassen 1969).
  • 1980–1987 — Approximate bilinear algorithms (Bini 1980), the asymptotic sum inequality (Schönhage 1981) and the laser method (Strassen 1987).
  • 1990 — Coppersmith and Winograd introduce the tensor family CWq\mathrm{CW}_qCWq​ and progression-free extraction (J. Symbolic Comput. 1990).
  • 2010–2014 — Higher tensor powers: Stothers (fourth power; with Davie, Proc. Roy. Soc. Edinburgh 2013), Vassilevska Williams (eighth power, STOC 2012), Le Gall (thirty-second power, ISSAC 2014).
  • 2023–2024 — The refined laser method gives ω<2.3728596\omega<2.3728596ω<2.3728596 (Alman–Vassilevska Williams, TheoretiCS 2024). Asymmetric hashing reduces combination loss (Duan–Wu–Zhou). Finer variable sharing follows (Vassilevska Williams–Xu–Xu–Zhou).
  • 2024–2026 — Successive asymmetric compatibility tests (Alman–Duan–Vassilevska Williams–Xu–Xu–Zhou, arXiv:2404.16349). Dupont et al. optimize the eighth-power instance of this framework to ω<2.371177\omega<2.371177ω<2.371177 (arXiv:2608.16884).
  • 2026 — An OpenAI preprint, Staggered extraction for exact matrix multiplication over every field (OpenAI Math Release, September 24, 2026), claims ωF<2.371054886006746\omega_F<2.371054886006746ωF​<2.371054886006746 for every fixed field FFF, including every positive characteristic. It has not been peer reviewed, and the claim has not been formally verified.

Setting

Fix a field FFF. An arithmetic program is a straight-line sequence of gates, each a constant from FFF, an input entry, or the sum, difference or product of two earlier gates. Its cost counts the addition, subtraction and multiplication gates. A program multiplies n×nn\times nn×n matrices if designated registers equal the entries of ABABAB for every pair of input matrices A,BA,BA,B over FFF. A real number τ\tauτ is admissible if for every ε>0\varepsilon>0ε>0 there is C>0C>0C>0 such that for every n≥1n\ge1n≥1 some correct program has cost at most C nτ+εC\,n^{\tau+\varepsilon}Cnτ+ε, and

ωF=inf⁡{τ∈R: τ admissible over F}.\omega_F=\inf\{\tau\in\mathbb R:\ \tau\text{ admissible over }F\}.ωF​=inf{τ∈R: τ admissible over F}.

In Lean this is MatrixAllFields.MatrixMultiplication.Arithmetic.omega F, defined for every F : Type u with [Field F].

Formalization targets

Goal: the exponent bound over every field (Theorem 1.1)

∀ F field:ωF<2.371054886006746.\forall\,F\ \text{field}:\qquad \omega_F<2.371054886006746 .∀F field:ωF​<2.371054886006746.

The Lean statement also contains the numerical comparison 2.371054886006746<2.3710562.371054886006746<2.3710562.371054886006746<2.371056, which carries no mathematical content (the source writes the comparison as <2.371054887<2.371054887<2.371054887). This is Theorem 1.1 of the source. The goal is published on the platform with status Open: no machine-checked proof exists yet.

Significance

The result itself. If the source's argument and certificate are correct, the theorem lowers the best stated bound on ω\omegaω from 2.3711772.3711772.371177 (Dupont et al.) to 2.3710552.3710552.371055, and it does so uniformly over all fields, with exact algorithms in every positive characteristic. Any improvement in ω\omegaω lowers the exponent of every algorithm reducible to matrix multiplication. The method — pooling directional capacities across extraction depths and staggering lots so that one lot sits at each splitting stage — shows that combination losses in the asymmetric framework can be traded across depths.

Formalizing it. Bounds of this type rest on long chains of tensor-power constructions, recovery arguments and large rational parameter tables, checked in the source by an accompanying verifier with interval certificates for logarithms. A machine-checked proof would certify the whole chain from the arithmetic model to the final rational inequality. It would also give Mathlib the asymptotic sum inequality and Coppersmith–Winograd machinery, which every future bound on ω\omegaω needs.

Difficulty

Every recent improvement fights extraction losses. Restricting a tensor power to a direct sum of independent matrix products wastes variables whenever whole blocks must be disjoint, while the final products only need disjoint subsets. Prescribed marginals may also allow several joint distributions. Earlier analyses take the minimum of three directional capacities separately at each depth, so a shortage on one side at one depth is lost. Using capacity across depths requires that variables deleted in earlier extractions (to resolve conflicts or impose type conditions) can still be recovered exactly, over the original field and with only subexponentially many extra copies. Positive characteristic rules out arguments that divide by small integers or rely on characteristic-zero identities.

Formalization scope

  • The model is division-free straight-line programs over an arbitrary field F : Type u, with free constants from FFF and unit cost for add, sub and mul. This matches the source's "scalar additions and multiplications".
  • AdmissibleExponent F τ asks, for each ε>0\varepsilon>0ε>0, for one constant C>0C>0C>0 that works for every n≥1n\ge1n≥1. omega F is the sInf of the admissible set, which is nonempty (schoolbook algorithm) and bounded below by the output size, so a junk value cannot make the strict inequality true.
  • The goal quantifies over every field, including finite fields, so a proof cannot use characteristic-zero arguments or embeddings into C\mathbb CC.
  • The second conjunct is a trivially true rational comparison and can be ignored.
  • Infrastructure needed: tensor rank and border rank over arbitrary fields, the asymptotic sum inequality, the Coppersmith–Winograd tensor and its powers, method-of-types counting, and verified rational/logarithm interval arithmetic for the parameter certificate. All of this is reusable for other matrix-multiplication results.

Selected references

  • V. Strassen, Gaussian elimination is not optimal, Numer. Math. 13 (1969), 354–356. https://doi.org/10.1007/BF02165411
  • D. Bini, Relations between exact and approximate bilinear algorithms. Applications, Calcolo 17 (1980), 87–97. https://doi.org/10.1007/BF02575865
  • A. Schönhage, Partial and total matrix multiplication, SIAM J. Comput. 10 (1981), 434–455. https://doi.org/10.1137/0210032
  • V. Strassen, Relative bilinear complexity and matrix multiplication, J. reine angew. Math. 375/376 (1987), 406–443. https://doi.org/10.1515/crll.1987.375-376.406
  • D. Coppersmith and S. Winograd, Matrix multiplication via arithmetic progressions, J. Symbolic Comput. 9 (1990), 251–280. https://doi.org/10.1016/S0747-7171(08)80013-2
  • A. M. Davie and A. J. Stothers, Improved bound for complexity of matrix multiplication, Proc. Roy. Soc. Edinburgh Sect. A 143 (2013), 351–369. https://doi.org/10.1017/S0308210511001648
  • V. Vassilevska Williams, Multiplying matrices faster than Coppersmith–Winograd, STOC 2012, 887–898. https://doi.org/10.1145/2213977.2214056
  • F. Le Gall, Powers of tensors and fast matrix multiplication, ISSAC 2014, 296–303. https://arxiv.org/abs/1401.7714v1
  • J. Alman and V. Vassilevska Williams, A refined laser method and faster matrix multiplication, TheoretiCS 3 (2024), Art. 21. https://doi.org/10.46298/theoretics.24.21
  • R. Duan, H. Wu and R. Zhou, Faster matrix multiplication via asymmetric hashing, arXiv:2210.10173. https://arxiv.org/abs/2210.10173v5
  • V. Vassilevska Williams, Y. Xu, Z. Xu and R. Zhou, New bounds for matrix multiplication: from alpha to omega, arXiv:2307.07970. https://arxiv.org/abs/2307.07970v2
  • J. Alman, R. Duan, V. Vassilevska Williams, Y. Xu, Z. Xu and R. Zhou, More asymmetry yields faster matrix multiplication, arXiv:2404.16349v3. https://arxiv.org/abs/2404.16349v3
  • E. Dupont et al., Improving the matrix multiplication exponent with modern optimization, arXiv:2608.16884 (2026). https://doi.org/10.48550/arXiv.2608.16884
  • OpenAI, Staggered extraction for exact matrix multiplication over every field, OpenAI Math Release preprint, September 24, 2026 (Theorem 1.1, p. 2). https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/Staggered-extraction-for-exact-matrix-multiplication-over-every-field-September-24-2026/Staggered-extraction-for-exact-matrix-multiplication-over-every-field-September-24-2026.pdf
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Convex OptimizationNumerical Analysis·Captain: mikedeng1

Low-rank Matrix Recovery via Iteratively Reweighted Least Squares Minimization 1: IRLS-M Converges to the Nuclear-Norm Minimizer Under the Strong Rank Null Space PropertyResearch Paper

Motivation

Many data problems ask for a matrix of low rank from far fewer linear measurements than it has entries: matrix completion (recommender systems, where a few ratings of a large user–item table are observed), system identification, and quantum state tomography. Minimizing the rank under the measurement constraints is NP-hard in general. The standard convex surrogate replaces the rank by the nuclear norm, the sum of the singular values, and recovers the low-rank matrix exactly when the measurement map is well conditioned on low-rank matrices (Recht, Fazel, Parrilo 2010; Candès, Recht 2009).

Solving the nuclear norm problem at scale is itself a numerical challenge: interior point methods do not scale, and first-order methods such as singular value thresholding (Cai, Candès, Shen 2010) need many iterations. Fornasier, Rauhut and Ward proposed an alternative, iteratively reweighted least squares for matrices (IRLS-M), which replaces the nonsmooth problem by a sequence of weighted least squares problems whose weights are recomputed from the current iterate. It is the matrix analogue of the IRLS method for sparse vectors of Daubechies, DeVore, Fornasier, Güntürk 2010, and a closely related algorithm was studied at the same time by Mohan and Fazel (Allerton 2010; journal version JMLR 2012).

Timeline. 2008–2010: nuclear norm recovery under rank restricted isometry (Recht–Fazel–Parrilo) and the rank null space property (Recht–Xu–Hassibi). 2010: convergence of IRLS for ℓ1\ell_1ℓ1​ under the vector null space property (Daubechies et al.). 2010–2011: IRLS-M and its convergence under the strong rank null space property (this paper, arXiv:1010.2471, SIAM J. Optim. 21(4), 2011).

Setting

Throughout, XXX is a real n×pn\times pn×p matrix with n≤pn\le pn≤p, with singular values σ1(X)≥⋯≥σn(X)≥0\sigma_1(X)\ge\dots\ge\sigma_n(X)\ge0σ1​(X)≥⋯≥σn​(X)≥0. The Frobenius norm is ∥X∥F\|X\|_F∥X∥F​, the nuclear norm is ∥X∥∗=∑iσi(X)\|X\|_*=\sum_i\sigma_i(X)∥X∥∗​=∑i​σi​(X), and ⟨X,Y⟩=∑i,jXijYij\langle X,Y\rangle=\sum_{i,j}X_{ij}Y_{ij}⟨X,Y⟩=∑i,j​Xij​Yij​. A linear measurement map S:Rn×p→Rm\mathcal S:\mathbb R^{n\times p}\to\mathbb R^mS:Rn×p→Rm is given by matrices A1,…,AmA_1,\dots,A_mA1​,…,Am​ through S(X)l=⟨Al,X⟩\mathcal S(X)_l=\langle A_l,X\rangleS(X)l​=⟨Al​,X⟩; the data are M∈Rm\mathscr M\in\mathbb R^mM∈Rm.

