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Proof of The Dissipative Hamilton-Jacobi Operator on a Hilbert Triple Satisfies the Comparison Hypotheses

propositionprop:dissipative-hamilton-jacobi-hilbert-triple-2026a
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· 9,529 chars · 11 deps · depth 27 Reason: Initial publication of the proof: verification of the three comparison hypotheses for the dissipative Hamilton-Jacobi operator, including the bound on the form operator over the admissible sets.

Properness is exact; the structure condition follows from the monotonicity identity for the form operator together with two completions of squares; and on the admissible sets the quadratic term in the shifted operator bounds the norm of Ax, which yields an explicit shift modulus.

Proof

Each result cited is universally quantified over the data in its own statement. Throughout, a+bH2=aH2+2a,bH+bH2|a+b|_{H}^{2}=|a|_{H}^{2}+2\langle a,b\rangle_{H}+|b|_{H}^{2} for a,bHa,b\in H by Elementary Identities in a Real Inner Product Space §expansion, and a,bHaHbH|\langle a,b\rangle_{H}|\le|a|_{H}|b|_{H} by The Cauchy-Schwarz Inequality in a Real Inner Product Space. We record one identity: for x,yD(A)x,y\in D(A),

AxAy,xyH=xyV2,(1)\langle Ax-Ay,\,x-y\rangle_{H}=|x-y|_{V}^{2}, \tag{1}

since xyVx-y\in V, so that Ax,xyH=x,xyV\langle Ax,x-y\rangle_{H}=\langle x,x-y\rangle_{V} and Ay,xyH=y,xyV\langle Ay,x-y\rangle_{H}=\langle y,x-y\rangle_{V} by Hilbert Triples: Standing Notation and Background §operator, and subtracting gives xy,xyV\langle x-y,x-y\rangle_{V}.

Claim 1. Each of λ0r\lambda_{0}r, 12pH2\tfrac12|p|_{H}^{2}, Ax,pH\langle Ax,p\rangle_{H} and g(x)g(x) is a real number for (x,r,p,X)D(A)×R×H×Sym(V)(x,r,p,X)\in D(A)\times\mathbb{R}\times H\times\mathrm{Sym}(V), so FF is a function from D(A)×R×H×Sym(V)D(A)\times\mathbb{R}\times H\times\mathrm{Sym}(V) to R\mathbb{R}. Since W=D(A)H=D(A)W=D(A)\cap H=D(A), this is exactly the shape required by Second-Order Equation Operator on an Open Subset of a Hilbert Triple and Its δ\delta-Shifts §operator. The defining expression does not involve the fourth argument, so F(x,r,p,X)=F(x,r,p,X)F(x,r,p,X)=F(x,r,p,X') for all X,XSym(V)X,X'\in\mathrm{Sym}(V), i.e. FF is first order; degenerate ellipticity follows from A First-Order Equation Operator is Degenerate Elliptic and Its δ\delta-Shifts Ignore the Form Argument §elliptic.

Claim 2. Let RR be positive, let xD(A)x\in D(A), pHp\in H, XSym(V)X\in\mathrm{Sym}(V) and let r,sRr,s\in\mathbb{R} satisfy RsrR-R\le s\le r\le R. All terms of FF other than λ0r\lambda_{0}r are unchanged when rr is replaced by ss, so

F(x,r,p,X)F(x,s,p,X)=λ0(rs),F(x,r,p,X)-F(x,s,p,X)=\lambda_{0}(r-s),

and in particular λ0(rs)F(x,r,p,X)F(x,s,p,X)\lambda_{0}(r-s)\le F(x,r,p,X)-F(x,s,p,X). Thus λ0\lambda_{0} is a properness constant for FF at RR, for every positive RR, and FF is locally strictly proper.

Claim 3. The function ω2\omega_{2} is a modulus of continuity, both conditions of Modulus of Continuity holding trivially. So is ω3\omega_{3}: its values 34t\tfrac34t are nonnegative for t0t\ge0, and for positive ϵ\epsilon every tt with 0tϵ0\le t\le\epsilon satisfies 34tϵ\tfrac34 t\le\epsilon.

