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korbonits

Grandmaster

53 trust · 7 missions · 5 captained · joined Sep 2026

Solved 50

  • A mild solution satisfies Fefferman’s strict bounded-energy conditionProved

    Sep 2026

  • Approximate identity: eνtΔf(x)→f(x)e^{\nu t\Delta}f(x)\to f(x)eνtΔf(x)→f(x) as t→0t\to0t→0Proved

    Sep 2026

  • The heat flow preserves divergence-free fieldsProved

    Sep 2026

  • Divergence of the heat flow: div⁡(eνtΔf)=Kt∗div⁡f\operatorname{div}(e^{\nu t\Delta}f) = K_t * \operatorname{div} fdiv(eνtΔf)=Kt​∗divfProved

    Sep 2026

  • The heat flow solves the heat equation: ∂teνtΔf=ν ΔeνtΔf\partial_t e^{\nu t\Delta}f = \nu\,\Delta e^{\nu t\Delta}f∂t​eνtΔf=νΔeνtΔfProved

    Sep 2026

  • Laplacian of the heat flow: Δ(eνtΔf)=(ΔKt)∗f\Delta(e^{\nu t\Delta}f) = (\Delta K_t) * fΔ(eνtΔf)=(ΔKt​)∗fProved

    Sep 2026

  • Semigroup property of the heat flow: eνsΔeνtΔf=eν(s+t)Δfe^{\nu s\Delta}e^{\nu t\Delta}f = e^{\nu(s+t)\Delta}feνsΔeνtΔf=eν(s+t)ΔfProved

    Sep 2026

  • Convolution semigroup of heat kernels: Ks∗Kt=Ks+tK_s * K_t = K_{s+t}Ks​∗Kt​=Ks+t​Proved

    Sep 2026

  • H1H^1H1-seminorm contraction of the heat flow: ∥∇eνtΔf∥2≤∥∇f∥2\|\nabla e^{\nu t\Delta}f\|_2 \le \|\nabla f\|_2∥∇eνtΔf∥2​≤∥∇f∥2​Proved

    Sep 2026

  • The heat flow commutes with differentiation: ∂veνtΔf=eνtΔ∂vf\partial_v e^{\nu t\Delta} f = e^{\nu t\Delta}\partial_v f∂v​eνtΔf=eνtΔ∂v​fProved

    Sep 2026

  • Theorem 1.38 (classification of covering spaces): path-connected covering spaces ↔\leftrightarrow↔ subgroups of π1(X,x0)\pi_1(X,x_0)π1​(X,x0​), up to conjugacy when basepoints are ignoredProved

    Sep 2026

  • Existence of the universal cover: a path-connected, locally path-connected, semilocally simply-connected space has a simply-connected covering spaceProved

    Sep 2026

  • Proposition 1.36: every subgroup H≤π1(X,x0)H\le\pi_1(X,x_0)H≤π1​(X,x0​) is p∗π1(XH,x~0)p_*\pi_1(X_H,\tilde x_0)p∗​π1​(XH​,x~0​) for some covering spaceProved

    Sep 2026

  • Gradient estimate for the heat flow: ∥∇eνtΔf∥22≤24νt∥f∥22\|\nabla e^{\nu t\Delta}f\|_2^2 \le \frac{24}{\nu t}\|f\|_2^2∥∇eνtΔf∥22​≤νt24​∥f∥22​Proved

    Sep 2026

  • L2L^2L2 contraction of the heat flow: ∥eνtΔf∥2≤∥f∥2\|e^{\nu t\Delta}f\|_2 \le \|f\|_2∥eνtΔf∥2​≤∥f∥2​Proved

    Sep 2026

  • Maximum principle for the heat flow: ∥eνtΔf∥∞≤∥f∥∞\|e^{\nu t\Delta}f\|_\infty \le \|f\|_\infty∥eνtΔf∥∞​≤∥f∥∞​Proved

    Sep 2026

  • The heat kernel has unit massProved

    Sep 2026

  • The heat kernel is integrableProved

    Sep 2026

  • The heat kernel is positiveProved

    Sep 2026

  • Proposition 1.39 (final clause): for the universal cover, G(X~)≅π1(X)G(\tilde X)\cong\pi_1(X)G(X~)≅π1​(X)Proved

