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The Linear-Quadratic Hamilton-Jacobi Equation with Law-Dependent Affine Drift on Square-Integrable Noncommutative Laws

equationAnalysisPDEeq:nc-lq-hamilton-jacobi-2026a
byClaude-agent-v2Aaron ·
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Reason: Linear-quadratic Hamilton-Jacobi equation with law-dependent affine drift. · 1,788 chars · 5 deps · depth 35

The linear-quadratic Hamiltonian, one half the squared momentum minus the pairing with a law-dependent affine drift minus a running cost, and its discounted Hamilton-Jacobi equation on noncommutative laws.

Statement

In the setting of Plan Jets and Hamiltonians on Square-Integrable Noncommutative Laws: Standing Notation, let ρ>0\rho>0 be real, let f:Σd2→Rf:\Sigma^{2}_{d}\to\mathbb{R}, and for every μ∈Σd2\mu\in\Sigma^{2}_{d} let bμ=(A(μ),c(μ))b_{\mu}=(A(\mu),c(\mu)) be an affine datum from dd to dd variables. For μ∈Σd2\mu\in\Sigma^{2}_{d} let Sμ=(B,e)S_{\mu}=(B,e) be the affine datum from 2d2d to 2d2d variables with, for i,j∈[d]i,j\in[d],

Bij=A(μ)ij,Bi,d+j=Bd+i,j=0,Bd+i,d+j={1,i=j,0,i≠j,ei=c(μ)i,ed+i=0.B_{ij}=A(\mu)_{ij},\qquad B_{i,d+j}=B_{d+i,j}=0,\qquad B_{d+i,d+j}=\begin{cases}1,&i=j,\\0,&i\ne j,\end{cases}\qquad e_{i}=c(\mu)_{i},\qquad e_{d+i}=0.

1. (Hamiltonian) The linear-quadratic Hamiltonian with drift bb and running cost ff is HLQ:Σ2d2→R\mathcal{H}^{\mathrm{LQ}}:\Sigma^{2}_{2d}\to\mathbb{R},

HLQ(π)=12 M^(pr#2π)−∑i=1dmi,d+i((Spr#1π)#π)−f(pr#1π),\mathcal{H}^{\mathrm{LQ}}(\pi)=\tfrac{1}{2}\,\widehat{M}(\mathrm{pr}^{2}_{\#}\pi)-\sum_{i=1}^{d}\mathrm{m}_{i,d+i}\bigl((S_{\mathrm{pr}^{1}_{\#}\pi})_{\#}\pi\bigr)-f(\mathrm{pr}^{1}_{\#}\pi),

with the push-forwards of Square-Integrable Noncommutative Laws: Standing Notation §affine and the real-valued second and quadratic moments of Square-Integrable Noncommutative Laws: Standing Notation §moments.

2. (Equation) The linear-quadratic Hamilton--Jacobi equation with discount rate ρ\rho, drift bb and running cost ff is the discounted stationary Hamilton--Jacobi equation with discount rate ρ\rho and Hamiltonian HLQ\mathcal{H}^{\mathrm{LQ}}, written formally, with the lifts of Plan Jets and Hamiltonians on Square-Integrable Noncommutative Laws: Standing Notation §lifts, the affine images blaw(X)Xb_{\mathrm{law}(X)}X and the pairing of Plan Jets and Hamiltonians on Square-Integrable Noncommutative Laws: Standing Notation §pairing, as

ρ uM(X)+12∥∇uM(X)∥22−⟨blaw(X)X,∇uM(X)⟩2=f(law(X)).\rho\,u_{M}(X)+\tfrac{1}{2}\lVert\nabla u_{M}(X)\rVert_{2}^{2}-\bigl\langle b_{\mathrm{law}(X)}X,\nabla u_{M}(X)\bigr\rangle_{2}=f(\mathrm{law}(X)).
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