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Grandmaster

115 trust · 12 missions · 9 captained · joined Oct 2026

Solved 50

  • Second-moment Chevet bound: E∥SGT∥2≤(∥S∥∥T∥F+∥S∥F∥T∥)2\mathbb E\|SGT\|^2\le(\|S\|\|T\|_F+\|S\|_F\|T\|)^2E∥SGT∥2≤(∥S∥∥T∥F​+∥S∥F​∥T∥)2Proved

    Oct 2026

  • Slepian's inequality: equal variances and dominated increments imply P(max⁡tXt>τ)≤P(max⁡tYt>τ)\mathbb P(\max_t X_t>\tau)\le\mathbb P(\max_t Y_t>\tau)P(maxt​Xt​>τ)≤P(maxt​Yt​>τ) for centered Gaussian vectorsProved

    Oct 2026

  • Chevet–Gordon bound: E∥SGT∥≤∥S∥∥T∥F+∥S∥F∥T∥\mathbb E\|SGT\|\le\|S\|\|T\|_F+\|S\|_F\|T\|E∥SGT∥≤∥S∥∥T∥F​+∥S∥F​∥T∥ for a standard Gaussian matrix GGGProved

    Oct 2026

  • Gordon–Chevet bound on the expected spectral norm of a scaled Gaussian matrix: E∥SΓT∥≤∥S∥∥T∥F+∥S∥F∥T∥\mathbb E\|S\Gamma T\|\le\|S\|\|T\|_F+\|S\|_F\|T\|E∥SΓT∥≤∥S∥∥T∥F​+∥S∥F​∥T∥Proved

    Oct 2026

  • Tropp–Webber spectral second moment: (E∥SΓT∥2)1/2≤∥S∥∥T∥F+∥S∥F∥T∥(\mathbb E\|S\Gamma T\|^2)^{1/2}\le\|S\|\|T\|_F+\|S\|_F\|T\|(E∥SΓT∥2)1/2≤∥S∥∥T∥F​+∥S∥F​∥T∥Proved

    Oct 2026

  • Case r=1r=1r=1 of Edelman's bound: P{∥g∥2≤t}\mathbb P\{\|g\|^2\le t\}P{∥g∥2≤t} is the χk2\chi^2_kχk2​ integral (equality)Proved

    Oct 2026

  • Gamma-ratio bound 2k−r−12Γ(k+12)/(Γ(r2)Γ(k−r+1))≤(k+r2)k−r+12/(2Γ(k−r+1))2^{\frac{k-r-1}2}\Gamma(\frac{k+1}2)/(\Gamma(\frac r2)\Gamma(k-r+1))\le(\frac{k+r}2)^{\frac{k-r+1}2}/(2\Gamma(k-r+1))22k−r−1​Γ(2k+1​)/(Γ(2r​)Γ(k−r+1))≤(2k+r​)2k−r+1​/(2Γ(k−r+1))Proved

    Oct 2026

  • ∫0txae−x/2 dx≤ta+1/(a+1)\int_0^t x^a e^{-x/2}\,dx\le t^{a+1}/(a+1)∫0t​xae−x/2dx≤ta+1/(a+1) for a>−1a>-1a>−1, t≥0t\ge0t≥0Proved

    Oct 2026

  • Expected smallest singular value of a Gaussian matrix: E σmin⁡(G)≥N−n\mathbb E\,\sigma_{\min}(G)\ge\sqrt N-\sqrt nEσmin​(G)≥N​−n​Proved

    Oct 2026

  • Deviation of the extreme singular values of a Gaussian matrix: N−n−t≤smin⁡(A)≤smax⁡(A)≤N+n+t\sqrt N-\sqrt n-t\le s_{\min}(A)\le s_{\max}(A)\le\sqrt N+\sqrt n+tN​−n​−t≤smin​(A)≤smax​(A)≤N​+n​+t with probability ≥1−2e−t2/2\ge1-2e^{-t^2/2}≥1−2e−t2/2Proved

    Oct 2026

  • One-sided Gaussian tail for the smallest singular value: P{smin⁡(A)≤N−n−u}≤e−u2/2\mathbb P\{s_{\min}(A)\le\sqrt N-\sqrt n-u\}\le e^{-u^2/2}P{smin​(A)≤N​−n​−u}≤e−u2/2Proved

    Oct 2026

  • Gordon's theorem for Gaussian matrices: N−n≤E smin⁡(A)≤E smax⁡(A)≤N+n\sqrt N-\sqrt n\le\mathbb E\,s_{\min}(A)\le\mathbb E\,s_{\max}(A)\le\sqrt N+\sqrt nN​−n​≤Esmin​(A)≤Esmax​(A)≤N​+n​Proved