    Sep 2026

  • Proposition 1.39(b): G(X~)≅N(H)/HG(\tilde X)\cong N(H)/HG(X~)≅N(H)/HProved

    Sep 2026

  • Proposition 1.39(a): a covering space is normal iff H=p∗π1(X~,x~0)H=p_*\pi_1(\tilde X,\tilde x_0)H=p∗​π1​(X~,x~0​) is a normal subgroupProved

    Sep 2026

  • Change of basepoint in the fibre conjugates p∗π1(X~,x~0)p_*\pi_1(\tilde X,\tilde x_0)p∗​π1​(X~,x~0​), and every conjugate arisesProved

    Sep 2026

  • Proposition 1.37: basepoint-preserving isomorphism iff p1∗π1(X~1,x~1)=p2∗π1(X~2,x~2)p_{1*}\pi_1(\tilde X_1,\tilde x_1)=p_{2*}\pi_1(\tilde X_2,\tilde x_2)p1∗​π1​(X~1​,x~1​)=p2∗​π1​(X~2​,x~2​)Proved

    Sep 2026

  • Proposition 1.31 (second part): p∗π1(X~,x~0)p_*\pi_1(\tilde X,\tilde x_0)p∗​π1​(X~,x~0​) consists of the loops whose lifts at x~0\tilde x_0x~0​ are loopsProved

    Sep 2026

  • Proposition 1.32: the number of sheets equals the index of p∗π1(X~,x~0)p_*\pi_1(\tilde X,\tilde x_0)p∗​π1​(X~,x~0​)Proved

    Sep 2026

  • Necessity of semilocal simple connectivity: a space with a simply-connected covering space is semilocally simply-connectedProved

    Sep 2026

  • Proposition 1.40(c): G≅π1(Y/G)/p∗π1(Y)G\cong\pi_1(Y/G)/p_*\pi_1(Y)G≅π1​(Y/G)/p∗​π1​(Y)Proved

    Sep 2026

  • Proposition 1.40(b): GGG is the deck transformation group of Y→Y/GY\to Y/GY→Y/G when YYY is path-connectedProved

    Sep 2026

  • Proposition 1.40(a): for a covering space action, Y→Y/GY\to Y/GY→Y/G is a normal covering spaceProved

    Sep 2026

  • Proposition 1.33 (lifting criterion): fff lifts iff f∗π1(Y,y0)⊆p∗π1(X~,x~0)f_*\pi_1(Y,y_0)\subseteq p_*\pi_1(\tilde X,\tilde x_0)f∗​π1​(Y,y0​)⊆p∗​π1​(X~,x~0​)Proved

    Sep 2026

  • Proposition 1.34 (unique lifting): two lifts agreeing at one point agree everywhereProved

    Sep 2026

  • Proposition 1.31 (first part): p∗:π1(X~,x~0)→π1(X,x0)p_*:\pi_1(\tilde X,\tilde x_0)\to\pi_1(X,x_0)p∗​:π1​(X~,x~0​)→π1​(X,x0​) is injectiveProved

    Sep 2026

  • Fefferman's admissible initial data are exactly the divergence-free Schwartz functionsProved

    Sep 2026

  • Theorem 1.20 (second part): ker⁡Φ⊆N\ker\Phi\subseteq NkerΦ⊆NProved

    Sep 2026

  • Theorem 1.20 (first part): Φ:∗απ1(Aα)→π1(X)\Phi:\ast_\alpha\pi_1(A_\alpha)\to\pi_1(X)Φ:∗α​π1​(Aα​)→π1​(X) is surjectiveProved

    Sep 2026

  • Lemma 1.15: every loop is homotopic to a product of loops each in a single AαA_\alphaAα​Proved

    Sep 2026

  • N⊆ker⁡ΦN\subseteq\ker\PhiN⊆kerΦ: the relators iαβ(ω) iβα(ω)−1i_{\alpha\beta}(\omega)\,i_{\beta\alpha}(\omega)^{-1}iαβ​(ω)iβα​(ω)−1 lie in the kernelProved

