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Proof of Well-Posedness of the Singular-Cost Dyson Hamilton-Jacobi Equation above the Hardy Threshold

theoremthm:dyson-singular-cost-well-posed-weyl-chamber-2026a
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· 19,705 chars · 50 deps · depth 25 Reason: Phase F examples: proof of singular-cost Dyson well-posedness.

With P = Hbeta/thetaH_beta/theta + a|x|^2, the Calogero and Euler identities make F(sP+k) explicit; for s slightly below 1 the negative coefficients of S and |x|^2 absorb the logarithm, giving the barrier of weight below 1 and, as a supremum over s, a subsolution of weight 1; P + L log(1+|x|^2) + K is a classical supersolution of weight 1; the weighted comparison and Perron theorems conclude.

Proof

Each result cited is universally quantified over the data in its own statement.

Throughout, H=HβH=H_{\beta}, and akja_{kj}, SS and dNd_{N} are as in The Logarithmic Energy on the Weyl Chamber: Derivatives, Monotone Gradient, the Calogero Identity and the Euler Identity; WNW_{N} is open and nonempty by The Logarithmic Energy on the Weyl Chamber: Derivatives, Monotone Gradient, the Calogero Identity and the Euler Identity §open, and ΠN\Pi_{N} is as in The Logarithmic Energy of N Ordered Particles on the Weyl Chamber §energy. We write nΠ=∑(i,j)∈ΠN1n_{\Pi}=\sum_{(i,j)\in\Pi_{N}}1, NR=∑k=1N1N_{\mathbb{R}}=\sum_{k=1}^{N}1 (a real number), q0(x)=∥x∥2q_{0}(x)=\lVert x\rVert^{2}, q(x)=1+∥x∥2q(x)=1+\lVert x\rVert^{2} and l(x)=log⁡q(x)l(x)=\log q(x). For a function φ\varphi of class C2C^{2} on WNW_{N} we abbreviate F(x,φ(x),Dφ(x),D2φ(x))F(x,\varphi(x),D\varphi(x),D^{2}\varphi(x)) to F[φ](x)F[\varphi](x). Elementary order arithmetic is by Elementary Order Arithmetic in an Ordered Field, Elementary Arithmetic in an Ordered Field and Properties of the Absolute Value in an Ordered Field.

Step 0 (conventions and elementary facts). (a) Signs. 0≤dN0\le d_{N} and 0≤NR0\le N_{\mathbb{R}}, being finite sums of numbers equal to 00 or 11 (claim 5 of Properties of Finite Sums). ΠN\Pi_{N} contains (1,2)(1,2), the sum of 11 over {(1,2)}\{(1,2)\} is 11 by claim 1 of Peeling, Splitting, and Interchange for Sums over a Finite Index Set, so 1≤nΠ1\le n_{\Pi} by Nonnegativity and Monotonicity of a Sum over a Finite Index Set §monotone. For x∈WNx\in W_{N} we have 0≤∥x∥20\le\lVert x\rVert^{2}, so 1≤q(x)1\le q(x) and 0<q(x)−1≤10<q(x)^{-1}\le1 by Order Reversal under Reciprocals, and Summability of the Reciprocals of the Squares §reciprocal. Finally 0≤∣g(x)∣≤M0\le|g(x)|\le M at any point xx of WNW_{N}, so 0≤M0\le M.

(b) Logarithm. By The Function slog⁡ss\log s: Continuity, Young's Inequality and Lower Bounds, with the Elementary Bounds for the Exponential and the Logarithm §log, 1−t−1≤log⁡t≤t−11-t^{-1}\le\log t\le t-1 for positive tt, and log⁡(st)=log⁡s+log⁡t\log(st)=\log s+\log t for positive s,ts,t by The Natural Logarithm. Hence: (b1) if 0<y≤z0<y\le z then log⁡y≤log⁡z\log y\le\log z, because log⁡z=log⁡y+log⁡(zy−1)\log z=\log y+\log(zy^{-1}) and log⁡(zy−1)≥1−yz−1≥0\log(zy^{-1})\ge1-yz^{-1}\ge0, as yz−1≤1yz^{-1}\le1; (b2) log⁡(t2)=2log⁡t\log(t^{2})=2\log t for positive tt; (b3) 0≤1−q(x)−1≤l(x)0\le1-q(x)^{-1}\le l(x); (b4) 0<1−2−1≤log⁡20<1-2^{-1}\le\log2.