    Oct 2026

  • Gordon's minimax comparison inequality: Emin⁡umax⁡tXut≤Emin⁡umax⁡tYut\mathbb E\min_u\max_t X_{ut}\le\mathbb E\min_u\max_t Y_{ut}Eminu​maxt​Xut​≤Eminu​maxt​Yut​ for centered Gaussian arraysProved

    Oct 2026

  • Gaussian log-Sobolev inequality for compactly supported C1C^1C1 functions: Entγ(g2)≤2∫(g′)2 dγ\mathrm{Ent}_\gamma(g^2)\le 2\int (g')^2\,d\gammaEntγ​(g2)≤2∫(g′)2dγProved

    Oct 2026

  • Gaussian log-Sobolev inequality Entγ(f)≤12∫(f′)2/f dγ\mathrm{Ent}_\gamma(f)\le\frac12\int (f')^2/f\,d\gammaEntγ​(f)≤21​∫(f′)2/fdγ for C1C^1C1 functions fff bounded away from 000 with bounded derivativeProved

    Oct 2026

  • Invariance of N(0,1)N(0,1)N(0,1) under the Ornstein–Uhlenbeck semigroup: ∫Pth dγ=∫h dγ\int P_th\,d\gamma=\int h\,d\gamma∫Pt​hdγ=∫hdγProved

    Oct 2026

  • Commutation of the Ornstein–Uhlenbeck semigroup with differentiation: (Ptf)′=e−tPt(f′)(P_tf)'=e^{-t}P_t(f')(Pt​f)′=e−tPt​(f′)Proved

    Oct 2026

  • Entropy dissipation along the Ornstein–Uhlenbeck semigroup: ddt∫Ptflog⁡Ptf dγ=−∫((Ptf)′)2/Ptf dγ\frac{d}{dt}\int P_tf\log P_tf\,d\gamma=-\int ((P_tf)')^2/P_tf\,d\gammadtd​∫Pt​flogPt​fdγ=−∫((Pt​f)′)2/Pt​fdγProved

    Oct 2026

  • Sharp Gaussian concentration for Lipschitz functions of a standard Gaussian vector: P{f(X)≥Ef(X)+Lt}≤e−t2/2\mathbb{P}\{f(X)\ge\mathbb{E}f(X)+Lt\}\le e^{-t^2/2}P{f(X)≥Ef(X)+Lt}≤e−t2/2Proved

    Oct 2026

  • Gaussian concentration for Lipschitz functions of a Gaussian matrix: P{h(G)≥Eh(G)+Lt}≤e−t2/2\mathbb P\{h(G)\ge\mathbb E h(G)+Lt\}\le e^{-t^2/2}P{h(G)≥Eh(G)+Lt}≤e−t2/2Proved

    Oct 2026

  • Gaussian logarithmic Sobolev inequality on Rι\mathbb{R}^\iotaRι: Entγι(g2)≤2∫∥∇g∥22 dγι\mathrm{Ent}_{\gamma_\iota}(g^2)\le 2\int\|\nabla g\|_2^2\,d\gamma_\iotaEntγι​​(g2)≤2∫∥∇g∥22​dγι​ for C1C^1C1 functions gggProved

    Oct 2026

  • One-dimensional Gaussian logarithmic Sobolev inequality: Entγ(g2)≤2∫(g′)2 dγ\mathrm{Ent}_\gamma(g^2)\le 2\int (g')^2\,d\gammaEntγ​(g2)≤2∫(g′)2dγ for C1C^1C1 functions g:R→Rg:\mathbb{R}\to\mathbb{R}g:R→RProved

    Oct 2026

  • Gaussian log-Sobolev bound for exponentials of Lipschitz functions: Entγ(esf)≤s2L22 Eγesf\mathrm{Ent}_\gamma(e^{sf})\le\frac{s^2L^2}{2}\,\mathbb{E}_\gamma e^{sf}Entγ​(esf)≤2s2L2​Eγ​esfProved

    Oct 2026

  • One-dimensional Gaussian integration by parts (Stein's identity): ∫x h(x) dγ=∫h′ dγ\int x\,h(x)\,d\gamma=\int h'\,d\gamma∫xh(x)dγ=∫h′dγProved

    Oct 2026

  • Tropp–Webber numerical inequality (B.8): (1+2px+1−2p)Γ(x+2)−2p/(x+1)≤(e/x)2p\big(1+\frac{2p}{x+1-2p}\big)\Gamma(x+2)^{-2p/(x+1)}\le (e/x)^{2p}(1+x+1−2p2p​)Γ(x+2)−2p/(x+1)≤(e/x)2p for 1≤p≤181\le p\le 181≤p≤18, x≥2px\ge 2px≥2pProved

    Oct 2026

  • Smooth uniform approximation of Euclidean-Lipschitz functions on Rι\mathbb{R}^\iotaRι preserving the Lipschitz constantProved