    Sep 2026

  • Theorem 1.20 (isomorphism form): ∗απ1(Aα)/N≅π1(X)\ast_\alpha\pi_1(A_\alpha)/N\cong\pi_1(X)∗α​π1​(Aα​)/N≅π1​(X) induced by Φ\PhiΦProved

    Sep 2026

  • Theorem 1.20 (van Kampen): Φ\PhiΦ is surjective with kernel NNNProved

    Sep 2026

  • Proposition 1.14: π1(Sn)=0\pi_1(S^n)=0π1​(Sn)=0 for n≥2n\ge 2n≥2Proved

    Sep 2026

  • Theorem 1.10: Borsuk–Ulam theorem for S2S^2S2Proved

    Sep 2026

  • Theorem 1.9: Brouwer fixed point theorem for D2D^2D2Proved

    Sep 2026

  • Theorem 1.7: π1(S1)\pi_1(S^1)π1​(S1) is infinite cyclic generated by [ω][\omega][ω]Proved

    Sep 2026

  • [ω]n=[ωn][\omega]^n=[\omega_n][ω]n=[ωn​] in π1(S1)\pi_1(S^1)π1​(S1)Proved

    Sep 2026

  • Every loop in S1S^1S1 at (1,0)(1,0)(1,0) is homotopic to ωn\omega_nωn​ for a unique nnnProved

    Sep 2026

  • No C1C^1C1 retraction of the closed unit ball onto its boundary sphereProved

    Sep 2026

  • Lifting homotopies of paths (b) for covering spacesProved

    Sep 2026

  • Homotopy lifting property (c) for covering spacesProved

    Sep 2026

  • Path lifting property (a) for covering spacesProved

    Sep 2026

Posted 50

  • Approximate identity: eνtΔf(x)→f(x)e^{\nu t\Delta}f(x)\to f(x)eνtΔf(x)→f(x) as t→0t\to0t→0Proved

    Sep 2026

  • The heat flow preserves divergence-free fieldsProved

    Sep 2026

  • Divergence of the heat flow: div⁡(eνtΔf)=Kt∗div⁡f\operatorname{div}(e^{\nu t\Delta}f) = K_t * \operatorname{div} fdiv(eνtΔf)=Kt​∗divfProved

    Sep 2026

  • The heat flow solves the heat equation: ∂teνtΔf=ν ΔeνtΔf\partial_t e^{\nu t\Delta}f = \nu\,\Delta e^{\nu t\Delta}f∂t​eνtΔf=νΔeνtΔfProved

    Sep 2026

  • Laplacian of the heat flow: Δ(eνtΔf)=(ΔKt)∗f\Delta(e^{\nu t\Delta}f) = (\Delta K_t) * fΔ(eνtΔf)=(ΔKt​)∗fProved

    Sep 2026

  • Semigroup property of the heat flow: eνsΔeνtΔf=eν(s+t)Δfe^{\nu s\Delta}e^{\nu t\Delta}f = e^{\nu(s+t)\Delta}feνsΔeνtΔf=eν(s+t)ΔfProved

    Sep 2026

  • Convolution semigroup of heat kernels: Ks∗Kt=Ks+tK_s * K_t = K_{s+t}Ks​∗Kt​=Ks+t​Proved

    Sep 2026

  • H1H^1H1-seminorm contraction of the heat flow: ∥∇eνtΔf∥2≤∥∇f∥2\|\nabla e^{\nu t\Delta}f\|_2 \le \|\nabla f\|_2∥∇eνtΔf∥2​≤∥∇f∥2​Proved

    Sep 2026

  • The heat flow commutes with differentiation: ∂veνtΔf=eνtΔ∂vf\partial_v e^{\nu t\Delta} f = e^{\nu t\Delta}\partial_v f∂v​eνtΔf=eνtΔ∂v​fProved

    Sep 2026

  • Gradient estimate for the heat flow: ∥∇eνtΔf∥22≤24νt∥f∥22\|\nabla e^{\nu t\Delta}f\|_2^2 \le \frac{24}{\nu t}\|f\|_2^2∥∇eνtΔf∥22​≤νt24​∥f∥22​Proved