The best kkk-rank approximation error is ρk(X)∗=min⁡rank⁡Z≤k∥X−Z∥∗\rho_k(X)_*=\min_{\operatorname{rank}Z\le k}\|X-Z\|_*ρk​(X)∗​=minrankZ≤k​∥X−Z∥∗​. The map S\mathcal SS has the strong rank null space property (SRNSP) of order kkk with constant η∈(0,1)\eta\in(0,1)η∈(0,1) if every nonzero X∈ker⁡SX\in\ker\mathcal SX∈kerS and every split X=X1+X2X=X_1+X_2X=X1​+X2​ with rank⁡X1≤k\operatorname{rank}X_1\le krankX1​≤k admit another split X=H1+H2X=H_1+H_2X=H1​+H2​ with rank⁡H1≤2k\operatorname{rank}H_1\le2krankH1​≤2k, ⟨H1,H2⟩=0\langle H_1,H_2\rangle=0⟨H1​,H2​⟩=0, X1H2T=0X_1H_2^{\mathsf T}=0X1​H2T​=0, X1TH2=0X_1^{\mathsf T}H_2=0X1T​H2​=0 and ∥H1∥∗≤η∥H2∥∗\|H_1\|_*\le\eta\|H_2\|_*∥H1​∥∗​≤η∥H2​∥∗​.

For ε>0\varepsilon>0ε>0 the weight of XXX is W=UΣε−1UTW=U\Sigma_\varepsilon^{-1}U^{\mathsf T}W=UΣε−1​UT, where XXT=UΣ2UTXX^{\mathsf T}=U\Sigma^2U^{\mathsf T}XXT=UΣ2UT and Σε=diag⁡(max⁡{σj,ε})\Sigma_\varepsilon=\operatorname{diag}(\max\{\sigma_j,\varepsilon\})Σε​=diag(max{σj​,ε}). The IRLS-M algorithm with parameters K∈NK\in\mathbb NK∈N and γ>0\gamma>0γ>0 starts from W0=IW^0=IW0=I, ε0=1\varepsilon_0=1ε0​=1 and repeats

Xℓ∈arg⁡min⁡S(X)=M∥(Wℓ−1)1/2X∥F2,εℓ=min⁡{εℓ−1,γσK+1(Xℓ)},X^\ell\in\arg\min_{\mathcal S(X)=\mathscr M}\|(W^{\ell-1})^{1/2}X\|_F^2,\qquad\varepsilon_\ell=\min\{\varepsilon_{\ell-1},\gamma\sigma_{K+1}(X^\ell)\},Xℓ∈argS(X)=Mmin​∥(Wℓ−1)1/2X∥F2​,εℓ​=min{εℓ−1​,γσK+1​(Xℓ)},

with WℓW^\ellWℓ the weight of XℓX^\ellXℓ at level εℓ\varepsilon_\ellεℓ​; it stops when εℓ=0\varepsilon_\ell=0εℓ​=0. Two functionals organize the analysis: J(X,W)=12(∥W1/2X∥F2+∥W−1/2∥F2)\mathcal J(X,W)=\tfrac12(\|W^{1/2}X\|_F^2+\|W^{-1/2}\|_F^2)J(X,W)=21​(∥W1/2X∥F2​+∥W−1/2∥F2​), of which IRLS-M is an alternating minimization, and Jε(X)=∑i=1njε(σi(X))\mathcal J_\varepsilon(X)=\sum_{i=1}^n j^\varepsilon(\sigma_i(X))Jε​(X)=∑i=1n​jε(σi​(X)) with jε(u)=∣u∣j^\varepsilon(u)=|u|jε(u)=∣u∣ for ∣u∣≥ε|u|\ge\varepsilon∣u∣≥ε and (u2+ε2)/(2ε)(u^2+\varepsilon^2)/(2\varepsilon)(u2+ε2)/(2ε) otherwise.

Formalization targets

Goal: Theorem 6.11

For γ=1/n\gamma=1/nγ=1/n, any KKK, a surjective S\mathcal SS and any run (Xℓ,εℓ)(X^\ell,\varepsilon_\ell)(Xℓ,εℓ​):

(i)S SRNSP of order K, εℓ→0 ⟹ Xℓ→Xˉ, rank⁡Xˉ≤K, Xˉ=the unique nuclear norm minimizer.\text{(i)}\quad \mathcal S\ \text{SRNSP of order }K,\ \varepsilon_\ell\to0\ \Longrightarrow\ X^\ell\to\bar X,\ \operatorname{rank}\bar X\le K,\ \bar X=\text{the unique nuclear norm minimizer.}(i)S SRNSP of order K, εℓ​→0 ⟹ Xℓ→Xˉ, rankXˉ≤K, Xˉ=the unique nuclear norm minimizer.

(ii) If εℓ→ε>0\varepsilon_\ell\to\varepsilon>0εℓ​→ε>0, the iterates are relatively compact, their accumulation points minimize Jε\mathcal J_\varepsilonJε​ on the feasible set, and the sequence converges when that minimizer is unique; under the SRNSP with η<1−2/(K−2)\eta<1-2/(K-2)η<1−2/(K−2), every accumulation point Xˉ\bar XXˉ satisfies, for every feasible XXX and k<K−2η/(1−η)k<K-2\eta/(1-\eta)k<K−2η/(1−η),

∥X−Xˉ∥∗≤Λρk(X)∗,Λ=4(1+η)2(1−η)2((K−k)(1−η)−2η)+2(1+η)1−η.\|X-\bar X\|_*\le\Lambda\rho_k(X)_*,\qquad\Lambda=\frac{4(1+\eta)^2}{(1-\eta)^2((K-k)(1-\eta)-2\eta)}+\frac{2(1+\eta)}{1-\eta}.∥X−Xˉ∥∗​≤Λρk​(X)∗​,Λ=(1−η)2((K−k)(1−η)−2η)4(1+η)2​+1−η2(1+η)​.

(iii) Under the same SRNSP, if a feasible matrix of rank at most kkk exists, then εℓ→0\varepsilon_\ell\to0εℓ​→0.

Milestones

In attack order: the weighted least squares step (Lemma 5.1, the optimality condition (5.4)); the weight step (Lemma 5.2, Proposition 5.3); monotonicity of J\mathcal JJ along the run (Proposition 6.1); singular value facts (Weyl's Theorem 7.1, attainment of ρk\rho_kρk​ at the spectral truncation, Lemma 6.10, Proposition 7.2); null space theory (Theorem 6.3, the inverse triangle inequality Lemma 6.6 with (6.5), Corollary 6.7); and the two steps of the proof of (ii), the optimality condition (6.10) for Jε\mathcal J_\varepsilonJε​ and the bound (6.11).

Significance

Theorem 6.11 is the convergence guarantee of IRLS-M. Combined with the fact that a small rank restricted isometry constant implies the SRNSP (Proposition 6.8, the companion mission), it yields Proposition 2.1 of the paper: under δ4K<2−1\delta_{4K}<\sqrt2-1δ4K​<2​−1, IRLS-M recovers every rank-kkk matrix exactly and approximately low-rank matrices stably. Part (iii) says that the algorithm detects exact low-rank data on its own: the smoothing parameter must vanish.

The result is proved on paper; no machine-checked proof exists. A complete formalization would give a machine-checked convergence proof of an IRLS-type method; none is on the platform, for vectors or matrices. It also produces reusable matrix analysis: Weyl's perturbation bound for singular values, the nuclear norm best rank-kkk approximation (a Mirsky-type theorem), additivity of the nuclear norm under orthogonality, the null space characterization of nuclear norm recovery, and optimality conditions for spectral functions.

Difficulty

Two steps resist the obvious argument. First, the weight update is a constrained minimization over the positive definite cone; identifying its solution (Proposition 5.3) requires a duality or spectral argument rather than setting a gradient to zero, because the constraint W⪯ε−1IW\preceq\varepsilon^{-1}IW⪯ε−1I is active on small singular values. Second, in case (ii) the limit functional Jε\mathcal J_\varepsilonJε​ is convex but not strictly convex, so accumulation points cannot be pinned down by uniqueness; the analysis must instead pass the optimality condition (5.4) of the iterates to the limit, using continuity of the weights in the iterate, and derive (6.10). The step relating ∇Jε\nabla\mathcal J_\varepsilon∇Jε​ to WXˉW\bar XWXˉ needs the differentiability of unitarily invariant spectral functions, which the paper imports from Lewis and Sendov. Weyl's inequality and the spectral truncation facts, routine on paper, are not yet in Mathlib for rectangular matrices.

Formalization scope

All matrices are real (Matrix (Fin n) (Fin p) ℝ); the paper treats real and complex matrices alike. The paper's standing assumption n≤pn\le pn≤p is a hypothesis wherever n×nn\times nn×n objects (XXTXX^{\mathsf T}XXT, WWW, γ=1/n\gamma=1/nγ=1/n, Jε\mathcal J_\varepsilonJε​) occur. Nuclear norm, Frobenius norm, trace inner product and singular values come from the published definition HighDimStat_MatrixRank_Core; sv X i is σi+1(X)\sigma_{i+1}(X)σi+1​(X), 0-based. The measurement map is given by measurement matrices (observationOp), which represents every linear map to Rm\mathbb R^mRm. The weight is defined with Mathlib's continuous functional calculus, and W1/2W^{1/2}W1/2 is cfc Real.sqrt W. The algorithm is the relation IsRun: each Xℓ+1X^{\ell+1}Xℓ+1 is some minimizer of (2.9), X0X^0X0 is free, and εj=0\varepsilon_j=0εj​=0 after a stop. Accumulation points are MapClusterPt; uniqueness of a nuclear norm minimizer is a strict inequality against every other feasible matrix.

The goal cannot be satisfied vacuously: IsRun has a run for every surjective S\mathcal SS and every M\mathscr MM (Lemma 5.1 supplies the minimizers), it carries no positivity or uniqueness assumption a real run could violate, and the theorem keeps all three parts, including the unique-minimizer clause of (i) and the error bound of (ii) for every feasible XXX and every admissible kkk.

Two printed slips are corrected and disclosed: (5.5) omits the factor 12\tfrac1221​ of (5.1), and (6.5) reverses the bracket of (6.4) at ρk=0\rho_k=0ρk​=0. Contributions welcome: Weyl's inequality and the Mirsky-type truncation theorem for rectangular matrices, the spectral calculus behind Propositions 5.3 and (6.10), and proofs of the null space results, which are independent of the algorithm.

Selected references

  • M. Fornasier, H. Rauhut, R. Ward, Low-rank matrix recovery via iteratively reweighted least squares minimization, SIAM J. Optim. 21(4), 2011. https://arxiv.org/abs/1010.2471 (v4 is the version formalized)
  • B. Recht, M. Fazel, P. A. Parrilo, Guaranteed minimum-rank solutions of linear matrix equations via nuclear norm minimization, SIAM Review 52(3), 2010. https://doi.org/10.1137/070697835
  • B. Recht, W. Xu, B. Hassibi, Null space conditions and thresholds for rank minimization, Math. Program. 127, 2011. https://doi.org/10.1007/s10107-010-0422-2
  • I. Daubechies, R. DeVore, M. Fornasier, C. S. Güntürk, Iteratively reweighted least squares minimization for sparse recovery, Comm. Pure Appl. Math. 63(1), 2010. https://doi.org/10.1002/cpa.20303
  • K. Mohan, M. Fazel, Iterative reweighted least squares for matrix rank minimization, Proc. Allerton Conference, 2010; journal version Iterative reweighted algorithms for matrix rank minimization, JMLR 13, 2012. https://jmlr.org/papers/v13/mohan12a.html
  • E. J. Candès, B. Recht, Exact matrix completion via convex optimization, Found. Comput. Math. 9, 2009. https://doi.org/10.1007/s10208-009-9045-5
  • J.-F. Cai, E. J. Candès, Z. Shen, A singular value thresholding algorithm for matrix completion, SIAM J. Optim. 20(4), 2010. https://doi.org/10.1137/080738970
  • A. S. Lewis, H. S. Sendov, Nonsmooth analysis of singular values. I: Theory, Set-Valued Analysis 13(3), 2005. https://doi.org/10.1007/s11228-004-7197-7
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ProbabilityRandom Matrix Theory·Captain: mikedeng1

Random Matrices: Universality of ESDs and the Circular Law 2: The ESD of A_n/√n Converges to μ iff the Normalized Log-Determinants of A_n/√n − zI Converge to μ's Log-Potential for a.e. zResearch Paper

Motivation

The eigenvalues of a large non-Hermitian random matrix are hard to study directly. For Hermitian matrices, the empirical spectral distribution (ESD) is controlled by the resolvent and the Stieltjes transform, both stable under small perturbations. For non-Hermitian matrices no such tool exists: eigenvalues can move a long way under tiny perturbations, and the moment method fails because moments do not determine a measure on C\mathbb CC. The route that works, going back to Girko (1984) and used by Bai (1997), Götze–Tikhomirov (2007), Pan–Zhou (2007) and Tao–Vu (2008), passes through logarithmic determinants. The identity 1nlog⁡∣det⁡(A−zI)∣=∫log⁡∣w−z∣ dμA(w)\frac1n\log|\det(A-zI)|=\int\log|w-z|\,d\mu_A(w)n1​log∣det(A−zI)∣=∫log∣w−z∣dμA​(w) links the ESD μA\mu_AμA​ to a scalar quantity. That scalar is computable from the singular values of A−zIA-zIA−zI, which are eigenvalues of a Hermitian matrix.