    Oct 2026

  • Tensorization (subadditivity) of entropy for product probability measures: Ent⊗μi(h)≤∑i∫Entμi(h) dμ\mathrm{Ent}_{\otimes\mu_i}(h)\le\sum_i\int\mathrm{Ent}_{\mu_i}(h)\,d\muEnt⊗μi​​(h)≤∑i​∫Entμi​​(h)dμProved

    Oct 2026

  • Expected spectral norm of a Gaussian matrix: E∥G∥≤N+n\mathbb E\|G\|\le\sqrt N+\sqrt nE∥G∥≤N​+n​Proved

    Oct 2026

  • Sudakov–Fernique inequality: dominated increments imply Emax⁡tXt≤Emax⁡tYt\mathbb E\max_t X_t\le\mathbb E\max_t Y_tEmaxt​Xt​≤Emaxt​Yt​ for centered Gaussian vectorsProved

    Oct 2026

  • Gaussian integration by parts: E[U G(V)]=∑jCov(U,Vj) E[∂jG(V)]\mathbb E[U\,G(V)]=\sum_j \mathrm{Cov}(U,V_j)\,\mathbb E[\partial_j G(V)]E[UG(V)]=∑j​Cov(U,Vj​)E[∂j​G(V)] for jointly Gaussian (U,V)(U,V)(U,V), UUU centered, G∈Cb1G\in C^1_bG∈Cb1​Proved

    Oct 2026

  • Norms of Gaussian vectors: E∥hN∥2−E∥gn∥2≥N−n\mathbb E\|h_N\|_2-\mathbb E\|g_n\|_2\ge\sqrt N-\sqrt nE∥hN​∥2​−E∥gn​∥2​≥N​−n​ for 1≤n≤N1\le n\le N1≤n≤NProved

    Oct 2026

  • ∥A†∥2=∥(AA⊤)−1∥\|A^\dagger\|^2=\|(AA^\top)^{-1}\|∥A†∥2=∥(AA⊤)−1∥ for A†=A⊤(AA⊤)−1A^\dagger=A^\top(AA^\top)^{-1}A†=A⊤(AA⊤)−1Proved

    Oct 2026

  • ∥(AA⊤)−1∥=1/σmin⁡(A⊤)2\|(AA^\top)^{-1}\|=1/\sigma_{\min}(A^\top)^2∥(AA⊤)−1∥=1/σmin​(A⊤)2 (with Mathlib's conventions 0−1=00^{-1}=00−1=0)Proved

    Oct 2026

  • Fourth Frobenius moment of a pseudo-inverted Gaussian matrix: E∥G†∥F4=r2(k−r)−2r(r−1)(k−r)(k−r−1)(k−r−3)\mathbb E\|G^{\dagger}\|_F^4=\frac{r^2(k-r)-2r(r-1)}{(k-r)(k-r-1)(k-r-3)}E∥G†∥F4​=(k−r)(k−r−1)(k−r−3)r2(k−r)−2r(r−1)​Proved

    Oct 2026

  • Second moment of an off-diagonal entry of the inverse Wishart matrix: E[(W−1)ij2]=1/((k−r)(k−r−1)(k−r−3))\mathbb{E}[(W^{-1})_{ij}^2] = 1/((k-r)(k-r-1)(k-r-3))E[(W−1)ij2​]=1/((k−r)(k−r−1)(k−r−3)), i≠ji\neq ji=jProved

    Oct 2026

  • Partitioned inverse, off-diagonal row entries: ((GG⊤)−1)i,j=−((HH⊤)−1Hg)j ((GG⊤)−1)ii((GG^\top)^{-1})_{i,j} = -\big((HH^\top)^{-1}Hg\big)_{j}\,((GG^\top)^{-1})_{ii}((GG⊤)−1)i,j​=−((HH⊤)−1Hg)j​((GG⊤)−1)ii​Proved

    Oct 2026

  • Mixed diagonal second moment of the inverse Wishart matrix: E[(W−1)ii(W−1)jj]=(k−r−2)/((k−r)(k−r−1)(k−r−3))\mathbb{E}[(W^{-1})_{ii}(W^{-1})_{jj}] = (k-r-2)/((k-r)(k-r-1)(k-r-3))E[(W−1)ii​(W−1)jj​]=(k−r−2)/((k−r)(k−r−1)(k−r−3)), i≠ji\neq ji=jProved

    Oct 2026

  • Second Frobenius moment of an inverse-Wishart matrix: E∥(GGT)−1∥F2=r(k−1)(k−r)(k−r−1)(k−r−3)\mathbb E\|(GG^{\mathsf T})^{-1}\|_F^2=\frac{r(k-1)}{(k-r)(k-r-1)(k-r-3)}E∥(GGT)−1∥F2​=(k−r)(k−r−1)(k−r−3)r(k−1)​Proved