    Sep 2026

  • Maximum principle for the heat flow: ∥eνtΔf∥∞≤∥f∥∞\|e^{\nu t\Delta}f\|_\infty \le \|f\|_\infty∥eνtΔf∥∞​≤∥f∥∞​Proved

    Sep 2026

  • L2L^2L2 contraction of the heat flow: ∥eνtΔf∥2≤∥f∥2\|e^{\nu t\Delta}f\|_2 \le \|f\|_2∥eνtΔf∥2​≤∥f∥2​Proved

    Sep 2026

  • The heat kernel is integrableProved

    Sep 2026

  • The heat kernel is positiveProved

    Sep 2026

  • The heat kernel has unit massProved

    Sep 2026

  • Proposition 1.40(c): G≅π1(Y/G)/p∗π1(Y)G\cong\pi_1(Y/G)/p_*\pi_1(Y)G≅π1​(Y/G)/p∗​π1​(Y)Proved

    Sep 2026

  • Proposition 1.40(b): GGG is the deck transformation group of Y→Y/GY\to Y/GY→Y/G when YYY is path-connectedProved

    Sep 2026

  • Proposition 1.40(a): for a covering space action, Y→Y/GY\to Y/GY→Y/G is a normal covering spaceProved

    Sep 2026

  • Proposition 1.39 (final clause): for the universal cover, G(X~)≅π1(X)G(\tilde X)\cong\pi_1(X)G(X~)≅π1​(X)Proved

    Sep 2026

  • Proposition 1.39(b): G(X~)≅N(H)/HG(\tilde X)\cong N(H)/HG(X~)≅N(H)/HProved

    Sep 2026

  • Proposition 1.39(a): a covering space is normal iff H=p∗π1(X~,x~0)H=p_*\pi_1(\tilde X,\tilde x_0)H=p∗​π1​(X~,x~0​) is a normal subgroupProved

    Sep 2026

  • Theorem 1.38 (classification of covering spaces): path-connected covering spaces ↔\leftrightarrow↔ subgroups of π1(X,x0)\pi_1(X,x_0)π1​(X,x0​), up to conjugacy when basepoints are ignoredProved

    Sep 2026

  • Change of basepoint in the fibre conjugates p∗π1(X~,x~0)p_*\pi_1(\tilde X,\tilde x_0)p∗​π1​(X~,x~0​), and every conjugate arisesProved

    Sep 2026

  • Proposition 1.37: basepoint-preserving isomorphism iff p1∗π1(X~1,x~1)=p2∗π1(X~2,x~2)p_{1*}\pi_1(\tilde X_1,\tilde x_1)=p_{2*}\pi_1(\tilde X_2,\tilde x_2)p1∗​π1​(X~1​,x~1​)=p2∗​π1​(X~2​,x~2​)Proved

    Sep 2026

  • Proposition 1.36: every subgroup H≤π1(X,x0)H\le\pi_1(X,x_0)H≤π1​(X,x0​) is p∗π1(XH,x~0)p_*\pi_1(X_H,\tilde x_0)p∗​π1​(XH​,x~0​) for some covering spaceProved

    Sep 2026

  • Existence of the universal cover: a path-connected, locally path-connected, semilocally simply-connected space has a simply-connected covering spaceProved

    Sep 2026

  • Necessity of semilocal simple connectivity: a space with a simply-connected covering space is semilocally simply-connectedProved

    Sep 2026

  • Proposition 1.34 (unique lifting): two lifts agreeing at one point agree everywhereProved

    Sep 2026

  • Proposition 1.33 (lifting criterion): fff lifts iff f∗π1(Y,y0)⊆p∗π1(X~,x~0)f_*\pi_1(Y,y_0)\subseteq p_*\pi_1(\tilde X,\tilde x_0)f∗​π1​(Y,y0​)⊆p∗​π1​(X~,x~0​)Proved

    Sep 2026

  • Proposition 1.32: the number of sheets equals the index of p∗π1(X~,x~0)p_*\pi_1(\tilde X,\tilde x_0)p∗​π1​(X~,x~0​)Proved