(c) Calculus. If φ,ψ\varphi,\psi are of class C2C^{2} on an open set and c∈Rc\in\mathbb{R}, then cφ+ψc\varphi+\psi is of class C2C^{2}, with gradient cDφ+DψcD\varphi+D\psi and Hessian cD2φ+D2ψcD^{2}\varphi+D^{2}\psi: this is claims 1 and 3 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set, applied to first and to iterated partial derivatives, read through Gradient of a Real-Valued Function on a Euclidean Open Set and Hessian Matrix of a C^2 Function. A constant function is smooth (claim 2 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set), hence of class C2C^{2} by Smooth Map on a Euclidean Open Set, and its partial derivatives vanish, its difference quotients in Partial Derivative on a Euclidean Open Set being 00. Traces satisfy tr⁡(cX+Y)=ctr⁡X+tr⁡Y\operatorname{tr}(cX+Y)=c\operatorname{tr}X+\operatorname{tr}Y by claim 1 of Basic Properties of the Trace. By claim 1 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n, ∥z∥2=z⋅z\lVert z\rVert^{2}=z\cdot z, so by Bilinearity and Symmetry of the Dot Product on Rn\mathbb{R}^n

∥cz+z′∥2=c2∥z∥2+2c z⋅z′+∥z′∥2.\lVert cz+z'\rVert^{2}=c^{2}\lVert z\rVert^{2}+2c\,z\cdot z'+\lVert z'\rVert^{2}.

(d) The squared norm. By claim 2 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n, q0(x)=1⋅dE(x,0RN)2q_{0}(x)=1\cdot d_{E}(x,0_{\mathbb{R}^{N}})^{2}, so by A Scaled Squared Distance to a Point is of Class C2C^2, with Gradient and Hessian (with c=1c=1 and aa the origin), on every open subset of RN\mathbb{R}^{N} the function q0q_{0} is of class C2C^{2} with Dq0(x)=2xDq_{0}(x)=2x and D2q0(x)=2IND^{2}q_{0}(x)=2I_{N}. By (c), the same holds for q=1+q0q=1+q_{0} on WNW_{N}.

Step 1 (the profile; claim 1). Let r=κ2+8θcr=\sqrt{\kappa^{2}+8\theta c} and r′=λ2+8θωr'=\sqrt{\lambda^{2}+8\theta\omega}, so r2=κ2+8θcr^{2}=\kappa^{2}+8\theta c and r′2=λ2+8θωr'^{2}=\lambda^{2}+8\theta\omega by Existence and Uniqueness of the Nonnegative Square Root. Since β=12(κ+r)\beta=\tfrac12(\kappa+r) gives β−κ=12(r−κ)\beta-\kappa=\tfrac12(r-\kappa),

β(β−κ)=14(r+κ)(r−κ)=14(r2−κ2)=2θc.\beta(\beta-\kappa)=\tfrac14(r+\kappa)(r-\kappa)=\tfrac14(r^{2}-\kappa^{2})=2\theta c .

Since a=(4θ)−1(r′−λ)a=(4\theta)^{-1}(r'-\lambda) gives 2θa+λ=12(r′+λ)2\theta a+\lambda=\tfrac12(r'+\lambda),

2θa2+λa=a(2θa+λ)=(8θ)−1(r′−λ)(r′+λ)=(8θ)−1(r′2−λ2)=ω.2\theta a^{2}+\lambda a=a(2\theta a+\lambda)=(8\theta)^{-1}(r'-\lambda)(r'+\lambda)=(8\theta)^{-1}(r'^{2}-\lambda^{2})=\omega .

Let V1(t)=θa t2V_{1}(t)=\theta a\,t^{2} for t∈Rt\in\mathbb{R}. By A Scaled Squared Distance to a Point is of Class C2C^2, with Gradient and Hessian with n=1n=1, c=θac=\theta a and aa the origin (and claims 1 and 2 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n in R1\mathbb{R}^{1}), V1V_{1} is of class C2C^{2} on R\mathbb{R} with V1′(t)=2θa tV_{1}'(t)=2\theta a\,t and V1′′(t)=2θaV_{1}''(t)=2\theta a. Moreover ∣t∣2=t2|t|^{2}=t^{2} (claims 1 and 4 of Properties of the Absolute Value in an Ordered Field), so

0≤(2θa∣t∣−1)2=4θ2a2t2−4θa∣t∣+1,0\le(2\theta a|t|-1)^{2}=4\theta^{2}a^{2}t^{2}-4\theta a|t|+1 ,