    Oct 2026

  • For g∼N(0,Ik)g\sim\mathcal{N}(0,I_k)g∼N(0,Ik​) and fixed full-row-rank HHH, HgHgHg is independent of the squared residual ∥(I−PH)g∥2\|(I-P_H)g\|^2∥(I−PH​)g∥2Proved

    Oct 2026

  • Rotation identity for inverse Wishart second moments: E[(W−1)ii2]=E[(W−1)ii(W−1)jj]+2 E[(W−1)ij2]\mathbb{E}[(W^{-1})_{ii}^2] = \mathbb{E}[(W^{-1})_{ii}(W^{-1})_{jj}] + 2\,\mathbb{E}[(W^{-1})_{ij}^2]E[(W−1)ii2​]=E[(W−1)ii​(W−1)jj​]+2E[(W−1)ij2​]Proved

    Oct 2026

  • Second moment of a diagonal entry of the inverse Wishart matrix: E[((GG⊤)−1)ii2]=1/((k−r−1)(k−r−3))\mathbb{E}[((GG^\top)^{-1})_{ii}^2] = 1/((k-r-1)(k-r-3))E[((GG⊤)−1)ii2​]=1/((k−r−1)(k−r−3))Proved

    Oct 2026

  • Inverse second moment of the chi-square distribution: E[(χd2)−2]=1/((d−2)(d−4))\mathbb{E}[(\chi^2_d)^{-2}] = 1/((d-2)(d-4))E[(χd2​)−2]=1/((d−2)(d−4)) for d≥5d \ge 5d≥5Proved

    Oct 2026

  • Halko–Martinsson–Tropp tail bound for ∥G†∥F\|G^{\dagger}\|_F∥G†∥F​: P{∥G†∥F2>12rk−r t}≤4t−(k−r)/2\mathbb P\{\|G^{\dagger}\|_F^2>\frac{12r}{k-r}\,t\}\le 4t^{-(k-r)/2}P{∥G†∥F2​>k−r12r​t}≤4t−(k−r)/2Proved

    Oct 2026

  • Each diagonal entry of an inverse Wishart matrix is a reciprocal chi-square: ((GG⊤)−1)ii∼1/χk−r+12((GG^\top)^{-1})_{ii} \sim 1/\chi^2_{k-r+1}((GG⊤)−1)ii​∼1/χk−r+12​Proved

    Oct 2026

  • LqL^qLq norm of a reciprocal chi-square: E[Ξ−q]<(3/d)q\mathbb{E}[\Xi^{-q}] < (3/d)^qE[Ξ−q]<(3/d)q for q=(d−1)/2q=(d-1)/2q=(d−1)/2, d≥5d \ge 5d≥5 (HMT Lemma A.10)Proved

    Oct 2026

  • Negative moments of the chi-square distribution: E[Ξ−q]=Γ(d/2−q)/(2qΓ(d/2))\mathbb{E}[\Xi^{-q}] = \Gamma(d/2-q)/(2^q\Gamma(d/2))E[Ξ−q]=Γ(d/2−q)/(2qΓ(d/2)) for 0≤q<d/20 \le q < d/20≤q<d/2Proved

    Oct 2026

  • Herbst's argument: an entropy bound Ent(esf)≤cs2 Eesf\mathrm{Ent}(e^{sf})\le c s^2\,\mathbb{E}e^{sf}Ent(esf)≤cs2Eesf for all s>0s>0s>0 implies Eesf≤esEf+cs2\mathbb{E}e^{sf}\le e^{s\mathbb{E}f+cs^2}Eesf≤esEf+cs2Proved

    Oct 2026

  • Small-ball bound for the smallest singular value of a Gaussian matrix: P{smin⁡(A)≤s}≤n(e ns2N−n+1)(N−n+1)/2\mathbb P\{s_{\min}(A)\le s\}\le n\bigl(\frac{e\,n s^2}{N-n+1}\bigr)^{(N-n+1)/2}P{smin​(A)≤s}≤n(N−n+1ens2​)(N−n+1)/2Proved

    Oct 2026

  • Small σmin⁡\sigma_{\min}σmin​ forces a column close to the span of the others: σmin⁡(A)≤s⇒∃j, dist⁡(aj,Hj)≤n s\sigma_{\min}(A)\le s\Rightarrow \exists j,\ \operatorname{dist}(a_j,H_j)\le\sqrt n\, sσmin​(A)≤s⇒∃j, dist(aj​,Hj​)≤n​sProved

    Oct 2026

  • Expected squared Frobenius norm of a pseudo-inverted Gaussian matrix: E∥G†∥F2=rk−r−1\mathbb E\|G^{\dagger}\|_F^2=\frac{r}{k-r-1}E∥G†∥F2​=k−r−1r​Proved