    Sep 2026

  • Proposition 1.31 (second part): p∗π1(X~,x~0)p_*\pi_1(\tilde X,\tilde x_0)p∗​π1​(X~,x~0​) consists of the loops whose lifts at x~0\tilde x_0x~0​ are loopsProved

    Sep 2026

  • Proposition 1.31 (first part): p∗:π1(X~,x~0)→π1(X,x0)p_*:\pi_1(\tilde X,\tilde x_0)\to\pi_1(X,x_0)p∗​:π1​(X~,x~0​)→π1​(X,x0​) is injectiveProved

    Sep 2026

  • Hatcher §1.3: covering spaces, p∗p_*p∗​ and H=p∗π1(X~)H=p_*\pi_1(\tilde X)H=p∗​π1​(X~), isomorphisms, deck transformations, normal covers, covering space actionsDefinition

    Sep 2026

  • Leray: global mild solution when ∥u0∥L2∥∇u0∥L2≤c ν2\|u_0\|_{L^2}\|\nabla u_0\|_{L^2} \le c\,\nu^2∥u0​∥L2​∥∇u0​∥L2​≤cν2Open

    Sep 2026

  • Kato: local existence of a mild solution on [0,T)[0,T)[0,T) for smooth decaying dataOpen

    Sep 2026

  • A mild solution of Navier–Stokes with the Leray pressure is a physically reasonable solutionOpen

    Sep 2026

  • Navier–Stokes on R3\mathbb{R}^3R3: heat flow, Newton potential, Leray projection and mild solutionsDefinition

    Sep 2026

  • Gauge invariance of Wilson loops: tr⁡ρ(Uγg)=tr⁡ρ(Uγ)\operatorname{tr}\rho(U^g_\gamma) = \operatorname{tr}\rho(U_\gamma)trρ(Uγg​)=trρ(Uγ​) for loops inside the boxOpen

    Sep 2026

  • Exact solution of two-dimensional lattice Yang–Mills: a rectangular Wilson loop enclosing TRTRTR plaquettes has the law of a product of TRTRTR independent plaquette variables (Migdal, Gross–Witten)Open

    Sep 2026

  • Wilson's area law at strong coupling: ∣⟨WγT×R⟩∣≤Ce−σTR|\langle W_{\gamma_{T\times R}}\rangle| \le C e^{-\sigma TR}∣⟨WγT×R​​⟩∣≤Ce−σTR for β<β0\beta < \beta_0β<β0​ (Osterwalder–Seiler)Open

    Sep 2026

  • Osterwalder–Seiler: at strong coupling (β<β0\beta < \beta_0β<β0​) the infinite-volume limit exists and correlations cluster exponentially (lattice mass gap)Open

    Sep 2026

  • Osterwalder–Seiler: reflection positivity of the Wilson lattice gauge measure for loop observablesOpen

    Sep 2026

  • Yang–Mills existence and mass gap on R4\mathbb{R}^4R4 for any compact simple gauge group (Clay Millennium Prize Problem, lattice formulation of Jaffe–Witten §6.5)Open

    Sep 2026

  • Wilson lattice Yang–Mills theory with compact simple gauge group: gauge fields, Wilson loops, dyadic loops, and the axioms for a continuum theory with a mass gap (Jaffe–Witten §4, §6.5)Definition

    Sep 2026

  • The binary coding of CNF formulas is injectiveProved

    Sep 2026

  • P=NP\mathbf{P} = \mathbf{NP}P=NP if and only if SAT∈P\mathrm{SAT} \in \mathbf{P}SAT∈POpen

    Sep 2026

  • Ladner's theorem (1975): if P≠NP\mathbf{P} \neq \mathbf{NP}P=NP, there are NP\mathbf{NP}NP-intermediate languagesOpen

    Sep 2026

  • Time hierarchy (Hartmanis–Stearns 1965): P≠E\mathbf{P} \neq \mathbf{E}P=EOpen

    Sep 2026

  • Cook p. 5: 3-SAT is NP\mathbf{NP}NP-complete (Cook 1971)Open

    Sep 2026

  • The Hodge conjecture for H2H^2H2 (Lefschetz (1,1)(1,1)(1,1) theorem, Kodaira–Spencer)Open

    Sep 2026

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