and dividing by 4θa>04\theta a>0 gives 1⋅∣t∣−(4θa)−1≤V1(t)1\cdot|t|-(4\theta a)^{-1}\le V_{1}(t). Let P^(x)=H(x)+∑k=1NV1(xk)\widehat{P}(x)=H(x)+\sum_{k=1}^{N}V_{1}(x_{k}). By claim 3 of Properties of Finite Sums and claim 1 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n, ∑k=1NV1(xk)=θa∥x∥2\sum_{k=1}^{N}V_{1}(x_{k})=\theta a\lVert x\rVert^{2}, so P^=θP\widehat{P}=\theta P. By The Confined Logarithmic Energy on the Weyl Chamber: Regularity, Penalty Property, Monotone Gradient and the Dissipation Inequality §penalty with a0=1a_{0}=1 and b0=(4θa)−1b_{0}=(4\theta a)^{-1}, P^\widehat{P} is a penalty on WNW_{N}. Hence P=θ−1P^P=\theta^{-1}\widehat{P} is of class C2C^{2} by (c) and Penalty on an Open Subset of Euclidean Space §regularity; and for t∈Rt\in\mathbb{R}, multiplying by θ\theta and by θ−1\theta^{-1} (claim 5 of Elementary Arithmetic in an Ordered Field) shows {x∈WN:P(x)≤t}={x∈WN:P^(x)≤θt}\{x\in W_{N}:P(x)\le t\}=\{x\in W_{N}:\widehat{P}(x)\le\theta t\}, which is compact by Penalty on an Open Subset of Euclidean Space §sublevel. So PP is a penalty on WNW_{N}, and claim 1 holds.

Step 2 (derivatives of PP). By The Confined Logarithmic Energy on the Weyl Chamber: Regularity, Penalty Property, Monotone Gradient and the Dissipation Inequality §regularity with this V1V_{1} and The Logarithmic Energy on the Weyl Chamber: Derivatives, Monotone Gradient, the Calogero Identity and the Euler Identity §derivatives, ∂kP^(x)=2θa xk+∂kH(x)\partial_{k}\widehat{P}(x)=2\theta a\,x_{k}+\partial_{k}H(x) and tr⁡(D2P^(x))=βS(x)+∑k=1N2θa=βS(x)+2θaNR\operatorname{tr}(D^{2}\widehat{P}(x))=\beta S(x)+\sum_{k=1}^{N}2\theta a=\beta S(x)+2\theta a N_{\mathbb{R}}. By (c),

DP(x)=θ−1DH(x)+2a x,tr⁡(D2P(x))=θ−1βS(x)+2aNR.DP(x)=\theta^{-1}DH(x)+2a\,x,\qquad \operatorname{tr}\bigl(D^{2}P(x)\bigr)=\theta^{-1}\beta S(x)+2aN_{\mathbb{R}} .

By (c), The Logarithmic Energy on the Weyl Chamber: Derivatives, Monotone Gradient, the Calogero Identity and the Euler Identity §calogero and The Logarithmic Energy on the Weyl Chamber: Derivatives, Monotone Gradient, the Calogero Identity and the Euler Identity §euler,

∥DP(x)∥2=θ−2∥DH(x)∥2+4aθ−1DH(x)⋅x+4a2∥x∥2=θ−2β2S(x)−2aθ−1βdN+4a2∥x∥2.\lVert DP(x)\rVert^{2}=\theta^{-2}\lVert DH(x)\rVert^{2}+4a\theta^{-1}DH(x)\cdot x+4a^{2}\lVert x\rVert^{2}=\theta^{-2}\beta^{2}S(x)-2a\theta^{-1}\beta d_{N}+4a^{2}\lVert x\rVert^{2}.

Step 3 (the key identity). Let s,k∈Rs,k\in\mathbb{R} and φ=sP+k\varphi=sP+k. By (c), φ\varphi is of class C2C^{2} with Dφ=sDPD\varphi=sDP and D2φ=sD2PD^{2}\varphi=sD^{2}P, and ∥sDP∥2=s2∥DP∥2\lVert sDP\rVert^{2}=s^{2}\lVert DP\rVert^{2}. Insert Step 2 into the operator, write λsP=λsθ−1H+λsa∥x∥2\lambda sP=\lambda s\theta^{-1}H+\lambda sa\lVert x\rVert^{2}, and use c=(2θ)−1(β2−κβ)c=(2\theta)^{-1}(\beta^{2}-\kappa\beta) from Step 1. Collecting the coefficients of S(x)S(x) and of ∥x∥2\lVert x\rVert^{2} gives, for x∈WNx\in W_{N},

F[φ](x)=e(s)S(x)+f(s)∥x∥2+λsθ−1H(x)−s2aβdN−κsaNR+λk−g(x),F[\varphi](x)=e(s)S(x)+f(s)\lVert x\rVert^{2}+\lambda s\theta^{-1}H(x)-s^{2}a\beta d_{N}-\kappa saN_{\mathbb{R}}+\lambda k-g(x), e(s)=(2θ)−1((sβ)2−κsβ−β2+κβ),f(s)=2θa2s2+λas−ω.e(s)=(2\theta)^{-1}\bigl((s\beta)^{2}-\kappa s\beta-\beta^{2}+\kappa\beta\bigr),\qquad f(s)=2\theta a^{2}s^{2}+\lambda as-\omega .

Here e(1)=0e(1)=0, and f(1)=0f(1)=0 by Step 1.