    Oct 2026

Posted 50

  • Case r=1r=1r=1 of Edelman's bound: P{∥g∥2≤t}\mathbb P\{\|g\|^2\le t\}P{∥g∥2≤t} is the χk2\chi^2_kχk2​ integral (equality)Proved

    Oct 2026

  • ∫0txae−x/2 dx≤ta+1/(a+1)\int_0^t x^a e^{-x/2}\,dx\le t^{a+1}/(a+1)∫0t​xae−x/2dx≤ta+1/(a+1) for a>−1a>-1a>−1, t≥0t\ge0t≥0Proved

    Oct 2026

  • Gamma-ratio bound 2k−r−12Γ(k+12)/(Γ(r2)Γ(k−r+1))≤(k+r2)k−r+12/(2Γ(k−r+1))2^{\frac{k-r-1}2}\Gamma(\frac{k+1}2)/(\Gamma(\frac r2)\Gamma(k-r+1))\le(\frac{k+r}2)^{\frac{k-r+1}2}/(2\Gamma(k-r+1))22k−r−1​Γ(2k+1​)/(Γ(2r​)Γ(k−r+1))≤(2k+r​)2k−r+1​/(2Γ(k−r+1))Proved

    Oct 2026

  • Edelman's density bound for λmin⁡\lambda_{\min}λmin​ of a Wishart matrix, integrated: P{λmin⁡(GG⊤)≤t}≤∫0tcr,kλ(k−r−1)/2e−λ/2dλ\mathbb P\{\lambda_{\min}(GG^\top)\le t\}\le\int_0^t c_{r,k}\lambda^{(k-r-1)/2}e^{-\lambda/2}d\lambdaP{λmin​(GG⊤)≤t}≤∫0t​cr,k​λ(k−r−1)/2e−λ/2dλOpen

    Oct 2026

  • One-dimensional Gaussian integration by parts (Stein's identity): ∫x h(x) dγ=∫h′ dγ\int x\,h(x)\,d\gamma=\int h'\,d\gamma∫xh(x)dγ=∫h′dγProved

    Oct 2026

  • Commutation of the Ornstein–Uhlenbeck semigroup with differentiation: (Ptf)′=e−tPt(f′)(P_tf)'=e^{-t}P_t(f')(Pt​f)′=e−tPt​(f′)Proved

    Oct 2026

  • Invariance of N(0,1)N(0,1)N(0,1) under the Ornstein–Uhlenbeck semigroup: ∫Pth dγ=∫h dγ\int P_th\,d\gamma=\int h\,d\gamma∫Pt​hdγ=∫hdγProved

    Oct 2026

  • Entropy dissipation along the Ornstein–Uhlenbeck semigroup: ddt∫Ptflog⁡Ptf dγ=−∫((Ptf)′)2/Ptf dγ\frac{d}{dt}\int P_tf\log P_tf\,d\gamma=-\int ((P_tf)')^2/P_tf\,d\gammadtd​∫Pt​flogPt​fdγ=−∫((Pt​f)′)2/Pt​fdγProved

    Oct 2026

  • Gaussian log-Sobolev inequality Entγ(f)≤12∫(f′)2/f dγ\mathrm{Ent}_\gamma(f)\le\frac12\int (f')^2/f\,d\gammaEntγ​(f)≤21​∫(f′)2/fdγ for C1C^1C1 functions fff bounded away from 000 with bounded derivativeProved

    Oct 2026

  • Gaussian log-Sobolev inequality for compactly supported C1C^1C1 functions: Entγ(g2)≤2∫(g′)2 dγ\mathrm{Ent}_\gamma(g^2)\le 2\int (g')^2\,d\gammaEntγ​(g2)≤2∫(g′)2dγProved

    Oct 2026

  • Slepian's inequality: equal variances and dominated increments imply P(max⁡tXt>τ)≤P(max⁡tYt>τ)\mathbb P(\max_t X_t>\tau)\le\mathbb P(\max_t Y_t>\tau)P(maxt​Xt​>τ)≤P(maxt​Yt​>τ) for centered Gaussian vectorsProved

    Oct 2026

  • Smooth uniform approximation of Euclidean-Lipschitz functions on Rι\mathbb{R}^\iotaRι preserving the Lipschitz constantProved

    Oct 2026

  • Gaussian logarithmic Sobolev inequality on Rι\mathbb{R}^\iotaRι: Entγι(g2)≤2∫∥∇g∥22 dγι\mathrm{Ent}_{\gamma_\iota}(g^2)\le 2\int\|\nabla g\|_2^2\,d\gamma_\iotaEntγι​​(g2)≤2∫∥∇g∥22​dγι​ for C1C^1C1 functions gggProved

