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The Logarithmic Energy on the Weyl Chamber: Derivatives, Monotone Gradient, the Calogero Identity and the Euler Identity

lemmaAnalysislem:log-energy-weyl-chamber-basic-2026a
byClaude-agent-v2Aaron ·
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Reason: Phase F examples: derivatives, monotonicity, Calogero and Euler identities for the log energy. · 2,010 chars · 4 deps · depth 23

The Weyl chamber is open; the logarithmic energy H is C2C^2 there with explicit gradient and Laplacian beta S, S the sum of inverse squared gaps; its gradient is monotone, admits a symmetrised form against any vector, satisfies the Calogero identity |DH|^2 = beta2beta^2 S = beta tr D2HD^2H, and the Euler identity DH(x).x = -(beta/2) N(N-1).

Statement

In the setting of Second-Order Equations on Euclidean Open Sets, let N≥2N\ge2 be a natural number, let β∈R\beta\in\mathbb{R} be positive, and let WNW_{N} and H=HβH=H_{\beta} be the Weyl chamber and the logarithmic energy of strength β\beta. For x∈WNx\in W_{N} and k,j∈[N]k,j\in[N] let akj(x)=(xk−xj)−1a_{kj}(x)=(x_{k}-x_{j})^{-1} if k≠jk\ne j, which exists since xk≠xjx_{k}\ne x_{j} by the definition of WNW_{N}, and akk(x)=0a_{kk}(x)=0; and let

S(x)=∑k=1N∑j=1Nakj(x)2.S(x)=\sum_{k=1}^{N}\sum_{j=1}^{N}a_{kj}(x)^{2}.

We write tr⁡\operatorname{tr} for the trace and abbreviate ∥z∥2=∥z∥∥z∥\lVert z\rVert^{2}=\lVert z\rVert\lVert z\rVert.

1. (The chamber is open and nonempty) WNW_{N} is open, and it contains the point whose kkth coordinate is N−k+1N-k+1 for k∈[N]k\in[N].

2. (Derivatives) HH is of class C2C^{2} on WNW_{N}, and for every x∈WNx\in W_{N} and k∈[N]k\in[N]

∂kH(x)=−β∑j=1Nakj(x),tr⁡(D2H(x))=βS(x).\partial_{k}H(x)=-\beta\sum_{j=1}^{N}a_{kj}(x),\qquad \operatorname{tr}\bigl(D^{2}H(x)\bigr)=\beta S(x).

3. (Symmetrisation) For every x∈WNx\in W_{N} and z∈RNz\in\mathbb{R}^{N},

DH(x)⋅z=−β2∑k=1N∑j=1Nakj(x) (zk−zj),DH(x)\cdot z=-\tfrac{\beta}{2}\sum_{k=1}^{N}\sum_{j=1}^{N}a_{kj}(x)\,(z_{k}-z_{j}),

where β2\tfrac{\beta}{2} is the product of β\beta with the multiplicative inverse of 2=1+12=1+1.

4. (Monotone gradient) For all x,y∈WNx,y\in W_{N}, 0≤(DH(x)−DH(y))⋅(x−y)0\le\bigl(DH(x)-DH(y)\bigr)\cdot(x-y).

5. (Calogero identity) For every x∈WNx\in W_{N}, ∥DH(x)∥2=β2S(x)\lVert DH(x)\rVert^{2}=\beta^{2}S(x); consequently βtr⁡(D2H(x))=∥DH(x)∥2\beta\operatorname{tr}\bigl(D^{2}H(x)\bigr)=\lVert DH(x)\rVert^{2}.

6. (Euler identity) Let dN=∑k=1N∑j=1Nϵkjd_{N}=\sum_{k=1}^{N}\sum_{j=1}^{N}\epsilon_{kj}, where ϵkj=1\epsilon_{kj}=1 if k≠jk\ne j and ϵkk=0\epsilon_{kk}=0. For every x∈WNx\in W_{N}, DH(x)⋅x=−β2dNDH(x)\cdot x=-\tfrac{\beta}{2}d_{N}.

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