Step 4 (two bounds on HH). (U) For every positive μ\mu and x∈WNx\in W_{N},

H(x)≤βnΠ2μS(x)+βnΠ2(log⁡μ−1).H(x)\le\tfrac{\beta n_{\Pi}}{2\mu}S(x)+\tfrac{\beta n_{\Pi}}{2}(\log\mu-1).

Indeed, let (i,j)∈ΠN(i,j)\in\Pi_{N} and t=xi−xj>0t=x_{i}-x_{j}>0, so aij(x)=t−1a_{ij}(x)=t^{-1}. The lower bound of (b) at μt2\mu t^{2}, together with (b2), gives log⁡μ+2log⁡t=log⁡(μt2)≥1−μ−1aij(x)2\log\mu+2\log t=\log(\mu t^{2})\ge1-\mu^{-1}a_{ij}(x)^{2}, so −log⁡t≤12(μ−1aij(x)2−1+log⁡μ)-\log t\le\tfrac12(\mu^{-1}a_{ij}(x)^{2}-1+\log\mu). Squares are nonnegative, so aij(x)2≤∑j′=1Naij′(x)2≤S(x)a_{ij}(x)^{2}\le\sum_{j'=1}^{N}a_{ij'}(x)^{2}\le S(x) by claims 5 and 6 of Properties of Finite Sums. Hence −log⁡(xi−xj)≤12(μ−1S(x)−1+log⁡μ)-\log(x_{i}-x_{j})\le\tfrac12(\mu^{-1}S(x)-1+\log\mu) for every (i,j)∈ΠN(i,j)\in\Pi_{N}. Summing over ΠN\Pi_{N} (Nonnegativity and Monotonicity of a Sum over a Finite Index Set §comparison, and claims 3 and 4 of Properties of a Sum over a Finite Index Set) and multiplying by β\beta gives (U).

(L) For every x∈WNx\in W_{N},

H(x)≥−βnΠlog⁡2−βnΠ2 l(x).H(x)\ge-\beta n_{\Pi}\log2-\tfrac{\beta n_{\Pi}}{2}\,l(x).

Indeed, for (i,j)∈ΠN(i,j)\in\Pi_{N}, claims 2, 3 and 5 of Properties of the Absolute Value in an Ordered Field and claim 4 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n give 0<xi−xj≤∣xi∣+∣xj∣≤2∥x∥0<x_{i}-x_{j}\le|x_{i}|+|x_{j}|\le2\lVert x\rVert, so (xi−xj)2≤4∥x∥2≤4q(x)(x_{i}-x_{j})^{2}\le4\lVert x\rVert^{2}\le4q(x) by claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field. By (b1) and (b2), 2log⁡(xi−xj)≤log⁡4+l(x)=2log⁡2+l(x)2\log(x_{i}-x_{j})\le\log4+l(x)=2\log2+l(x). Summing over ΠN\Pi_{N} as in (U) and multiplying by −β-\beta gives (L).

Step 5 (classical subsolutions of weight below 11). Let s0=2−1(1+κ(2β)−1)s_{0}=2^{-1}\bigl(1+\kappa(2\beta)^{-1}\bigr). As stated in the theorem, 0≤κ<2β0\le\kappa<2\beta, so 0≤κ(2β)−1<10\le\kappa(2\beta)^{-1}<1 and, by claim 8 of Elementary Order Arithmetic in an Ordered Field, 0<s00<s_{0} and κ(2β)−1<s0<1\kappa(2\beta)^{-1}<s_{0}<1. Fix ss with s0≤s<1s_{0}\le s<1; then κ2<sβ<β\tfrac{\kappa}{2}<s\beta<\beta. Since t2−κt−(u2−κu)=(t−u)(t+u−κ)t^{2}-\kappa t-(u^{2}-\kappa u)=(t-u)(t+u-\kappa),

e(s)=(2θ)−1(sβ−β)(sβ+β−κ)<0,e(s)=(2\theta)^{-1}(s\beta-\beta)(s\beta+\beta-\kappa)<0,

the first factor being negative and the second positive (as sβ>κ2s\beta>\tfrac{\kappa}{2} and β>κ2\beta>\tfrac{\kappa}{2}); and

f(s)=f(s)−f(1)=(s−1)(2θa2(s+1)+λa)<0.f(s)=f(s)-f(1)=(s-1)\bigl(2\theta a^{2}(s+1)+\lambda a\bigr)<0 .