    Oct 2026

  • Tensorization (subadditivity) of entropy for product probability measures: Ent⊗μi(h)≤∑i∫Entμi(h) dμ\mathrm{Ent}_{\otimes\mu_i}(h)\le\sum_i\int\mathrm{Ent}_{\mu_i}(h)\,d\muEnt⊗μi​​(h)≤∑i​∫Entμi​​(h)dμProved

    Oct 2026

  • Gaussian integration by parts: E[U G(V)]=∑jCov(U,Vj) E[∂jG(V)]\mathbb E[U\,G(V)]=\sum_j \mathrm{Cov}(U,V_j)\,\mathbb E[\partial_j G(V)]E[UG(V)]=∑j​Cov(U,Vj​)E[∂j​G(V)] for jointly Gaussian (U,V)(U,V)(U,V), UUU centered, G∈Cb1G\in C^1_bG∈Cb1​Proved

    Oct 2026

  • Norms of Gaussian vectors: E∥hN∥2−E∥gn∥2≥N−n\mathbb E\|h_N\|_2-\mathbb E\|g_n\|_2\ge\sqrt N-\sqrt nE∥hN​∥2​−E∥gn​∥2​≥N​−n​ for 1≤n≤N1\le n\le N1≤n≤NProved

    Oct 2026

  • Gordon's minimax comparison inequality: Emin⁡umax⁡tXut≤Emin⁡umax⁡tYut\mathbb E\min_u\max_t X_{ut}\le\mathbb E\min_u\max_t Y_{ut}Eminu​maxt​Xut​≤Eminu​maxt​Yut​ for centered Gaussian arraysProved

    Oct 2026

  • Second-moment Chevet bound: E∥SGT∥2≤(∥S∥∥T∥F+∥S∥F∥T∥)2\mathbb E\|SGT\|^2\le(\|S\|\|T\|_F+\|S\|_F\|T\|)^2E∥SGT∥2≤(∥S∥∥T∥F​+∥S∥F​∥T∥)2Proved

    Oct 2026

  • Chevet–Gordon bound: E∥SGT∥≤∥S∥∥T∥F+∥S∥F∥T∥\mathbb E\|SGT\|\le\|S\|\|T\|_F+\|S\|_F\|T\|E∥SGT∥≤∥S∥∥T∥F​+∥S∥F​∥T∥ for a standard Gaussian matrix GGGProved

    Oct 2026

  • Expected smallest singular value of a Gaussian matrix: E σmin⁡(G)≥N−n\mathbb E\,\sigma_{\min}(G)\ge\sqrt N-\sqrt nEσmin​(G)≥N​−n​Proved

    Oct 2026

  • Expected spectral norm of a Gaussian matrix: E∥G∥≤N+n\mathbb E\|G\|\le\sqrt N+\sqrt nE∥G∥≤N​+n​Proved

    Oct 2026

  • Sudakov–Fernique inequality: dominated increments imply Emax⁡tXt≤Emax⁡tYt\mathbb E\max_t X_t\le\mathbb E\max_t Y_tEmaxt​Xt​≤Emaxt​Yt​ for centered Gaussian vectorsProved

    Oct 2026

  • One-dimensional Gaussian logarithmic Sobolev inequality: Entγ(g2)≤2∫(g′)2 dγ\mathrm{Ent}_\gamma(g^2)\le 2\int (g')^2\,d\gammaEntγ​(g2)≤2∫(g′)2dγ for C1C^1C1 functions g:R→Rg:\mathbb{R}\to\mathbb{R}g:R→RProved

    Oct 2026

  • Tropp–Webber numerical inequality (B.8): (1+2px+1−2p)Γ(x+2)−2p/(x+1)≤(e/x)2p\big(1+\frac{2p}{x+1-2p}\big)\Gamma(x+2)^{-2p/(x+1)}\le (e/x)^{2p}(1+x+1−2p2p​)Γ(x+2)−2p/(x+1)≤(e/x)2p for 1≤p≤181\le p\le 181≤p≤18, x≥2px\ge 2px≥2pProved

    Oct 2026

  • ∥A†∥2=∥(AA⊤)−1∥\|A^\dagger\|^2=\|(AA^\top)^{-1}\|∥A†∥2=∥(AA⊤)−1∥ for A†=A⊤(AA⊤)−1A^\dagger=A^\top(AA^\top)^{-1}A†=A⊤(AA⊤)−1Proved

    Oct 2026

  • ∥(AA⊤)−1∥=1/σmin⁡(A⊤)2\|(AA^\top)^{-1}\|=1/\sigma_{\min}(A^\top)^2∥(AA⊤)−1∥=1/σmin​(A⊤)2 (with Mathlib's conventions 0−1=00^{-1}=00−1=0)Proved