Tao and Vu, with an appendix by Krishnapur (Ann. Probab. 38 (2010) 2023–2065), turn this link into an exact criterion. Theorem 1.15 of that paper states that the ESD of a normalized i.i.d. random matrix converges to a measure μ\muμ if and only if the normalized log-determinants converge to the logarithmic potential of μ\muμ for almost every zzz. The same holds for a regularized version built from the singular values. This mission formalizes Theorem 1.15 and the main steps of its proof (§8 and Appendix A of the published article).

Setting

Let xxx be a complex random variable with Ex=0\mathbf E x=0Ex=0 and E∣x∣2=1\mathbf E|x|^2=1E∣x∣2=1, and let (xij)i,j≥1(x_{ij})_{i,j\ge1}(xij​)i,j≥1​ be independent copies of xxx on a probability space (Ω,P)(\Omega,\mathbf P)(Ω,P). For each nnn, Xn=(xij)1≤i,j≤nX_n=(x_{ij})_{1\le i,j\le n}Xn​=(xij​)1≤i,j≤n​. Let MnM_nMn​ be deterministic n×nn\times nn×n complex matrices with

(1.3)sup⁡n1n2∥Mn∥22<∞,∥M∥22=∑i,j∣mij∣2,\text{(1.3)}\qquad\sup_n\frac1{n^2}\|M_n\|_2^2<\infty,\qquad\|M\|_2^2=\sum_{i,j}|m_{ij}|^2,(1.3)nsup​n21​∥Mn​∥22​<∞,∥M∥22​=i,j∑​∣mij​∣2,

and put An=Mn+XnA_n=M_n+X_nAn​=Mn​+Xn​.

For A∈Mn(C)A\in M_n(\mathbb C)A∈Mn​(C) with eigenvalues λ1,…,λn\lambda_1,\dots,\lambda_nλ1​,…,λn​, counted with algebraic multiplicity, the ESD is μA=1n∑iδλi\mu_A=\frac1n\sum_i\delta_{\lambda_i}μA​=n1​∑i​δλi​​. Its singular values are σ1(A)≥⋯≥σn(A)≥0\sigma_1(A)\ge\dots\ge\sigma_n(A)\ge0σ1​(A)≥⋯≥σn​(A)≥0. A sequence of random measures μn\mu_nμn​ converges in probability to a deterministic μ\muμ if, for every continuous compactly supported f:C→Rf:\mathbb C\to\mathbb Rf:C→R, ∫f dμn−∫f dμ\int f\,d\mu_n-\int f\,d\mu∫fdμn​−∫fdμ tends to 000 in probability. It converges almost surely if, with probability one, ∫f dμn→∫f dμ\int f\,d\mu_n\to\int f\,d\mu∫fdμn​→∫fdμ for all such fff at once. The logarithmic potential of a measure μ\muμ is z↦∫log⁡∣w−z∣ dμ(w)z\mapsto\int\log|w-z|\,d\mu(w)z↦∫log∣w−z∣dμ(w).

Hypothesis (1.4) states that, for almost every zzz, the ESDs of the deterministic matrices (1nMn−zI)(1nMn−zI)∗(\frac1{\sqrt n}M_n-zI)(\frac1{\sqrt n}M_n-zI)^*(n​1​Mn​−zI)(n​1​Mn​−zI)∗ converge to a limit.

In Lean everything lives in the namespace UnivESD.LogDet. The ESD is esd, the one-based singular value is sv, logPotential is the logarithmic potential, and ConvInProb/ConvAS/ESDConvInProb/ESDConvAS are the modes of convergence. IIDArray is the entry model, HSBound is (1.3), shiftA M xs z n ω is 1nAn−zI\frac1{\sqrt n}A_n-zIn​1​An​−zI, and Cond14 is (1.4).

Formalization targets

Goal: Theorem 1.15

Let μ\muμ be a probability measure on C\mathbb CC with ∫∣z∣2 dμ<∞\int|z|^2\,d\mu<\infty∫∣z∣2dμ<∞. The following are equivalent:

  1. μ1nAn→μ\mu_{\frac1{\sqrt n}A_n}\to\muμn​1​An​​→μ in probability;
  2. for a.e. zzz, 1nlog⁡∣det⁡(1nAn−zI)∣→∫Clog⁡∣w−z∣ dμ(w)\displaystyle\frac1n\log\Big|\det\big(\tfrac1{\sqrt n}A_n-zI\big)\Big|\to\int_{\mathbb C}\log|w-z|\,d\mu(w)n1​log​det(n​1​An​−zI)​→∫C​log∣w−z∣dμ(w) in probability;
  3. for a.e. zzz there are εn>0\varepsilon_n>0εn​>0, εn→0\varepsilon_n\to0εn​→0, with
1nlog⁡det⁡((1nAn−zI)(1nAn−zI)∗+εnI)→2∫Clog⁡∣w−z∣ dμ(w)\frac1n\log\det\Big(\big(\tfrac1{\sqrt n}A_n-zI\big)\big(\tfrac1{\sqrt n}A_n-zI\big)^*+\varepsilon_nI\Big)\to2\int_{\mathbb C}\log|w-z|\,d\mu(w)n1​logdet((n​1​An​−zI)(n​1​An​−zI)∗+εn​I)→2∫C​log∣w−z∣dμ(w)

in probability.

Under (1.4) the same equivalence holds with almost sure convergence throughout.

Milestones, in the order the proof uses them

  • (8.1): for a.e. zzz, w↦log⁡∣w−z∣w\mapsto\log|w-z|w↦log∣w−z∣ is μ\muμ-integrable.
  • Lemma A.3 (Weyl's comparison for products): ∏j≤J∣λj∣≤∏j≤Jσj(A)\prod_{j\le J}|\lambda_j|\le\prod_{j\le J}\sigma_j(A)∏j≤J​∣λj​∣≤∏j≤J​σj​(A) and ∏j≥Jσj(A)≤∏j≥J∣λj∣\prod_{j\ge J}\sigma_j(A)\le\prod_{j\ge J}|\lambda_j|∏j≥J​σj​(A)≤∏j≥J​∣λj​∣.
  • (8.3): P(σn−i≤ci/n)=O(exp⁡(−n0.01))\mathbf P(\sigma_{n-i}\le ci/n)=O(\exp(-n^{0.01}))P(σn−i​≤ci/n)=O(exp(−n0.01)) for 2n0.99≤i≤n−12n^{0.99}\le i\le n-12n0.99≤i≤n−1.
  • (8.2): 1n∑i=1n(log⁡σi2+εn−log⁡σi)→0\frac1n\sum_{i=1}^n\big(\log\sqrt{\sigma_i^2+\varepsilon_n}-\log\sigma_i\big)\to0n1​∑i=1n​(logσi2​+εn​​−logσi​)→0 almost surely.
  • p. 2057: almost surely, eventually, 1n∑(1−κ)n<i≤nlog⁡1σi≤O(κlog⁡1κ)\frac1n\sum_{(1-\kappa)n<i\le n}\log\frac1{\sigma_i}\le O(\kappa\log\frac1\kappa)n1​∑(1−κ)n<i≤n​logσi​1​≤O(κlogκ1​), and the same bound for log⁡1∣λi∣\log\frac1{|\lambda_i|}log∣λi​∣1​.

Significance

Theorem 1.15 reduces convergence of a non-Hermitian ESD to a family of scalar limit statements. Each of these can be attacked through Hermitian tools, because the regularized log-determinant in (iii) is a smooth functional of the singular values. Corollary 1.16 of the paper derives from it a practical criterion: the ESD converges to μ\muμ once the singular value distributions of 1nAn−zI\frac1{\sqrt n}A_n-zIn​1​An​−zI converge for a.e. zzz to laws ηz\eta_zηz​ with ∫log⁡t dηz=2∫log⁡∣w−z∣ dμ\int\log t\,d\eta_z=2\int\log|w-z|\,d\mu∫logtdηz​=2∫log∣w−z∣dμ. With the universality principle (Theorem 1.5, the companion mission) and Mehta's computation for complex Gaussian matrices, this yields the circular law for i.i.d. matrices with finite variance.

The theorem is proved in the source. To our knowledge neither it nor any of its milestones has a machine-checked proof. Mathlib has the ingredients for the objects (characteristic polynomials and their roots, LinearMap.singularValues, the strong law of large numbers) but not the results. A formal proof would give the platform its first verified bridge between eigenvalue and singular value asymptotics. Lemma A.3 alone, Weyl's multiplicative majorization, is a standard linear-algebra fact absent from Mathlib.

Difficulty

Two things make the obvious argument fail. First, log⁡\loglog is unbounded at 000. Vague convergence of μ1nAn\mu_{\frac1{\sqrt n}A_n}μn​1​An​​ controls ∫f dμn\int f\,d\mu_n∫fdμn​ only for continuous compactly supported fff, while log⁡∣w−z∣\log|w-z|log∣w−z∣ has a singularity at w=zw=zw=z and grows at infinity. Passing between (i) and (ii) therefore requires uniform control of the eigenvalues (and singular values) near 000 after the shift: the contribution of the smallest ones must vanish. Second, eigenvalues are not stable under perturbation, so this control cannot be read off the eigenvalues. It has to come from the singular values, through a lower-tail bound on σn−i\sigma_{n-i}σn−i​ that is exponentially small in a power of nnn, and through a deterministic inequality transferring bounds from singular values to eigenvalues. The smallest singular values (iii below n0.99n^{0.99}n0.99) need a separate polynomial lower bound (the paper's Lemma 4.1, posed in the companion mission). The tail bound in its printed form is false at that end of the range.