Put μs=λsθ−1βnΠ(2(−e(s)))−1\mu_{s}=\lambda s\theta^{-1}\beta n_{\Pi}\bigl(2(-e(s))\bigr)^{-1}, which is positive since nΠ≥1n_{\Pi}\ge1; Cs=λsθ−1βnΠ2(log⁡μs−1)C_{s}=\lambda s\theta^{-1}\tfrac{\beta n_{\Pi}}{2}(\log\mu_{s}-1); and Ks=λ−1(∣Cs∣+M)≥0K_{s}=\lambda^{-1}(|C_{s}|+M)\ge0. Multiplying (U) with μ=μs\mu=\mu_{s} by λsθ−1>0\lambda s\theta^{-1}>0 gives λsθ−1H(x)≤−e(s)S(x)+Cs\lambda s\theta^{-1}H(x)\le-e(s)S(x)+C_{s}. By Step 3 with k=−Ksk=-K_{s}, using f(s)∥x∥2≤0f(s)\lVert x\rVert^{2}\le0, −s2aβdN≤0-s^{2}a\beta d_{N}\le0, −κsaNR≤0-\kappa saN_{\mathbb{R}}\le0 (Step 0(a)) and −g(x)≤M-g(x)\le M,

F[sP−Ks](x)≤Cs−∣Cs∣−M+M≤0(x∈WN).F[sP-K_{s}](x)\le C_{s}-|C_{s}|-M+M\le0\qquad(x\in W_{N}).

So sP−KssP-K_{s} is a classical subsolution of FF on WNW_{N}. With s=s0<1s=s_{0}<1 this is hypothesis Comparison Principle with a Weighted Penalty for Operators Convex in the Value, Gradient and Matrix Variables §barrier for w=1w=1.

Step 6 (the operator hypotheses). Let b:WN→RNb:W_{N}\to\mathbb{R}^{N} be the constant map with value the origin and G(x)=cS(x)+ωq0(x)+g(x)G(x)=cS(x)+\omega q_{0}(x)+g(x). By claim 4 of Bilinearity and Symmetry of the Dot Product on Rn\mathbb{R}^n (with μ=0\mu=0), b(x)⋅p=0b(x)\cdot p=0, so FF is the operator of The Viscous Hamilton-Jacobi Operator with a Drift that is One-Sided Lipschitz on Sublevel Sets Satisfies the Operator Hypotheses of the Weighted-Penalty Comparison Principle with n=Nn=N, D=WND=W_{N}, the penalty PP, and λ,θ,κ,b,G\lambda,\theta,\kappa,b,G. The map bb is continuous, and it is one-sided Lipschitz on sublevel sets with cR=0c_{R}=0, since (b(x)−b(y))⋅(x−y)=0(b(x)-b(y))\cdot(x-y)=0. For continuity of GG: HH is of class C2C^{2} by The Logarithmic Energy on the Weyl Chamber: Derivatives, Monotone Gradient, the Calogero Identity and the Euler Identity §derivatives, so DHDH is continuous on WNW_{N} by Continuity of the Value, Gradient and Hessian Maps of a Differentiable Function §hessian; q0q_{0} is continuous on RN\mathbb{R}^{N} by The Squared Euclidean Norm is Smooth and claim 3 of Euclidean Space is Open in Itself, and CkC^k Maps are Continuous; so q0∘DHq_{0}\circ DH and the restriction of q0q_{0} to WNW_{N} are continuous on WNW_{N} by claims 3 and 4 of Semicontinuity and Continuity Under Composition with a Continuous Map. By The Logarithmic Energy on the Weyl Chamber: Derivatives, Monotone Gradient, the Calogero Identity and the Euler Identity §calogero, G=cβ−2(q0∘DH)+ωq0+gG=c\beta^{-2}(q_{0}\circ DH)+\omega q_{0}+g. A combination c1f1+c2f2+c3f3c_{1}f_{1}+c_{2}f_{2}+c_{3}f_{3} of real functions continuous on WNW_{N} is continuous (Continuous Map Between Metric Spaces, with the metric of The Absolute Value Metric on the Real Line): given xx and ε>0\varepsilon>0, take for each ii a δi\delta_{i} that works for fif_{i} at xx with ε(3(1+∣ci∣))−1\varepsilon\bigl(3(1+|c_{i}|)\bigr)^{-1}, and the least δ\delta of the three (claim 9 of Elementary Order Arithmetic in an Ordered Field); by claims 4 and 5 of Properties of the Absolute Value in an Ordered Field the combination then varies by less than ε\varepsilon. Hence GG is continuous and, by The Viscous Hamilton-Jacobi Operator with a Drift that is One-Sided Lipschitz on Sublevel Sets Satisfies the Operator Hypotheses of the Weighted-Penalty Comparison Principle, FF satisfies Comparison Principle with a Weighted Penalty for Operators Convex in the Value, Gradient and Matrix Variables §continuity, Comparison Principle with a Weighted Penalty for Operators Convex in the Value, Gradient and Matrix Variables §strictly-proper with γ=λ\gamma=\lambda, Comparison Principle with a Weighted Penalty for Operators Convex in the Value, Gradient and Matrix Variables §convex and Comparison Principle with a Weighted Penalty for Operators Convex in the Value, Gradient and Matrix Variables §structure. In particular FF is degenerate elliptic, by claim 1 of Strictly Proper Second-Order Equation Operator.

