TheoremBase

A Hamilton-Jacobi Operator with a Monotone Nonlinearity and a Lipschitz Perturbation Satisfies the Comparison Hypotheses

On a Hilbert triple, the operator obtained by adding a monotone nonlinearity and a Lipschitz perturbation to the drift of the dissipative Hamilton-Jacobi operator is first order, strictly proper, satisfies the first-order structure condition with an explicit structure pair, satisfies the shift-continuity condition, and therefore admits comparison. The cost is required only to be bounded and uniformly continuous for the norm of the smaller space. No restriction is placed on the size of the discount rate.

Statement

In the setting of Hilbert Triples: Standing Notation and Background, the set HH is open in HH by Hilbert Triples: Standing Notation and Background (v); accordingly W=D(A)∩H=D(A)W=D(A)\cap H=D(A) and V∩H=VV\cap H=V there. Let Sym(V)\mathrm{Sym}(V) be as in Hilbert Triples: Standing Notation and Background (vi) and let hh be the penalty function.

Let λ0,Cg∈R\lambda_{0},C_{g}\in\mathbb{R} satisfy 0<λ00<\lambda_{0} and 0≤Cg0\le C_{g}, let ωg\omega_{g} be a modulus of continuity, and let g:V→Rg:V\to\mathbb{R} satisfy

∣g(x)∣≤Cgfor every x∈V,∣g(x)−g(y)∣≤ωg(∣x−y∣V)for all x,y∈V.|g(x)|\le C_{g}\quad\text{for every }x\in V,\qquad |g(x)-g(y)|\le\omega_{g}\bigl(|x-y|_{V}\bigr)\quad\text{for all }x,y\in V .

Let B:V→HB:V\to H be a monotone nonlinearity for (H,V,A)(H,V,A), let ℓ∈R\ell\in\mathbb{R} satisfy 0≤ℓ0\le\ell, and let L:H→HL:H\to H be Lipschitz with constant ℓ\ell from (H,dH)(H,d_{H}) to itself. Put cL=∣L(0H)∣Hc_{L}=|L(0_{H})|_{H}.

Let FF be the function on D(A)×R×H×Sym(V)D(A)\times\mathbb{R}\times H\times\mathrm{Sym}(V) whose value at (x,r,p,X)(x,r,p,X) is

F(x,r,p,X)=λ0 r+12∣p∣H2+⟨Ax+B(x)+L(x),p⟩H−g(x),F(x,r,p,X)=\lambda_{0}\,r+\tfrac{1}{2}|p|_{H}^{2}+\langle Ax+B(x)+L(x),p\rangle_{H}-g(x),

which is defined because x∈D(A)x\in D(A) gives x∈Vx\in V and Ax∈HAx\in H by Hilbert Triples: Standing Notation and Background (iii), whence B(x)∈HB(x)\in H and g(x)∈Rg(x)\in\mathbb{R}, and x∈Hx\in H by Hilbert Triples: Standing Notation and Background (i), whence L(x)∈HL(x)\in H. Then the following hold.

1. (An operator of first order) FF is a second-order equation operator on HH relative to (H,V,A)(H,V,A) and is first order; consequently FF is degenerate elliptic by A First-Order Equation Operator is Degenerate Elliptic and Its δ\delta-Shifts Ignore the Form Argument (i).

2. (Strict properness) For every positive R∈RR\in\mathbb{R}, λ0\lambda_{0} is a properness constant for FF at RR; in particular FF is locally strictly proper. No further restriction on λ0\lambda_{0} is imposed anywhere below.

3. (The structure condition) Let ωˉg\bar{\omega}_{g} be the nondecreasing envelope of ωg\omega_{g} truncated at M=2CgM=2C_{g}, which satisfies ωˉg(t)≤2Cg\bar{\omega}_{g}(t)\le2C_{g} for every nonnegative tt by The Nondecreasing Envelope of a Truncated Modulus of Continuity (ii), let ωg∗\omega_{g}^{\ast} be its quadratic reparametrisation at 2Cg2C_{g}, let ω1\omega_{1} be the function on the nonnegative reals with

ω1(t)=ωg∗(t)+ℓ t,\omega_{1}(t)=\omega_{g}^{\ast}(t)+\ell\,t,

and let ω2\omega_{2} be the function with value ω2(t,α)=Kα t\omega_{2}(t,\alpha)=K\alpha\,t at each pair (t,α)(t,\alpha) of real numbers with 0≤t0\le t and 1<α1<\alpha, where K=2+4cL2+4ℓ2K=2+4c_{L}^{2}+4\ell^{2}. Then ω1\omega_{1} is a modulus of continuity, for every real α>1\alpha>1 the function t↦ω2(t,α)t\mapsto\omega_{2}(t,\alpha) on the nonnegative reals is a modulus of continuity, and for every positive R∈RR\in\mathbb{R} the pair (ω1,ω2)(\omega_{1},\omega_{2}) is a structure pair for FF at RR; in particular FF satisfies the first-order structure condition.

4. (The shift-continuity condition) FF satisfies the shift-continuity condition.

5. (Comparison for this operator) Let u,v:H→Ru,v:H\to\mathbb{R} and C∈RC\in\mathbb{R} satisfy u(x)≤Cu(x)\le C and −C≤v(x)-C\le v(x) for every x∈Hx\in H, let uu be a viscosity subsolution of FF on HH and let vv be a viscosity supersolution of FF on HH. Then u(x)≤v(x)u(x)\le v(x) for every x∈Vx\in V.

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