Formalization scope

Conventions committed to in Lean:

  • The ESD is n−1n^{-1}n−1 times the sum of Dirac masses over the root multiset of the characteristic polynomial, so multiplicities are kept. Test functions are real-valued, continuous and compactly supported. Almost sure ESD convergence uses one null set for all test functions.
  • The matrices XnX_nXn​ are the top-left corners of one infinite i.i.d. array. In-probability statements do not depend on how the XnX_nXn​ are coupled across nnn, but almost-sure statements do, and the paper's proof applies the strong law to this array. The limit in (1.4) is required to be a probability measure, which is equivalent under (1.3).
  • The second-moment condition on μ\muμ is Integrable (‖w‖²) μ. The logarithmic potential is a Bochner integral, which is 000 when not integrable; by (8.1) this happens only for a null set of zzz, which "for a.e. zzz" ignores.
  • Real.log 0 = 0. In (ii), a singular matrix would contribute 000 instead of −∞-\infty−∞; for this model the determinant is almost surely nonzero eventually. Every milestone with log⁡σi\log\sigma_ilogσi​ or log⁡∣λi∣\log|\lambda_i|log∣λi​∣ carries positivity of those quantities in its conclusion.
  • Singular values are one-based (sv A i is Mathlib's singularValues (i-1)). Eigenvalue enumerations are Fin n-indexed, and the paper's λi\lambda_iλi​ is index i−1i-1i−1.
  • The paper's O(⋅)O(\cdot)O(⋅) constants are existential and fixed before nnn. In the κlog⁡(1/κ)\kappa\log(1/\kappa)κlog(1/κ) bounds the constant is fixed before κ\kappaκ; a κ\kappaκ-dependent constant would make the bounds empty.

Disclosed corrections to the printed text:

  1. (iii)'s matrix. Theorem 1.15 prints a mis-bracketed product, and (1.8) prints (C+εnI)(C∗+εnI)(C+\varepsilon_nI)(C^*+\varepsilon_nI)(C+εn​I)(C∗+εn​I). The Lean uses CC∗+εnICC^*+\varepsilon_nICC∗+εn​I with C=1nAn−zIC=\frac1{\sqrt n}A_n-zIC=n​1​An​−zI, the matrix of (8.2) and of the proof of Corollary 1.16.
  2. (8.3)'s range. It is printed for 1≤i≤n−n0.991\le i\le n-n^{0.99}1≤i≤n−n0.99, which is false for small iii: for Gaussian entries and Mn=0M_n=0Mn​=0, nσn−1n\sigma_{n-1}nσn−1​ has a non-degenerate limit law. It is posed on 2n0.99≤i≤n−12n^{0.99}\le i\le n-12n0.99≤i≤n−1, the range the proof covers and the use needs.
  3. Lemma A.3, second inequality. It is posed for 1≤J≤n1\le J\le n1≤J≤n, since σ0\sigma_0σ0​ is undefined. The eigenvalues are ordered ∣λ1∣≥⋯≥∣λn∣|\lambda_1|\ge\dots\ge|\lambda_n|∣λ1​∣≥⋯≥∣λn​∣, not ∣λ1∣≤⋯≤∣λn∣|\lambda_1|\le\dots\le|\lambda_n|∣λ1​∣≤⋯≤∣λn​∣ as printed: the printed order is a slip. With it, both inequalities are weaker than Weyl's and cannot support the use on p. 2057, which orders the eigenvalues decreasingly. The decreasing order implies the printed form.
  4. (8.2) and (8.1). (8.2) is stated for every deterministic εn>0\varepsilon_n>0εn​>0 with εn→0\varepsilon_n\to0εn​→0; the proof uses nothing else. (8.1) is stated as μ\muμ-integrability plus local integrability of z↦∫∣log⁡∣w−z∣∣ dμ(w)z\mapsto\int|\log|w-z||\,d\mu(w)z↦∫∣log∣w−z∣∣dμ(w).

A trivializing formalization is ruled out by construction. The goal mentions only AnA_nAn​ and μ\muμ. The proof's comparison ensemble Bn=n diag(λi)B_n=\sqrt n\,\mathrm{diag}(\lambda_i)Bn​=n​diag(λi​) is not a hypothesis. No statement takes a log-potential or a log-determinant as an input that could be fixed to make it hold.

The companion mission (Theorem 1.5, universality) poses Theorem 2.1 (the replacement principle), Lemma 1.7 (tightness) and Lemma 4.1 (least singular value), which the proof here also uses. They are not restated here. Once that mission is published they belong here as references. Contributions are welcome on the linear-algebra layer (Lemma A.3, multiplicative Weyl majorization), the Fubini argument of (8.1), and the singular-value tail bound (8.3). These are reusable well beyond this paper.

Selected references

  • T. Tao, V. Vu (appendix by M. Krishnapur), Random matrices: Universality of ESDs and the circular law, Ann. Probab. 38(5) (2010) 2023–2065. https://doi.org/10.1214/10-AOP534 (source of this mission; published version).
  • V. L. Girko, The circular law, Teor. Veroyatnost. i Primenen. 29 (1984) 669–679. https://doi.org/10.1137/1129095
  • Z. D. Bai, Circular law, Ann. Probab. 25(1) (1997) 494–529. https://doi.org/10.1214/aop/1024404298
  • F. Götze, A. Tikhomirov, The circular law for random matrices, Ann. Probab. 38(4) (2010) 1444–1491. https://doi.org/10.1214/09-AOP522
  • T. Tao, V. Vu, Random matrices: the circular law, Commun. Contemp. Math. 10(2) (2008) 261–307. https://doi.org/10.1142/S0219199708002788
  • H. Weyl, Inequalities between the two kinds of eigenvalues of a linear transformation, Proc. Natl. Acad. Sci. USA 35 (1949) 408–411. https://doi.org/10.1073/pnas.35.7.408
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Numerical AnalysisOptimization·Captain: mikedeng1

The Primal-Dual Active Set Strategy as a Semismooth Newton Method III: Global Convergence under the Norm and Cone ConditionsResearch Paper

Motivation

Obstacle problems, contact problems and control-constrained optimal control problems lead, after discretization, to complementarity systems of the form "find y≤ψy \le \psiy≤ψ and λ≥0\lambda \ge 0λ≥0 with Ay+λ=fAy + \lambda = fAy+λ=f and λi(yi−ψi)=0\lambda_i(y_i - \psi_i) = 0λi​(yi​−ψi​)=0". The primal-dual active set strategy solves such systems by guessing which constraints are active, solving one linear system, and updating the guess. It is widely used because each iteration is a single linear solve and, in practice, it terminates after few iterations.

Hintermüller, Ito and Kunisch (SIAM J. Optim. 13(3), 2002; authors' version hal-01660511v1) showed that the strategy is a semismooth Newton method applied to a reformulation of the complementarity system with a max-function. This gives local superlinear convergence. For global convergence, from arbitrary initial data, the paper gives three sufficient conditions on the matrix AAA: the M-matrix case (Theorem 3.2), the condition of Theorem 3.3 treated in this mission, and small perturbations of M-matrices (Theorem 3.4). Theorem 3.3 is the one that goes beyond sign patterns: it covers P-matrices whose blocks satisfy a norm bound and a cone condition, with the sum of the components of yyy serving as a merit function.

Setting

Fix n≥0n \ge 0n≥0, a matrix A∈Rn×nA \in \mathbb{R}^{n \times n}A∈Rn×n, vectors f,ψ∈Rnf, \psi \in \mathbb{R}^nf,ψ∈Rn and a parameter c>0c > 0c>0. Vectors are ordered componentwise. The problem is

Ay+λ=f,λ−max⁡(0,λ+c(y−ψ))=0,(3.1)Ay + \lambda = f, \qquad \lambda - \max\big(0, \lambda + c(y - \psi)\big) = 0, \tag{3.1}Ay+λ=f,λ−max(0,λ+c(y−ψ))=0,(3.1)

with the maximum taken componentwise. In the paper's notation the matrix is AAA and the index sets are calligraphic: A\mathcal{A}A (active) and I\mathcal{I}I (inactive).

A P-matrix is a square matrix all of whose principal minors are positive. For an index set I⊆{1,…,n}\mathcal{I} \subseteq \{1,\dots,n\}I⊆{1,…,n} with complement A\mathcal{A}A, AIA_{\mathcal{I}}AI​ is the principal submatrix of AAA on I\mathcal{I}I, and AIAA_{\mathcal{I}\mathcal{A}}AIA​ is the submatrix with rows in I\mathcal{I}I and columns in A\mathcal{A}A. For a P-matrix every AIA_{\mathcal{I}}AI​ is invertible.

The primal-dual active set algorithm starts from an arbitrary pair (y0,λ0)(y^0, \lambda^0)(y0,λ0). Given (yk,λk)(y^k, \lambda^k)(yk,λk) it sets

Ak={i:λik+c(yik−ψi)>0},Ik={i:λik+c(yik−ψi)≤0},\mathcal{A}_k = \{ i : \lambda^k_i + c(y^k_i - \psi_i) > 0 \}, \qquad \mathcal{I}_k = \{ i : \lambda^k_i + c(y^k_i - \psi_i) \le 0 \},Ak​={i:λik​+c(yik​−ψi​)>0},Ik​={i:λik​+c(yik​−ψi​)≤0},

and determines (yk+1,λk+1)(y^{k+1}, \lambda^{k+1})(yk+1,λk+1) from

Ayk+1+λk+1=f,yk+1=ψ on Ak,λk+1=0 on Ik.Ay^{k+1} + \lambda^{k+1} = f, \qquad y^{k+1} = \psi \text{ on } \mathcal{A}_k, \qquad \lambda^{k+1} = 0 \text{ on } \mathcal{I}_k .Ayk+1+λk+1=f,yk+1=ψ on Ak​,λk+1=0 on Ik​.

For a rectangular matrix BBB, B+B_+B+​ is the matrix of the positive parts max⁡(0,bij)\max(0, b_{ij})max(0,bij​) of its entries, and ∥⋅∥1\|\cdot\|_1∥⋅∥1​ is the matrix norm subordinate to the one-norms, i.e. the maximal absolute column sum. Thus ∥B+∥1=max⁡j∑imax⁡(0,bij)\|B_+\|_1 = \max_j \sum_i \max(0, b_{ij})∥B+​∥1​=maxj​∑i​max(0,bij​).

Formalization targets

Goal: Theorem 3.3

If AAA is a P-matrix and for every partition of {1,…,n}\{1, \dots, n\}{1,…,n} into disjoint sets I\mathcal{I}I and A\mathcal{A}A

∥(AI−1AIA)+∥1<1and∑i∈I(AI−1v)i≥0  for all v≥0,\big\|(A_{\mathcal{I}}^{-1} A_{\mathcal{I}\mathcal{A}})_+\big\|_1 < 1 \qquad\text{and}\qquad \sum_{i \in \mathcal{I}} (A_{\mathcal{I}}^{-1} v)_i \ge 0 \ \text{ for all } v \ge 0,​(AI−1​AIA​)+​​1​<1andi∈I∑​(AI−1​v)i​≥0  for all v≥0,

then for every solution x∗=(y∗,λ∗)x^* = (y^*, \lambda^*)x∗=(y∗,λ∗) of (3.1) and every run of the algorithm, xk=(yk,λk)→x∗x^k = (y^k, \lambda^k) \to x^*xk=(yk,λk)→x∗.

Milestones

The proof in the paper passes through the following claims, in order: the sign facts λIkk≤0\lambda^k_{\mathcal{I}_k} \le 0λIk​k​≤0 and yAkk≥ψAky^k_{\mathcal{A}_k} \ge \psi_{\mathcal{A}_k}yAk​k​≥ψAk​​ for k≥1k \ge 1k≥1; the update formula on the inactive set derived from the Newton system (3.3); inequality (3.6); inequality (3.7),

∑i=1n(yik+1−yik)≤−∥yk−ψ∥1,Ak+∥(AIk−1AIkAk)+∥1 ∥yk−ψ∥1,Ak;\sum_{i=1}^n (y^{k+1}_i - y^k_i) \le -\|y^k - \psi\|_{1,\mathcal{A}_k} + \big\|(A_{\mathcal{I}_k}^{-1} A_{\mathcal{I}_k\mathcal{A}_k})_+\big\|_1 \, \|y^k - \psi\|_{1,\mathcal{A}_k};i=1∑n​(yik+1​−yik​)≤−∥yk−ψ∥1,Ak​​+​(AIk​−1​AIk​Ak​​)+​​1​∥yk−ψ∥1,Ak​​;

and the fact that a repeated active set yields a solution of (3.1).