Step 7 (comparison; claim 2). Apply Comparison Principle with a Weighted Penalty for Operators Convex in the Value, Gradient and Matrix Variables with D=WND=W_{N}, the penalty PP of Step 1, w=1w=1 and γ=λ\gamma=\lambda; its hypotheses 1 to 4 hold by Step 6, and hypothesis 5 by Step 5. Since 1⋅P=P1\cdot P=P, the growth assumptions of claim 2 are exactly those on u−wPu-wP and v−wPv-wP, so u(x)≤v(x)u(x)\le v(x) for every x∈WNx\in W_{N}.

Step 8 (a viscosity subsolution of weight 11). Let mm be as in Basic Properties of the Sublevel Sets of a Penalty §bounded-below, so m≤Pm\le P. Let F={sP−Ks:s0≤s<1}\mathcal{F}=\{sP-K_{s}:s_{0}\le s<1\}, a nonempty set. Each member is of class C2C^{2} and a classical subsolution (Step 5), hence a viscosity subsolution by claim 1 of Classical Sub- and Supersolutions of a Degenerate Elliptic Operator are Viscosity Sub- and Supersolutions, FF being degenerate elliptic (Step 6). For s0≤s<1s_{0}\le s<1 we have 0<1−s≤10<1-s\le1, so for y∈WNy\in W_{N}

P(y)−(sP(y)−Ks)=(1−s)P(y)+Ks≥(1−s)m≥−∣m∣;P(y)-\bigl(sP(y)-K_{s}\bigr)=(1-s)P(y)+K_{s}\ge(1-s)m\ge-|m| ;

thus every v∈Fv\in\mathcal{F} satisfies v≤P+∣m∣v\le P+|m|. Fix x∈WNx\in W_{N}. By Continuity of the Value, Gradient and Hessian Maps of a Differentiable Function §value, PP is continuous at xx, so there is δ>0\delta>0 with P(y)<P(x)+1P(y)<P(x)+1 whenever dE(x,y)<δd_{E}(x,y)<\delta; with r=δ2r=\tfrac{\delta}{2}, every v∈Fv\in\mathcal{F} satisfies v(y)≤P(x)+1+∣m∣v(y)\le P(x)+1+|m| whenever dE(y,x)≤rd_{E}(y,x)\le r. So F\mathcal{F} is locally uniformly bounded above, and since FF is continuous (Step 6), The Upper Semicontinuous Envelope of a Supremum of Viscosity Subsolutions is a Viscosity Subsolution shows that u‾=u~∗\underline{u}=\widetilde{u}^{*}, where u~(x)=sup⁡{v(x):v∈F}\widetilde{u}(x)=\sup\{v(x):v\in\mathcal{F}\}, is a viscosity subsolution of FF on WNW_{N}.

The function P+∣m∣P+|m| is of class C2C^{2} by (c), hence continuous by Continuity of the Value, Gradient and Hessian Maps of a Differentiable Function §value, hence upper semicontinuous on WNW_{N} (claim 3 of Properties of the Absolute Value in an Ordered Field). As u~≤P+∣m∣\widetilde{u}\le P+|m|, Properties of the Upper Semicontinuous Envelope §least gives u‾≤P+∣m∣\underline{u}\le P+|m|. Growth from above: for δ>0\delta>0, δP≥δm≥−δ∣m∣\delta P\ge\delta m\ge-\delta|m|, so u‾−P≤∣m∣≤(1+δ)∣m∣+δP\underline{u}-P\le|m|\le(1+\delta)|m|+\delta P. Growth from below: by Properties of the Upper Semicontinuous Envelope §bounds, u‾≥u~≥sP−Ks\underline{u}\ge\widetilde{u}\ge sP-K_{s} for every s∈[s0,1)s\in[s_{0},1). If 0<δ≤1−s00<\delta\le1-s_{0}, take s=1−δs=1-\delta: u‾−P≥−K1−δ−δP\underline{u}-P\ge-K_{1-\delta}-\delta P. If δ>δ0=1−s0\delta>\delta_{0}=1-s_{0}, take s=s0s=s_{0}: u‾−P≥−Ks0−δ0P=−Ks0−δP+(δ−δ0)P≥−(Ks0+(δ−δ0)∣m∣)−δP\underline{u}-P\ge-K_{s_{0}}-\delta_{0}P=-K_{s_{0}}-\delta P+(\delta-\delta_{0})P\ge-\bigl(K_{s_{0}}+(\delta-\delta_{0})|m|\bigr)-\delta P. So u‾−P\underline{u}-P has PP-subordinate growth from above and from below.