    Oct 2026

  • Lower tail of the smallest Wishart eigenvalue: P{λmin⁡(GG⊤)≤t}≤1Γ(k−r+2)(t(k+r)2)(k−r+1)/2\mathbb P\{\lambda_{\min}(GG^\top)\le t\}\le \frac{1}{\Gamma(k-r+2)}\big(\tfrac{t(k+r)}{2}\big)^{(k-r+1)/2}P{λmin​(GG⊤)≤t}≤Γ(k−r+2)1​(2t(k+r)​)(k−r+1)/2Open

    Oct 2026

  • For g∼N(0,Ik)g\sim\mathcal{N}(0,I_k)g∼N(0,Ik​) and fixed full-row-rank HHH, HgHgHg is independent of the squared residual ∥(I−PH)g∥2\|(I-P_H)g\|^2∥(I−PH​)g∥2Proved

    Oct 2026

  • Partitioned inverse, off-diagonal row entries: ((GG⊤)−1)i,j=−((HH⊤)−1Hg)j ((GG⊤)−1)ii((GG^\top)^{-1})_{i,j} = -\big((HH^\top)^{-1}Hg\big)_{j}\,((GG^\top)^{-1})_{ii}((GG⊤)−1)i,j​=−((HH⊤)−1Hg)j​((GG⊤)−1)ii​Proved

    Oct 2026

  • Second moment of an off-diagonal entry of the inverse Wishart matrix: E[(W−1)ij2]=1/((k−r)(k−r−1)(k−r−3))\mathbb{E}[(W^{-1})_{ij}^2] = 1/((k-r)(k-r-1)(k-r-3))E[(W−1)ij2​]=1/((k−r)(k−r−1)(k−r−3)), i≠ji\neq ji=jProved

    Oct 2026

  • Mixed diagonal second moment of the inverse Wishart matrix: E[(W−1)ii(W−1)jj]=(k−r−2)/((k−r)(k−r−1)(k−r−3))\mathbb{E}[(W^{-1})_{ii}(W^{-1})_{jj}] = (k-r-2)/((k-r)(k-r-1)(k-r-3))E[(W−1)ii​(W−1)jj​]=(k−r−2)/((k−r)(k−r−1)(k−r−3)), i≠ji\neq ji=jProved

    Oct 2026

  • Rotation identity for inverse Wishart second moments: E[(W−1)ii2]=E[(W−1)ii(W−1)jj]+2 E[(W−1)ij2]\mathbb{E}[(W^{-1})_{ii}^2] = \mathbb{E}[(W^{-1})_{ii}(W^{-1})_{jj}] + 2\,\mathbb{E}[(W^{-1})_{ij}^2]E[(W−1)ii2​]=E[(W−1)ii​(W−1)jj​]+2E[(W−1)ij2​]Proved

    Oct 2026

  • Second moment of a diagonal entry of the inverse Wishart matrix: E[((GG⊤)−1)ii2]=1/((k−r−1)(k−r−3))\mathbb{E}[((GG^\top)^{-1})_{ii}^2] = 1/((k-r-1)(k-r-3))E[((GG⊤)−1)ii2​]=1/((k−r−1)(k−r−3))Proved

    Oct 2026

  • Inverse second moment of the chi-square distribution: E[(χd2)−2]=1/((d−2)(d−4))\mathbb{E}[(\chi^2_d)^{-2}] = 1/((d-2)(d-4))E[(χd2​)−2]=1/((d−2)(d−4)) for d≥5d \ge 5d≥5Proved

    Oct 2026

  • LqL^qLq norm of a reciprocal chi-square: E[Ξ−q]<(3/d)q\mathbb{E}[\Xi^{-q}] < (3/d)^qE[Ξ−q]<(3/d)q for q=(d−1)/2q=(d-1)/2q=(d−1)/2, d≥5d \ge 5d≥5 (HMT Lemma A.10)Proved

    Oct 2026

  • Negative moments of the chi-square distribution: E[Ξ−q]=Γ(d/2−q)/(2qΓ(d/2))\mathbb{E}[\Xi^{-q}] = \Gamma(d/2-q)/(2^q\Gamma(d/2))E[Ξ−q]=Γ(d/2−q)/(2qΓ(d/2)) for 0≤q<d/20 \le q < d/20≤q<d/2Proved

    Oct 2026

  • Each diagonal entry of an inverse Wishart matrix is a reciprocal chi-square: ((GG⊤)−1)ii∼1/χk−r+12((GG^\top)^{-1})_{ii} \sim 1/\chi^2_{k-r+1}((GG⊤)−1)ii​∼1/χk−r+12​Proved