Companion statements

Existence of a run from every initial pair when AAA is a P-matrix; Remark 3.3 (an M-matrix satisfies the conditions of Theorem 3.3); and the stronger conclusion of the proof, that every run reaches x∗x^*x∗ after finitely many steps.

Significance

Theorem 3.3 gives global convergence of the primal-dual active set strategy for a class of matrices that is not restricted to M-matrices, and identifies M(y)=∑iyi\mathcal{M}(y) = \sum_i y_iM(y)=∑i​yi​ as a merit function under its two conditions. The paper points out that the result applies to discretizations of control-constrained optimal control problems, where the system matrix is generally not an M-matrix, and Remark 3.3 shows that the M-matrix case falls under it.

The result is proved on paper; none of it has been machine-checked. A formal development would produce a checked global convergence theorem for a semismooth Newton method, together with reusable statements about principal blocks of P-matrices and the subordinate one-norm of a positive part. The step from "the merit function does not increase" to convergence is the part of the paper's argument that a formal proof has to make fully precise (see below).

Difficulty

The obvious route is the paper's: show that ∑iyik\sum_i y^k_i∑i​yik​ decreases strictly until the active set repeats, conclude that no active set can recur, and use finiteness of the set of possible active sets. The inequalities (3.6) and (3.7) give only a non-strict decrease. The paper's assertion "<0< 0<0, unless yk+1=yky^{k+1} = y^kyk+1=yk" does not follow from them as written: the right-hand side of (3.7) vanishes when yk=ψy^k = \psiyk=ψ on Ak\mathcal{A}_kAk​, and the cone condition permits ∑i∈I(AI−1λIk)i=0\sum_{i \in \mathcal{I}} (A_{\mathcal{I}}^{-1}\lambda^k_{\mathcal{I}})_i = 0∑i∈I​(AI−1​λIk​)i​=0 with λIk≠0\lambda^k_{\mathcal{I}} \neq 0λIk​=0. A complete proof has to exclude cycling among active sets at equal merit value by a further argument. That is the central difficulty of this mission, and the reason the strict part of (3.7) is not stated as a milestone.

Formalization scope

Vectors are Fin n → ℝ and matrices Matrix (Fin n) (Fin n) ℝ; index sets are Finset (Fin n) and blocks are submatrices along the subtype inclusion. The P-matrix predicate is the published definition RobinsonSR.Schur.IsPMatrix (every nonempty principal minor is positive). The algorithm is encoded as a relation between consecutive iterates, and a run is an infinite sequence related step by step with arbitrary initial data; the stopping option of the algorithm is not modelled. The solution of (3.1) enters as a hypothesis: for a P-matrix it exists and is unique, so no assumption beyond the paper is made. Convergence is convergence of (yk,λk)(y^k, \lambda^k)(yk,λk) in Rn×Rn\mathbb{R}^n \times \mathbb{R}^nRn×Rn. The parameter c>0c > 0c>0 is the paper's standing assumption.

Conventions committed to:

  • both conditions of Theorem 3.3 range over every index set, including I=∅\mathcal{I} = \emptysetI=∅ and I={1,…,n}\mathcal{I} = \{1,\dots,n\}I={1,…,n};
  • ∥B+∥1\|B_+\|_1∥B+​∥1​ is the maximal column sum of the positive part, computed as a supremum in R≥0\mathbb{R}_{\ge 0}R≥0​, and equals 000 for a matrix with no columns;
  • the cone condition is ∑i∈I(AI−1v)i≥0\sum_{i\in\mathcal{I}}(A_{\mathcal{I}}^{-1}v)_i \ge 0∑i∈I​(AI−1​v)i​≥0 for v≥0v \ge 0v≥0, not entrywise nonnegativity of AI−1A_{\mathcal{I}}^{-1}AI−1​;
  • the milestones on the iterates hold from k=1k = 1k=1 on, as in the paper.

The goal does not assume a decrease of the merit function or finite termination; a formalization that adds either as a hypothesis would be trivial and is ruled out. The run-existence companion shows that the hypothesis "let (yk,λk)(y^k,\lambda^k)(yk,λk) be a run" can be met, so the goal is not vacuous.

A complete development needs: invertibility of principal blocks of a P-matrix, the block form of one step, the elementary estimate of ∑i(Bx)i\sum_i (B x)_i∑i​(Bx)i​ by ∥B+∥1∑jxj\|B_+\|_1 \sum_j x_j∥B+​∥1​∑j​xj​ for x≥0x \ge 0x≥0, and an argument that excludes cycling. Proofs of any milestone, of the companion statements, or of the goal through an argument other than the paper's are welcome.

Selected references

  • M. Hintermüller, K. Ito, K. Kunisch, The primal-dual active set strategy as a semismooth Newton method, SIAM J. Optim. 13(3):865–888, 2002. https://doi.org/10.1137/S1052623401383558 ; authors' version https://hal.science/hal-01660511v1
  • A. Berman, R. J. Plemmons, Nonnegative Matrices in the Mathematical Sciences, Academic Press, 1979 (SIAM Classics reprint 1994). https://doi.org/10.1137/1.9781611971262
10 thms1 active userReviewed
ProbabilityRandom Matrix Theory·Captain: mikedeng1

Random Matrices: Universality of ESDs and the Circular Law 1: For i.i.d. Zero-Mean Unit-Variance Entries, the ESD of (M_n + X_n)/√n Does Not Depend on the Entry Distribution in the LimitResearch Paper

Motivation

The eigenvalues of a large random matrix with independent entries follow deterministic limiting laws. For non-Hermitian matrices with i.i.d. entries of mean zero and variance one, the circular law asserts that the eigenvalues of 1nXn\frac1{\sqrt n}X_nn​1​Xn​ become uniformly distributed on the unit disk. These laws are used across statistics (covariance and signal-plus-noise models), numerical analysis (spectra of perturbed matrices), mathematical physics and the theory of neural networks; what makes them usable is universality: the limit depends only on the mean and variance of the entries, not on their distribution.

Timeline of the circular law and its universality:

  • 1965: Ginibre computes the joint eigenvalue density for complex Gaussian entries; Mehta (1967) derives the circular law in that case.
  • 1984: Girko proposes a general approach via log-determinants; his argument has gaps.
  • 1997: Bai gives the first rigorous proof for continuous entries with finite (2+η)(2+\eta)(2+η)-th moment and bounded density.
  • 2007–2008: Götze–Tikhomirov, Pan–Zhou and Tao–Vu remove the density assumption under extra moment conditions, using lower bounds on the least singular value.
  • 2010: Tao and Vu (Ann. Probab. 38 (2010) 2023–2065) prove universality under the minimal assumption of finite variance, and with a deterministic shift MnM_nMn​; the circular law in full generality follows.

This mission formalizes the main universality theorem of that paper (Theorem 1.5) together with the lemmas its proof rests on.

Setting

Let AAA be an n×nn\times nn×n complex matrix with eigenvalues λ1,…,λn\lambda_1,\dots,\lambda_nλ1​,…,λn​, counted with algebraic multiplicity. Its empirical spectral distribution (ESD) is the probability measure

μA=1n∑i=1nδλi\mu_A=\frac1n\sum_{i=1}^n\delta_{\lambda_i}μA​=n1​i=1∑n​δλi​​

on C\mathbb CC. The Hilbert–Schmidt norm is ∥A∥22=trace(AA∗)=∑i,j∣aij∣2\|A\|_2^2=\mathrm{trace}(AA^*)=\sum_{i,j}|a_{ij}|^2∥A∥22​=trace(AA∗)=∑i,j​∣aij​∣2.

A complex random variable xxx has zero mean and unit variance if Ex=0\mathbf E x=0Ex=0 and E∣x∣2=1\mathbf E|x|^2=1E∣x∣2=1. Given such xxx and yyy, let Xn=(xij)1≤i,j≤nX_n=(x_{ij})_{1\le i,j\le n}Xn​=(xij​)1≤i,j≤n​ and Yn=(yij)1≤i,j≤nY_n=(y_{ij})_{1\le i,j\le n}Yn​=(yij​)1≤i,j≤n​ have entries that are i.i.d. copies of xxx, resp. yyy. Let MnM_nMn​ be deterministic n×nn\times nn×n matrices with

sup⁡n1n2∥Mn∥22<∞,(1.3)\sup_n\frac1{n^2}\|M_n\|_2^2<\infty,\qquad(1.3)nsup​n21​∥Mn​∥22​<∞,(1.3)

and set An=Mn+XnA_n=M_n+X_nAn​=Mn​+Xn​, Bn=Mn+YnB_n=M_n+Y_nBn​=Mn​+Yn​.

Measures on C\mathbb CC carry the vague topology: test functions are continuous compactly supported f:C→Rf:\mathbb C\to\mathbb Rf:C→R. The random measures μ1nAn−μ1nBn\mu_{\frac1{\sqrt n}A_n}-\mu_{\frac1{\sqrt n}B_n}μn​1​An​​−μn​1​Bn​​ converge to zero in probability if, for every test function fff and ε>0\varepsilon>0ε>0,

P(∣∫f dμ1nAn−∫f dμ1nBn∣≥ε)→0,\mathbf P\Bigl(\Bigl|\int f\,d\mu_{\frac1{\sqrt n}A_n}-\int f\,d\mu_{\frac1{\sqrt n}B_n}\Bigr|\ge\varepsilon\Bigr)\to0,P(​∫fdμn​1​An​​−∫fdμn​1​Bn​​​≥ε)→0,

and almost surely if, with probability one, the difference of integrals tends to zero for every test function. The additional hypothesis

(1.4)μ(1nMn−zI)(1nMn−zI)∗ converges for almost every z∈C(1.4)\qquad \mu_{(\frac1{\sqrt n}M_n-zI)(\frac1{\sqrt n}M_n-zI)^*}\ \text{converges for almost every } z\in\mathbb C(1.4)μ(n​1​Mn​−zI)(n​1​Mn​−zI)∗​ converges for almost every z∈C

concerns only the deterministic shift.

Formalization targets

Goal: Theorem 1.5 (universality principle)

μ1nAn−μ1nBn⟶0 in probability;(1.4) ⟹ μ1nAn−μ1nBn⟶0 almost surely.\mu_{\frac1{\sqrt n}A_n}-\mu_{\frac1{\sqrt n}B_n}\longrightarrow0\ \text{in probability};\qquad (1.4)\ \Longrightarrow\ \mu_{\frac1{\sqrt n}A_n}-\mu_{\frac1{\sqrt n}B_n}\longrightarrow0\ \text{almost surely}.μn​1​An​​−μn​1​Bn​​⟶0 in probability;(1.4) ⟹ μn​1​An​​−μn​1​Bn​​⟶0 almost surely.

The statement involves no limiting law: it compares two ensembles, so it holds whether or not μ1nAn\mu_{\frac1{\sqrt n}A_n}μn​1​An​​ itself converges.