Step 9 (a viscosity supersolution of weight 11). Let L=βnΠ(2θ)−1>0L=\beta n_{\Pi}(2\theta)^{-1}>0, Λ=θ−1βnΠlog⁡2≥0\Lambda=\theta^{-1}\beta n_{\Pi}\log2\ge0 (by (b4)),

K′=λ−1(λΛ+(a+L)βdN+κ(a+L)NR+M)≥0,u‾=P+L l+K′.K'=\lambda^{-1}\bigl(\lambda\Lambda+(a+L)\beta d_{N}+\kappa(a+L)N_{\mathbb{R}}+M\bigr)\ge0,\qquad \overline{u}=P+L\,l+K' .

Derivatives of ll. The set V=(0,∞)V=(0,\infty) is open in R1\mathbb{R}^{1} and q(x)∈Vq(x)\in V for x∈WNx\in W_{N}. By The Natural Logarithm, log⁡\log is smooth on VV with derivative ρ(t)=t−1\rho(t)=t^{-1}; ρ=∂1log⁡\rho=\partial_{1}\log is smooth on VV by claim 3 of Coordinate Functions, the CkC^k Hierarchy, and Partial Derivatives of a Smooth Map, and ∂1ρ(t)=−(t−1)2\partial_{1}\rho(t)=-(t^{-1})^{2} by claim 2 of Reciprocal Rule for One-Dimensional Derivatives (for a function of one variable on an open interval, the limit defining the partial derivative in Partial Derivative on a Euclidean Open Set is the one defining the derivative in Derivative at an Interior Point). By claims 1 and 2 of A Composition of CkC^k Maps Between Euclidean Open Sets is of Class CkC^k (smooth maps being of class CkC^{k} for every kk by Smooth Map on a Euclidean Open Set) and Step 0(d), l=log⁡∘ql=\log\circ q is of class C2C^{2} on WNW_{N} with ∂il=(ρ∘q) ∂iq\partial_{i}l=(\rho\circ q)\,\partial_{i}q, i.e. Dl(x)=2q(x)−1xDl(x)=2q(x)^{-1}x; and ρ∘q\rho\circ q is of class C1C^{1} with ∂i(ρ∘q)(x)=−q(x)−2 2xi\partial_{i}(\rho\circ q)(x)=-q(x)^{-2}\,2x_{i}. By the product rule (claim 1 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set) and ∂i∂iq=2\partial_{i}\partial_{i}q=2 (Step 0(d), Hessian Matrix of a C^2 Function, Identity Matrix),

∂i∂il(x)=2q(x)−1−4q(x)−2xi2,tr⁡(D2l(x))=2q(x)−1NR−4q(x)−2∥x∥2≤2NR,\partial_{i}\partial_{i}l(x)=2q(x)^{-1}-4q(x)^{-2}x_{i}^{2},\qquad \operatorname{tr}\bigl(D^{2}l(x)\bigr)=2q(x)^{-1}N_{\mathbb{R}}-4q(x)^{-2}\lVert x\rVert^{2}\le2N_{\mathbb{R}},

by Trace of a Real Square Matrix, claims 2 and 3 of Properties of Finite Sums, claim 1 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n and Step 0(a).

Supersolution. By (c), u‾\overline{u} is of class C2C^{2} with Du‾=DP+L DlD\overline{u}=DP+L\,Dl and D2u‾=D2P+L D2lD^{2}\overline{u}=D^{2}P+L\,D^{2}l. Expanding ∥DP+L Dl∥2\lVert DP+L\,Dl\rVert^{2} by (c) and using Step 3 with s=1s=1, k=K′k=K' and e(1)=f(1)=0e(1)=f(1)=0,

F[u‾](x)=λθ−1H−aβdN−κaNR+λK′−g+λL l+θL DP⋅Dl+θ2L2∥Dl∥2−κ2Ltr⁡(D2l),F[\overline{u}](x)=\lambda\theta^{-1}H-a\beta d_{N}-\kappa aN_{\mathbb{R}}+\lambda K'-g+\lambda L\,l+\theta L\,DP\cdot Dl+\tfrac{\theta}{2}L^{2}\lVert Dl\rVert^{2}-\tfrac{\kappa}{2}L\operatorname{tr}(D^{2}l),

all functions evaluated at xx. By (L), θ−1H≥−Λ−L l\theta^{-1}H\ge-\Lambda-L\,l, so λθ−1H+λL l≥−λΛ\lambda\theta^{-1}H+\lambda L\,l\ge-\lambda\Lambda. By Step 2, Bilinearity and Symmetry of the Dot Product on Rn\mathbb{R}^n and The Logarithmic Energy on the Weyl Chamber: Derivatives, Monotone Gradient, the Calogero Identity and the Euler Identity §euler,