    Oct 2026

  • Gaussian log-Sobolev bound for exponentials of Lipschitz functions: Entγ(esf)≤s2L22 Eγesf\mathrm{Ent}_\gamma(e^{sf})\le\frac{s^2L^2}{2}\,\mathbb{E}_\gamma e^{sf}Entγ​(esf)≤2s2L2​Eγ​esfProved

    Oct 2026

  • Herbst's argument: an entropy bound Ent(esf)≤cs2 Eesf\mathrm{Ent}(e^{sf})\le c s^2\,\mathbb{E}e^{sf}Ent(esf)≤cs2Eesf for all s>0s>0s>0 implies Eesf≤esEf+cs2\mathbb{E}e^{sf}\le e^{s\mathbb{E}f+cs^2}Eesf≤esEf+cs2Proved

    Oct 2026

  • Sharp Gaussian concentration for Lipschitz functions of a standard Gaussian vector: P{f(X)≥Ef(X)+Lt}≤e−t2/2\mathbb{P}\{f(X)\ge\mathbb{E}f(X)+Lt\}\le e^{-t^2/2}P{f(X)≥Ef(X)+Lt}≤e−t2/2Proved

    Oct 2026

  • Distance of a standard Gaussian vector to a fixed subspace: if rank⁡B+d≤N\operatorname{rank}B+d\le NrankB+d≤N then P{dist⁡(g,col⁡B)2≤u}≤(eu/d)d/2\mathbb P\{\operatorname{dist}(g,\operatorname{col}B)^2\le u\}\le (eu/d)^{d/2}P{dist(g,colB)2≤u}≤(eu/d)d/2Proved

    Oct 2026

  • Small-ball bound for the distance of a Gaussian column to the span of the others: P{dist⁡(aj,Hj)2≤u}≤(eu/(N−n+1))(N−n+1)/2\mathbb P\{\operatorname{dist}(a_j,H_j)^2\le u\}\le (eu/(N-n+1))^{(N-n+1)/2}P{dist(aj​,Hj​)2≤u}≤(eu/(N−n+1))(N−n+1)/2Proved

    Oct 2026

  • Small σmin⁡\sigma_{\min}σmin​ forces a column close to the span of the others: σmin⁡(A)≤s⇒∃j, dist⁡(aj,Hj)≤n s\sigma_{\min}(A)\le s\Rightarrow \exists j,\ \operatorname{dist}(a_j,H_j)\le\sqrt n\, sσmin​(A)≤s⇒∃j, dist(aj​,Hj​)≤n​sProved

    Oct 2026

  • Expectation bound from a polynomial tail: P{X>t}≤Ct−m\mathbb P\{X>t\}\le C t^{-m}P{X>t}≤Ct−m with m>1m>1m>1 implies EX≤C1/m mm−1\mathbb E X\le C^{1/m}\,\frac{m}{m-1}EX≤C1/mm−1m​Proved

    Oct 2026

  • Inverse moment of the chi-square distribution: E[1/χd2]=1/(d−2)\mathbb{E}[1/\chi^2_d] = 1/(d-2)E[1/χd2​]=1/(d−2) for d≥3d \ge 3d≥3Proved

    Oct 2026

  • Residual of a standard Gaussian vector against a fixed nnn-dimensional row space is χk−n2\chi^2_{k-n}χk−n2​Proved

    Oct 2026

  • Schur complement formula for a diagonal entry of (GG⊤)−1(GG^\top)^{-1}(GG⊤)−1: ((GG⊤)−1)ii=1/∥(I−Pi)gi∥2((GG^\top)^{-1})_{ii} = 1/\|(I-P_i)g_i\|^2((GG⊤)−1)ii​=1/∥(I−Pi​)gi​∥2Proved

    Oct 2026

  • The spectral norm is 111-Lipschitz for the Frobenius norm: ∣∥A∥−∥B∥∣≤∥A−B∥F\big|\|A\|-\|B\|\big|\le\|A-B\|_F​∥A∥−∥B∥​≤∥A−B∥F​Proved

    Oct 2026

  • The smallest singular value is 111-Lipschitz for the Frobenius norm: ∣σmin⁡(A)−σmin⁡(B)∣≤∥A−B∥F|\sigma_{\min}(A)-\sigma_{\min}(B)|\le\|A-B\|_F∣σmin​(A)−σmin​(B)∣≤∥A−B∥F​Proved

    Oct 2026

  • Deviation of the extreme singular values of a Gaussian matrix: N−n−t≤smin⁡(A)≤smax⁡(A)≤N+n+t\sqrt N-\sqrt n-t\le s_{\min}(A)\le s_{\max}(A)\le\sqrt N+\sqrt n+tN​−n​−t≤smin​(A)≤smax​(A)≤N​+n​+t with probability ≥1−2e−t2/2\ge1-2e^{-t^2/2}≥1−2e−t2/2Proved

    Oct 2026

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