Milestones

The proof combines three results, each a milestone:

  • Theorem 2.1 (replacement principle), in probability and almost surely: if 1n2(∥An∥22+∥Bn∥22)\frac1{n^2}(\|A_n\|_2^2+\|B_n\|_2^2)n21​(∥An​∥22​+∥Bn​∥22​) is bounded and, for almost every zzz, 1nlog⁡∣det⁡(1nAn−zI)∣−1nlog⁡∣det⁡(1nBn−zI)∣→0\frac1n\log|\det(\frac1{\sqrt n}A_n-zI)|-\frac1n\log|\det(\frac1{\sqrt n}B_n-zI)|\to0n1​log∣det(n​1​An​−zI)∣−n1​log∣det(n​1​Bn​−zI)∣→0, then μ1nAn−μ1nBn→0\mu_{\frac1{\sqrt n}A_n}-\mu_{\frac1{\sqrt n}B_n}\to0μn​1​An​​−μn​1​Bn​​→0.
  • Lemma 1.7 (tightness): 1n2∥An∥22\frac1{n^2}\|A_n\|_2^2n21​∥An​∥22​ and ∫∣z∣2 dμ1nAn\int|z|^2\,d\mu_{\frac1{\sqrt n}A_n}∫∣z∣2dμn​1​An​​ are almost surely bounded.
  • Proposition 2.2 (converging determinant): for every zzz, the log-determinant difference (2.2) tends to zero in probability, and almost surely if (1.4) holds at zzz.

Supporting milestones: the linear-algebra Lemmas A.1 (interlacing), A.2 (Weyl's second-moment inequality) and A.4 (negative second moment); the probabilistic dominated convergence Lemma 3.1; Girko's identity (Lemma 3.3); the least singular value bound (Lemma 4.1); the lower tail bound for distances to subspaces (Proposition 5.1); and the high- and low-dimensional row contributions (Lemmas 4.2 and 4.3).

Significance

The result. Theorem 1.5 with Mn=0M_n=0Mn​=0 and yyy complex Gaussian transfers Mehta's computation for the Ginibre ensemble to every zero-mean unit-variance entry distribution: this is the circular law under the optimal moment assumption (Theorem 1.10 of the paper). With nonzero MnM_nMn​ it gives universality for perturbed and non-centred matrices, including results with entries of nonzero mean. The replacement principle (Theorem 2.1) is a general tool: it reduces vague convergence of non-Hermitian ESDs to convergence of log-determinants and applies to ensembles without independent entries.

Formalizing it. The theorem is proved in the paper; no part of it, and no ESD of a non-Hermitian matrix, has been formalized. The mission produces a machine-checked statement of universality in the vague topology and a library of reusable pieces: ESDs of complex matrices, convergence of random measures in probability and almost surely, interlacing and Weyl-type inequalities for singular values, and Girko's identity. Lemmas 4.1 and 5.1 rest on results the paper cites (Tao–Vu's least singular value bound, Talagrand's concentration inequality); formalizing those is part of the work.

Difficulty

The ESD of a non-Hermitian matrix is not stable under small perturbations: eigenvalues of a nearly singular matrix can move a long way, so the moment method and the Stieltjes transform method that settle the Hermitian case do not apply. The log-determinant 1nlog⁡∣det⁡(1nAn−zI)∣\frac1n\log|\det(\frac1{\sqrt n}A_n-zI)|n1​log∣det(n​1​An​−zI)∣ is a stable proxy only if the small singular values of 1nAn−zI\frac1{\sqrt n}A_n-zIn​1​An​−zI are controlled, and with only a second moment on the entries the entries can be unbounded, which defeats standard concentration arguments. The obvious approach, comparing AnA_nAn​ and BnB_nBn​ by swapping entries one at a time, needs smooth bounded statistics of the matrix, and the log-determinant is neither: it is unbounded near singular matrices.

Formalization scope

Matrices are Matrix (Fin n) (Fin n) ℂ; eigenvalues are the roots of the characteristic polynomial as a multiset, so the ESD counts algebraic multiplicity; for n=0n=0n=0 the ESD is the zero measure, harmless because every statement is asymptotic. The Hilbert–Schmidt norm is written as an explicit sum, not Mathlib's default (sup) matrix norm. Singular values are Mathlib's zero-indexed LinearMap.singularValues, shifted so that σ1\sigma_1σ1​ is the largest.

Conventions committed to:

  • Coupling. XnX_nXn​ is the top-left n×nn\times nn×n corner of one infinite i.i.d. array; the almost-sure statements depend on this choice, the in-probability ones do not. No relation between the xxx- and yyy-arrays is assumed.
  • (1.4) asks for a probability measure as the vague limit; under (1.3) any vague limit of these ESDs is one.
  • Almost sure convergence of ESDs uses one null set for all test functions.
  • Junk values. Lean has log⁡0=0\log 0=0log0=0 and 1/0=01/0=01/0=0. Theorem 2.1 therefore states its "determinants are nonzero" clause explicitly, and Proposition 2.2 concludes it (the paper's (2.2) is −∞-\infty−∞ at a vanishing determinant, so its convergence includes nonvanishing); Lemmas 4.2 and 4.3 assert positivity of the row distances they take logarithms of; Lemma 3.1's (1+δ)(1+\delta)(1+δ)-moment is a lower integral with values in [0,∞][0,\infty][0,∞], since a Bochner integral would vanish for non-integrable functions and make the hypothesis vacuous.
  • O(⋅)O(\cdot)O(⋅) constants are existential and fixed before the quantities they must not depend on: before ε\varepsilonε in Lemmas 4.2 and 4.3, before the sample point in Lemma 4.1, after ccc and before n,d,Wn,d,Wn,d,W and the row shift in Proposition 5.1.
  • Section 4 setting. Lemmas 4.2 and 4.3 carry the standing reductions of §4 as hypotheses: z=0z=0z=0, the row bound (4.2) ∥Zi∥=O(n)\|Z_i\|=O(\sqrt n)∥Zi​∥=O(n​) for n/2≤i≤nn/2\le i\le nn/2≤i≤n (which the paper obtains by permuting rows), and, for Lemma 4.3, convergence of μ1nMnMn∗\mu_{\frac1nM_nM_n^*}μn1​Mn​Mn∗​​. Proposition 5.1 quantifies over every deterministic row shift.
  • Printed slip. On p. 2045 the YiY_iYi​ are called "the rows of 1nBn\frac1{\sqrt n}B_nn​1​Bn​" and then normalized again; here YiY_iYi​ are the rows of BnB_nBn​, matching XiX_iXi​.

A trivializing formalization is excluded: the goal mentions only ESDs, i.i.d. entries, (1.3) and (1.4) — no log-determinant or singular value hypothesis — and its in-probability half holds without (1.4). Lemmas 6.3 and 6.4 and the internal Lemmas 3.2, 3.4, 5.3, 6.1, 6.6, 6.7 and Theorems 5.2, B.1 are not posed. Contributions are welcome on any milestone, and particularly on the deterministic Lemmas A.1, A.2, A.4 and 3.3, which are reusable well beyond this mission.

Selected references

  • T. Tao, V. Vu (appendix by M. Krishnapur), Random matrices: universality of ESDs and the circular law, The Annals of Probability 38(5) (2010) 2023–2065. https://doi.org/10.1214/10-AOP534 (the source; the published article is the citation basis)
  • J. Ginibre, Statistical ensembles of complex, quaternion, and real matrices, J. Math. Phys. 6 (1965) 440–449. https://doi.org/10.1063/1.1704292
  • V. L. Girko, The circular law, Teor. Veroyatnost. i Primenen. 29 (1984) 669–679; English translation Theory Probab. Appl. 29 (1985) 694–706. https://doi.org/10.1137/1129095
  • Z. D. Bai, Circular law, Ann. Probab. 25 (1997) 494–529. https://doi.org/10.1214/aop/1024404298
  • T. Tao, V. Vu, Random matrices: the circular law, Commun. Contemp. Math. 10 (2008) 261–307. https://doi.org/10.1142/S0219199708002788
  • R. B. Dozier, J. W. Silverstein, On the empirical distribution of eigenvalues of large dimensional information-plus-noise-type matrices, J. Multivariate Anal. 98 (2007) 678–694. https://doi.org/10.1016/j.jmva.2006.09.006
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OptimizationProbabilityRandom Matrix Theory·Captain: mikedeng1

Guaranteed Minimum-Rank Solutions of Linear Matrix Equations via Nuclear Norm Minimization 2: Nearly Isometric Random Maps Have δ_r ≤ δ with Probability 1 − e^(−c₁p) Once p ≥ c₀r(m+n)log(mn)Research Paper

Motivation

Many problems in system identification, collaborative filtering, low-dimensional embedding and model reduction ask for the matrix of least rank in an affine space. Affine rank minimization — given a linear map A:Rm×n→Rp\mathcal A:\mathbb R^{m\times n}\to\mathbb R^pA:Rm×n→Rp and b∈Rpb\in\mathbb R^pb∈Rp, find a matrix of minimum rank with A(X)=b\mathcal A(X)=bA(X)=b — is NP-hard in general. Recht, Fazel and Parrilo (arXiv:0706.4138; SIAM Review 52(3), 2010, doi:10.1137/070697835) showed that the convex relaxation which minimizes the nuclear norm ∥X∥∗\|X\|_*∥X∥∗​ (the sum of the singular values) instead of the rank recovers the minimum-rank solution exactly whenever A\mathcal AA satisfies a restricted isometry property on low-rank matrices. That deterministic theorem is the subject of the companion mission in this series.

A deterministic condition is only useful if maps satisfying it exist and are common. This mission formalizes the paper's second main result: random linear maps from a broad class — including Gaussian, symmetric Bernoulli and sparse random matrices — satisfy the restricted isometry property with overwhelming probability once the number of measurements ppp is of order r(m+n)log⁡(mn)r(m+n)\log(mn)r(m+n)log(mn). This parallels the role of random matrices in compressed sensing (Candès–Tao 2005; Baraniuk, Davenport, DeVore and Wakin 2008), where the vector restricted isometry property is established for random measurement matrices by a concentration and covering argument.

Setting

Write ⟨X,Y⟩=Tr⁡(X⊤Y)\langle X,Y\rangle=\operatorname{Tr}(X^\top Y)⟨X,Y⟩=Tr(X⊤Y) for the trace inner product on Rm×n\mathbb R^{m\times n}Rm×n and ∥X∥F\|X\|_F∥X∥F​ for the Frobenius norm. A linear map A:Rm×n→Rp\mathcal A:\mathbb R^{m\times n}\to\mathbb R^pA:Rm×n→Rp is given by ppp measurement matrices X1,…,XpX_1,\dots,X_pX1​,…,Xp​ through A(X)i=⟨Xi,X⟩\mathcal A(X)_i=\langle X_i,X\rangleA(X)i​=⟨Xi​,X⟩; ∥A(X)∥\|\mathcal A(X)\|∥A(X)∥ is the Euclidean norm in Rp\mathbb R^pRp, and ∥A∥=sup⁡{∥A(X)∥:∥X∥F≤1}\|\mathcal A\|=\sup\{\|\mathcal A(X)\|:\|X\|_F\le1\}∥A∥=sup{∥A(X)∥:∥X∥F​≤1} is the operator norm.

The rrr-restricted isometry constant δr(A)\delta_r(\mathcal A)δr​(A) (Definition 3.1) is the smallest δ≥0\delta\ge0δ≥0 such that

(1−δ)∥X∥F≤∥A(X)∥≤(1+δ)∥X∥Ffor all X with rank⁡X≤r.(1-\delta)\|X\|_F\le\|\mathcal A(X)\|\le(1+\delta)\|X\|_F\qquad\text{for all }X\text{ with }\operatorname{rank}X\le r.(1−δ)∥X∥F​≤∥A(X)∥≤(1+δ)∥X∥F​for all X with rankX≤r.