DP⋅Dl=2q−1θ−1DH⋅x+4aq−1∥x∥2=−q−1θ−1βdN+4aq−1∥x∥2≥−θ−1βdN,DP\cdot Dl=2q^{-1}\theta^{-1}DH\cdot x+4aq^{-1}\lVert x\rVert^{2}=-q^{-1}\theta^{-1}\beta d_{N}+4aq^{-1}\lVert x\rVert^{2}\ge-\theta^{-1}\beta d_{N},

since 0<q−1≤10<q^{-1}\le1 and 0≤dN0\le d_{N}; so θL DP⋅Dl≥−LβdN\theta L\,DP\cdot Dl\ge-L\beta d_{N}. Also θ2L2∥Dl∥2≥0\tfrac{\theta}{2}L^{2}\lVert Dl\rVert^{2}\ge0, −κ2Ltr⁡(D2l)≥−κLNR-\tfrac{\kappa}{2}L\operatorname{tr}(D^{2}l)\ge-\kappa LN_{\mathbb{R}} and −g≥−M-g\ge-M. Therefore

F[u‾](x)≥−λΛ−(a+L)βdN−κ(a+L)NR−M+λK′=0,F[\overline{u}](x)\ge-\lambda\Lambda-(a+L)\beta d_{N}-\kappa(a+L)N_{\mathbb{R}}-M+\lambda K'=0 ,

so u‾\overline{u} is a classical supersolution, hence a viscosity supersolution by claim 2 of Classical Sub- and Supersolutions of a Degenerate Elliptic Operator are Viscosity Sub- and Supersolutions.

Weight. u‾−P=L l+K′\overline{u}-P=L\,l+K'. From below: for δ>0\delta>0, −δ∣m∣−δP≤0≤L l+K′-\delta|m|-\delta P\le0\le L\,l+K' by (b3). From above: fix δ>0\delta>0 and let η=δa((1+δ)L)−1>0\eta=\delta a\bigl((1+\delta)L\bigr)^{-1}>0. The upper bound of (b) at ηq(x)\eta q(x) gives log⁡η+l(x)≤ηq(x)−1\log\eta+l(x)\le\eta q(x)-1, hence

(1+δ)L l(x)≤δa∥x∥2+δa+(1+δ)L ∣1+log⁡η∣.(1+\delta)L\,l(x)\le\delta a\lVert x\rVert^{2}+\delta a+(1+\delta)L\,|1+\log\eta| .

By (L), a∥x∥2=P(x)−θ−1H(x)≤P(x)+Λ+L l(x)a\lVert x\rVert^{2}=P(x)-\theta^{-1}H(x)\le P(x)+\Lambda+L\,l(x), so δa∥x∥2≤δP(x)+δΛ+δL l(x)\delta a\lVert x\rVert^{2}\le\delta P(x)+\delta\Lambda+\delta L\,l(x). Combining and subtracting δL l(x)\delta L\,l(x),

u‾(x)−P(x)≤(δΛ+δa+(1+δ)L∣1+log⁡η∣+K′)+δP(x).\overline{u}(x)-P(x)\le\bigl(\delta\Lambda+\delta a+(1+\delta)L|1+\log\eta|+K'\bigr)+\delta P(x).

So u‾−P\overline{u}-P has PP-subordinate growth from above and from below.

Step 10 (existence and uniqueness; claim 3). Apply Perron's Method with a Weighted Penalty for Operators Convex in the Value, Gradient and Matrix Variables: Existence and Uniqueness of a Viscosity Solution of Given Weight with D=WND=W_{N} (open and nonempty), the penalty PP, w=1w=1 and γ=λ\gamma=\lambda: its operator hypotheses hold by Step 6 and its barrier by Step 5 (s0<1s_{0}<1). Since 1⋅P=P1\cdot P=P, a function ff is of weight 11 in the sense of that theorem exactly when f−Pf-P has PP-subordinate growth from above and from below; so u‾\underline{u} (Step 8) and u‾\overline{u} (Step 9) are a viscosity subsolution and a viscosity supersolution of weight 11. By Perron's Method with a Weighted Penalty for Operators Convex in the Value, Gradient and Matrix Variables: Existence and Uniqueness of a Viscosity Solution of Given Weight §existence there is a function uu with the properties of claim 3, by Perron's Method with a Weighted Penalty for Operators Convex in the Value, Gradient and Matrix Variables: Existence and Uniqueness of a Viscosity Solution of Given Weight §uniqueness any two such functions are equal, and by Perron's Method with a Weighted Penalty for Operators Convex in the Value, Gradient and Matrix Variables: Existence and Uniqueness of a Viscosity Solution of Given Weight §continuity it is continuous on WNW_{N}. This proves claim 3.

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