A random linear map A\mathcal AA is nearly isometrically distributed (Definition 4.1) if for every XXX, E∥A(X)∥2=∥X∥F2\mathbb E\|\mathcal A(X)\|^2=\|X\|_F^2E∥A(X)∥2=∥X∥F2​; for every X≠0X\ne0X=0 and 0<ϵ<10<\epsilon<10<ϵ<1,

P(∣∥A(X)∥2−∥X∥F2∣≥ϵ∥X∥F2)≤2exp⁡(−p2(ϵ2/2−ϵ3/3));\mathbb P\big(\big|\|\mathcal A(X)\|^2-\|X\|_F^2\big|\ge\epsilon\|X\|_F^2\big)\le2\exp\Big(-\frac p2\big(\epsilon^2/2-\epsilon^3/3\big)\Big);P(​∥A(X)∥2−∥X∥F2​​≥ϵ∥X∥F2​)≤2exp(−2p​(ϵ2/2−ϵ3/3));

and for some γ>0\gamma>0γ>0 and all t>0t>0t>0, P(∥A∥≥1+mn/p+t)≤exp⁡(−γpt2)\mathbb P(\|\mathcal A\|\ge1+\sqrt{mn/p}+t)\le\exp(-\gamma pt^2)P(∥A∥≥1+mn/p​+t)≤exp(−γpt2).

For subspaces T1,T2T_1,T_2T1​,T2​ of a Euclidean space, the projection distance is ρ(T1,T2)=∥PT1−PT2∥\rho(T_1,T_2)=\|P_{T_1}-P_{T_2}\|ρ(T1​,T2​)=∥PT1​​−PT2​​∥, the operator norm of the difference of the orthogonal projections (4.10). For subspaces V⊆RmV\subseteq\mathbb R^mV⊆Rm, W⊆RnW\subseteq\mathbb R^nW⊆Rn, the subspace Σ(V,W)⊆Rm×n\Sigma(V,W)\subseteq\mathbb R^{m\times n}Σ(V,W)⊆Rm×n consists of the matrices whose column space lies in VVV and whose row space lies in WWW.

Formalization targets

Goal: Theorem 4.2

Fix 0<δ<10<\delta<10<δ<1. There are c0,c1>0c_0,c_1>0c0​,c1​>0 depending only on δ\deltaδ such that for all 1≤r≤m≤n1\le r\le m\le n1≤r≤m≤n with mn≥2mn\ge2mn≥2, all p≥c0 r(m+n)log⁡(mn)p\ge c_0\,r(m+n)\log(mn)p≥c0​r(m+n)log(mn), and every nearly isometric random map A:Rm×n→Rp\mathcal A:\mathbb R^{m\times n}\to\mathbb R^pA:Rm×n→Rp,

P(δr(A)>δ)≤e−c1p.\mathbb P\big(\delta_r(\mathcal A)>\delta\big)\le e^{-c_1p}.P(δr​(A)>δ)≤e−c1​p.

Milestones

  • Lemma 4.3. For a fixed subspace UUU with d=dim⁡U≤pd=\dim U\le pd=dimU≤p and 0<δ<10<\delta<10<δ<1, the map is a δ\deltaδ-isometry on all of UUU except with probability at most 2(12/δ)dexp⁡(−p2(δ2/8−δ3/24))2(12/\delta)^d\exp(-\frac p2(\delta^2/8-\delta^3/24))2(12/δ)dexp(−2p​(δ2/8−δ3/24)).
  • Lemma 4.4. If A\mathcal AA is a δ\deltaδ-isometry on a ddd-dimensional U1U_1U1​, it is a δ′\delta'δ′-isometry on any ddd-dimensional U2U_2U2​, with δ′=δ+(1+∥A∥)ρ(U1,U2)\delta'=\delta+(1+\|\mathcal A\|)\rho(U_1,U_2)δ′=δ+(1+∥A∥)ρ(U1​,U2​).
  • (4.17). ρ(Σ(V1,W1),Σ(V2,W2))≤ρ(V1,V2)+ρ(W1,W2)\rho(\Sigma(V_1,W_1),\Sigma(V_2,W_2))\le\rho(V_1,V_2)+\rho(W_1,W_2)ρ(Σ(V1​,W1​),Σ(V2​,W2​))≤ρ(V1​,V2​)+ρ(W1​,W2​).
  • Lemma 4.5. For 0<ϵ≤10<\epsilon\le10<ϵ≤1, the family {Σ(V,W):dim⁡V=dim⁡W=r}\{\Sigma(V,W):\dim V=\dim W=r\}{Σ(V,W):dimV=dimW=r} has an ϵ\epsilonϵ-net in ρ\rhoρ of size at most (2C0/ϵ)r(m+n−2r)(2C_0/\epsilon)^{r(m+n-2r)}(2C0​/ϵ)r(m+n−2r), with C0C_0C0​ absolute.

Significance

The theorem supplies the hypothesis of the paper's recovery theorem for random measurements: with δ=1/10\delta=1/10δ=1/10 and rank 5r5r5r, it shows that O(r(m+n)log⁡(mn))O(r(m+n)\log(mn))O(r(m+n)log(mn)) random linear measurements suffice for nuclear norm minimization to recover every matrix of rank at most rrr exactly. Since a rank-rrr matrix has r(m+n−r)r(m+n-r)r(m+n−r) degrees of freedom, this is within a logarithmic factor of the information-theoretic count. The result made the nuclear norm heuristic a guaranteed method and seeded the theory of low-rank matrix recovery, including matrix completion.

The result is proved in the paper, though Lemma 4.5 rests on Szarek's covering estimates for the Grassmannian, cited without proof. To the best of the curators' search of the platform, none of these statements is machine-checked: there is no formal treatment of the matrix restricted isometry property, of nets on Grassmannians in the projection metric, or of nearly isometric random maps. A formalization would supply the probabilistic half of a fully verified low-rank recovery guarantee, together with reusable pieces — the projection distance, the stability of near isometry under subspace perturbation, and a covering bound for Grassmannians.

Difficulty

The set of matrices of rank at most rrr is not a subspace, so concentration for one matrix and a union bound over a single net in Rm×n\mathbb R^{m\times n}Rm×n do not suffice: a net of the unit ball of all matrices has size exponential in mnmnmn, which would require ppp of order mnmnmn. The set must instead be covered by finitely many r2r^2r2-dimensional subspaces, which requires a quantitative covering of the Grassmannians G(m,r)G(m,r)G(m,r) and G(n,r)G(n,r)G(n,r) in the projection distance — the content of Lemma 4.5, whose source in the literature (Szarek) does not give the constant explicitly. A second subtlety is that the event "A\mathcal AA is a near-isometry on all of a subspace" involves an uncountable family of matrices, and the bound for the supremum of ∥A(X)∥\|\mathcal A(X)\|∥A(X)∥ over a unit sphere has to be controlled from the finitely many points of a net.

Formalization scope

All statements live in the namespace MinRankRecovery.RandomRIP. Matrices are Matrix (Fin m) (Fin n) ℝ; the Frobenius norm and the trace inner product come from the published module HighDimStat_MatrixRank_Core. A linear map is represented by its ppp measurement matrices Xs : Fin p → Matrix (Fin m) (Fin n) ℝ, which loses no generality. A random map is Xs : Ω → Fin p → Matrix … on a probability space (Ω, μ), with measurable entries.

Conventions committed to:

  • δr\delta_rδr​ is the infimum of the admissible δ≥0\delta\ge0δ≥0 and is defined for every rrr; the paper's 1≤r≤m≤n1\le r\le m\le n1≤r≤m≤n appears as hypotheses of the goal.
  • ∥A∥\|\mathcal A\|∥A∥ is a supremum over the nonempty, bounded Frobenius unit ball.
  • (4.1) includes integrability. (4.2) is imposed for X≠0X\ne0X=0 only, since at X=0X=0X=0 the printed inequality fails for large ppp. γ\gammaγ in (4.3) may depend on the distribution and dimensions.
  • Probability statements bound the (outer) measure of the failure event, since events quantified over all matrices need not be measurable.
  • For ρ\rhoρ and Σ(V,W)\Sigma(V,W)Σ(V,W), matrices are vectorized into EuclideanSpace ℝ (Fin m × Fin n), which carries the Frobenius inner product. Lemma 4.4 is stated on EuclideanSpace ℝ ι for any finite index type.
  • Real.log is the natural logarithm.

Two printed statements are corrected. Theorem 4.2 assumes mn≥2mn\ge2mn≥2: at m=n=r=1m=n=r=1m=n=r=1, log⁡(mn)=0\log(mn)=0log(mn)=0 and a two-point random scalar map is nearly isometric while violating the conclusion. Lemma 4.5 is posed for 0<ϵ≤10<\epsilon\le10<ϵ≤1, since for large ϵ\epsilonϵ the right side drops below 111.

The constants c0,c1c_0,c_1c0​,c1​ of the goal are quantified before the dimensions, the distribution and γ\gammaγ; a formalization in which they may depend on m,n,p,rm,n,p,rm,n,p,r or on the distribution, or in which the near-isometry hypothesis is unsatisfiable, would be trivial and is ruled out by these choices.

A complete development needs: orthogonal projections and operator norms on finite-dimensional inner product spaces (Mathlib), volumetric ϵ\epsilonϵ-nets of spheres in subspaces, covering bounds for real Grassmannians in the projection metric, and the measure-theoretic union bound. The Grassmannian covering bound and the stability lemma are reusable beyond this mission. Contributions of any milestone, including Lemma 4.5 on its own, are welcome.

Selected references

  • B. Recht, M. Fazel, P. A. Parrilo, Guaranteed Minimum-Rank Solutions of Linear Matrix Equations via Nuclear Norm Minimization, SIAM Review 52(3):471–501, 2010. Preprint arXiv:0706.4138v1. https://arxiv.org/abs/0706.4138
  • E. J. Candès, T. Tao, Decoding by Linear Programming, IEEE Trans. Inform. Theory 51(12), 2005. https://doi.org/10.1109/TIT.2005.858979
  • R. Baraniuk, M. Davenport, R. DeVore, M. Wakin, A Simple Proof of the Restricted Isometry Property for Random Matrices, Constructive Approximation 28(3), 2008. https://doi.org/10.1007/s00365-007-9003-x
  • S. J. Szarek, Metric entropy of homogeneous spaces, in Quantum Probability, Banach Center Publ. 43, 1998. https://arxiv.org/abs/math/9701213
  • E. J. Candès, Y. Plan, Tight Oracle Inequalities for Low-Rank Matrix Recovery From a Minimal Number of Noisy Random Measurements, IEEE Trans. Inform. Theory 57(4), 2011. https://arxiv.org/abs/1001.0339
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Numerical AnalysisOptimization·Captain: mikedeng1

Projection-like Retractions on Matrix Manifolds IV: Within σ_r(X̄)/2 of a Rank-r Matrix, the Truncated SVD Is the Unique Nearest Matrix of Rank Exactly rResearch Paper

Motivation

Optimization over sets of matrices of fixed rank comes up in low-rank matrix completion, model reduction, and the low-rank approximation of solutions of large matrix equations. A standard approach treats the constraint set as a Riemannian manifold and runs gradient or Newton-type methods on it (Absil, Mahony & Sepulchre 2008). Each iteration takes a step in the tangent space and then has to return to the manifold. A map that does this to first order is called a retraction, and its cost is often what decides whether a manifold method is practical.

Absil and Malick (2012) study retractions defined by projection: step to X+ZX+ZX+Z in the ambient space, then take the nearest point of the manifold. Their Proposition 3.2 shows that for any CkC^kCk submanifold (k≥2k\ge2k≥2) this projective retraction is a retraction. Section 3.2 makes it explicit for the manifold of fixed-rank matrices: near any matrix of rank rrr, the nearest matrix of rank exactly rrr is the truncated singular value decomposition (Proposition 3.3). Section 4.4 also gives a closed form for a second retraction on the same manifold, the orthographic retraction (Proposition 4.11).

Setting

Fix natural numbers nnn, mmm and r≥1r\ge1r≥1. The space Rn×m\mathbb R^{n\times m}Rn×m of real n×mn\times mn×m matrices carries the Frobenius norm ∥X∥2=∑i,jXij2=trace⁡(X⊤X)\|X\|^2=\sum_{i,j}X_{ij}^2=\operatorname{trace}(X^\top X)∥X∥2=∑i,j​Xij2​=trace(X⊤X) (3.6). The fixed-rank set is

Rr={X∈Rn×m: rank⁡(X)=r},\mathcal R_r=\{X\in\mathbb R^{n\times m}:\ \operatorname{rank}(X)=r\},Rr​={X∈Rn×m: rank(X)=r},

a smooth submanifold of Rn×m\mathbb R^{n\times m}Rn×m. It is not closed: its closure is the set of matrices of rank at most rrr.

A singular value decomposition (3.5) of XXX is a factorization X=UΣV⊤X=U\Sigma V^\topX=UΣV⊤ in which U=[u1,…,un]∈Rn×nU=[u_1,\dots,u_n]\in\mathbb R^{n\times n}U=[u1​,…,un​]∈Rn×n and V=[v1,…,vm]∈Rm×mV=[v_1,\dots,v_m]\in\mathbb R^{m\times m}V=[v1​,…,vm​]∈Rm×m are orthogonal and Σ∈Rn×m\Sigma\in\mathbb R^{n\times m}Σ∈Rn×m is zero off its diagonal. The diagonal of Σ\SigmaΣ holds the singular values of XXX in nonincreasing order,

σ1(X)≥σ2(X)≥⋯≥σmin⁡{n,m}(X)≥0,\sigma_1(X)\ge\sigma_2(X)\ge\cdots\ge\sigma_{\min\{n,m\}}(X)\ge0,σ1​(X)≥σ2​(X)≥⋯≥σmin{n,m}​(X)≥0,

and σi(X)=0\sigma_i(X)=0σi​(X)=0 for i>min⁡{n,m}i>\min\{n,m\}i>min{n,m}. A matrix has rank rrr exactly when σr(X)>0=σr+1(X)\sigma_r(X)>0=\sigma_{r+1}(X)σr​(X)>0=σr+1​(X). The truncated SVD of rank rrr is X^=∑i=1rσi(X)uivi⊤\hat X=\sum_{i=1}^r\sigma_i(X)u_iv_i^\topX^=∑i=1r​σi​(X)ui​vi⊤​ (3.7).

For a set QQQ and a point XXX, the projection PQ(X)P_Q(X)PQ​(X) is the set of nearest points: the Y∈QY\in QY∈Q with ∥X−Y∥≤∥X−W∥\|X-Y\|\le\|X-W\|∥X−Y∥≤∥X−W∥ for all W∈QW\in QW∈Q. For a set that is not closed, PQ(X)P_Q(X)PQ​(X) may be empty or contain several points.

Formalization targets

Goal: Proposition 3.3

Let Xˉ∈Rr\bar X\in\mathcal R_rXˉ∈Rr​. For every XXX with ∥X−Xˉ∥<σr(Xˉ)/2\|X-\bar X\|<\sigma_r(\bar X)/2∥X−Xˉ∥<σr​(Xˉ)/2 and every singular value decomposition X=UΣV⊤X=U\Sigma V^\topX=UΣV⊤,

PRr(X)={∑i=1rσi(X) uivi⊤}.P_{\mathcal R_r}(X)=\Bigl\{\sum_{i=1}^r\sigma_i(X)\,u_iv_i^\top\Bigr\}.PRr​​(X)={i=1∑r​σi​(X)ui​vi⊤​}.

The projection exists, is unique, and is the truncated SVD. The radius σr(Xˉ)/2\sigma_r(\bar X)/2σr​(Xˉ)/2 and the strict inequality are those of the paper.

Milestones

The paper's proof goes through four claims, which are the milestones in attack order:

  1. Weyl's bound (§3.2, proof of Proposition 3.3, citing Horn–Johnson 7.3.8): ∣σi(Xˉ)−σi(X)∣≤∥X−Xˉ∥|\sigma_i(\bar X)-\sigma_i(X)|\le\|X-\bar X\|∣σi​(Xˉ)−σi​(X)∣≤∥X−Xˉ∥ for every i≥1i\ge1i≥1.
  2. Eckart–Young (3.7): for every singular value decomposition of XXX, X^\hat XX^ is a nearest matrix to XXX of rank at most rrr.
  3. The gap (3.8): if rank⁡Xˉ=r\operatorname{rank}\bar X=rrankXˉ=r and ∥X−Xˉ∥<σr(Xˉ)/2\|X-\bar X\|<\sigma_r(\bar X)/2∥X−Xˉ∥<σr​(Xˉ)/2, then σr+1(X)<σr(Xˉ)/2<σr(X)\sigma_{r+1}(X)<\sigma_r(\bar X)/2<\sigma_r(X)σr+1​(X)<σr​(Xˉ)/2<σr​(X).
  4. Uniqueness under a gap (§3.2, proof of Proposition 3.3, citing Helmke–Moore): if σr(X)>σr+1(X)\sigma_r(X)>\sigma_{r+1}(X)σr​(X)>σr+1​(X), then X^\hat XX^ is the only nearest matrix of rank at most rrr.

Further result: Proposition 4.11

Write X=U[Σ0000]V⊤X=U\left[\begin{smallmatrix}\Sigma_0&0\\0&0\end{smallmatrix}\right]V^\topX=U[Σ0​0​00​]V⊤ (4.7), with Σ0\Sigma_0Σ0​ the positive diagonal of nonzero singular values, and a tangent vector Z=U[ACB0]V⊤Z=U\left[\begin{smallmatrix}A&C\\B&0\end{smallmatrix}\right]V^\topZ=U[AB​C0​]V⊤ (4.8). If Σ0+A\Sigma_0+AΣ0​+A is invertible, the orthographic retraction is

R(X,Z)=U[Σ0+ACBB(Σ0+A)−1C]V⊤.R(X,Z)=U\begin{bmatrix}\Sigma_0+A&C\\B&B(\Sigma_0+A)^{-1}C\end{bmatrix}V^\top .R(X,Z)=U[Σ0​+AB​CB(Σ0​+A)−1C​]V⊤.

Here R(X,Z)R(X,Z)R(X,Z) is the nearest point to X+ZX+ZX+Z of Rr∩(X+Z+NRr(X))\mathcal R_r\cap(X+Z+N_{\mathcal R_r}(X))Rr​∩(X+Z+NRr​​(X)).

Significance

The result. Proposition 3.3 reduces the projective retraction on Rr\mathcal R_rRr​ to one truncated singular value decomposition. With Proposition 3.2 this gives an explicit, computable retraction for Riemannian optimization on fixed-rank matrices. It is used, for instance, in low-rank matrix completion algorithms. The point is local: Rr\mathcal R_rRr​ is not closed, so far from Rr\mathcal R_rRr​ the nearest matrix of rank exactly rrr need not exist, and the proposition gives an explicit radius on which it does exist and is unique. Proposition 4.11 gives a second retraction that needs only products of matrices and one r×rr\times rr×r inverse.

Formalizing it. All results here are proved, on paper. To the best of a search of Mathlib and the Prove2Me catalog, none is machine-checked. Mathlib has singular values of linear maps between finite-dimensional inner product spaces (LinearMap.singularValues), but no singular value decomposition in matrix form, no Weyl perturbation inequality for singular values, and no Eckart–Young theorem. A complete development would add these, and the Eckart–Young theorem with its uniqueness case is a standard result of numerical linear algebra in its own right.

Difficulty

The proof in the paper is short only because it cites three facts, and each of them is a real piece of matrix analysis.

  • Weyl's bound needs the variational (min–max) description of singular values, which Mathlib does not have for singular values.
  • Eckart–Young requires comparing ∥X−Y∥\|X-Y\|∥X−Y∥ with the singular values of XXX for every YYY of rank at most rrr, not only for those diagonal in the same bases. The obvious approach, writing YYY in the singular bases of XXX, fails because YYY need not be diagonal there.
  • Uniqueness under the gap requires showing that every minimizer is diagonal in some singular bases of XXX and then using the gap to fix its support. Without the gap uniqueness fails: for X=I2X=I_2X=I2​ and r=1r=1r=1 every uu⊤uu^\topuu⊤ with ∥u∥=1\|u\|=1∥u∥=1 is a nearest point.

A further subtlety: Proposition 3.3 must hold for any singular value decomposition of XXX. Singular vectors are not unique, so the proof has to show that the truncation does not depend on the choice under the gap (3.8).

Formalization scope

Matrices are Matrix (Fin n) (Fin m) ℝ with Mathlib's Frobenius norm (open scoped Matrix.Norms.Frobenius). The projection is the published platform predicate RandomGradFree.Nonsmooth.IsMetricProjection, and PRr(X)P_{\mathcal R_r}(X)PRr​​(X) is the set {Y | IsMetricProjection (rankSet r) X Y}. The set equality with a singleton states existence, uniqueness and the formula together.

Conventions committed to:

  • sv X i is σi(X)\sigma_i(X)σi​(X), 1-based as on the page. It is Mathlib's 0-based singularValues of Matrix.toEuclideanLin X at i - 1, so the index 000 is meaningless and every statement uses indices ≥1\ge1≥1.
  • IsSVD X U S V is the predicate of (3.5). The singular value decomposition is a hypothesis of the theorems, never a choice made inside them, so the theorems hold for every singular value decomposition.
  • truncSVD r U S V is ∑i≤rΣiiuivi⊤\sum_{i\le r}\Sigma_{ii}u_iv_i^\top∑i≤r​Σii​ui​vi⊤​, written with the diagonal of S. That these entries are the singular values σi(X)\sigma_i(X)σi​(X) is a fact to be proved, not part of the definition.
  • The hypothesis r≥1r\ge1r≥1 is added, because σr\sigma_rσr​ needs it (and R0={0}\mathcal R_0=\{0\}R0​={0}). It is the only hypothesis of Proposition 3.3 not printed on the page.
  • In Proposition 4.11, matrices use the block index types Fin r ⊕ Fin p and Fin r ⊕ Fin q. The tangent vector and the normal space are taken in the form the page gives, and invertibility of Σ0+A\Sigma_0+AΣ0​+A is an explicit hypothesis. In the paper's proof it comes from "ZZZ in a neighborhood of the origin".

A formalization in which the radius is replaced by a smaller one, the projection is taken onto the matrices of rank at most rrr, or the singular value decomposition is chosen inside the statement is a different theorem and is ruled out.

Wanted contributions, all reusable beyond this mission:

  • existence of a singular value decomposition in matrix form, and the identification of its diagonal with singularValues;
  • Weyl's inequality for singular values;
  • the Eckart–Young theorem and its uniqueness case;
  • the Schur-complement rank formula for 2×22\times22×2 block matrices, used for Proposition 4.11.

Selected references

  • P.-A. Absil and J. Malick, Projection-like retractions on matrix manifolds, SIAM J. Optim. 22(1):135–158, 2012. https://doi.org/10.1137/100802529 (authors' version HAL hal-00651608v2: https://hal.science/hal-00651608v2)
  • P.-A. Absil, R. Mahony and R. Sepulchre, Optimization Algorithms on Matrix Manifolds, Princeton University Press, 2008. https://press.princeton.edu/absil
  • C. Eckart and G. Young, The approximation of one matrix by another of lower rank, Psychometrika 1(3):211–218, 1936. https://doi.org/10.1007/BF02288367
  • R. A. Horn and C. R. Johnson, Matrix Analysis, Cambridge University Press, 1985 (§7.3, §7.4). https://doi.org/10.1017/CBO9780511810817
  • U. Helmke and J. B. Moore, Optimization and Dynamical Systems, Springer, 1994 (Ch. 5). https://doi.org/10.1007/978-1-4471-3467-1
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