Let RR be positive, let x,yD(A)x,y\in D(A), rRr\in\mathbb{R}, X,YSym(H)X,Y\in\mathrm{Sym}(H) and let α,δ\alpha,\delta satisfy 1<α1<\alpha and 0<δ<10<\delta<1; put P=α(xy)P=\alpha(x-y). By Second-Order Equation Operator on an Open Subset of a Hilbert Triple and Its δ\delta-Shifts §shifted and the expansion of the norm,

Fδ(x,r,P,X)=λ0r+λ0δh(x)+12PH2+δP,AxH+δ22AxH2+Ax,PH+δAxH2g(x),F^{-}_{\delta}(x,r,P,X)=\lambda_{0}r+\lambda_{0}\delta h(x)+\tfrac12|P|_{H}^{2}+\delta\langle P,Ax\rangle_{H}+\tfrac{\delta^{2}}{2}|Ax|_{H}^{2}+\langle Ax,P\rangle_{H}+\delta|Ax|_{H}^{2}-g(x), Fδ+(y,r,P,Y)=λ0rλ0δh(y)+12PH2δP,AyH+δ22AyH2+Ay,PHδAyH2g(y).F^{+}_{\delta}(y,r,P,Y)=\lambda_{0}r-\lambda_{0}\delta h(y)+\tfrac12|P|_{H}^{2}-\delta\langle P,Ay\rangle_{H}+\tfrac{\delta^{2}}{2}|Ay|_{H}^{2}+\langle Ay,P\rangle_{H}-\delta|Ay|_{H}^{2}-g(y).

Subtracting and using (1) in the form Ax,PHAy,PH=αxyV2\langle Ax,P\rangle_{H}-\langle Ay,P\rangle_{H}=\alpha|x-y|_{V}^{2},

Fδ(x,r,P,X)Fδ+(y,r,P,Y)=λ0δ(h(x)+h(y))+αxyV2+Tx+Ty+g(y)g(x),F^{-}_{\delta}(x,r,P,X)-F^{+}_{\delta}(y,r,P,Y)=\lambda_{0}\delta\bigl(h(x)+h(y)\bigr)+\alpha|x-y|_{V}^{2}+T_{x}+T_{y}+g(y)-g(x),

where

Tx=δAxH2+δ22AxH2+δP,AxH,Ty=δAyH2δ22AyH2+δP,AyH.T_{x}=\delta|Ax|_{H}^{2}+\tfrac{\delta^{2}}{2}|Ax|_{H}^{2}+\delta\langle P,Ax\rangle_{H},\qquad T_{y}=\delta|Ay|_{H}^{2}-\tfrac{\delta^{2}}{2}|Ay|_{H}^{2}+\delta\langle P,Ay\rangle_{H}.

Since δ22AxH20\tfrac{\delta^{2}}{2}|Ax|_{H}^{2}\ge0 and δP,AxHδPHAxH\delta\langle P,Ax\rangle_{H}\ge-\delta|P|_{H}|Ax|_{H}, while δ(AxHPH2)20\delta\bigl(|Ax|_{H}-\tfrac{|P|_{H}}{2}\bigr)^{2}\ge0 gives δAxH2δPHAxHδ4PH2\delta|Ax|_{H}^{2}-\delta|P|_{H}|Ax|_{H}\ge-\tfrac{\delta}{4}|P|_{H}^{2}, we get Txδ4PH2T_{x}\ge-\tfrac{\delta}{4}|P|_{H}^{2}. Since δ1\delta\le1 we have δδ22δ2\delta-\tfrac{\delta^{2}}{2}\ge\tfrac{\delta}{2}, and δ2(AyHPH)20\tfrac{\delta}{2}\bigl(|Ay|_{H}-|P|_{H}\bigr)^{2}\ge0 gives δ2AyH2δPHAyHδ2PH2\tfrac{\delta}{2}|Ay|_{H}^{2}-\delta|P|_{H}|Ay|_{H}\ge-\tfrac{\delta}{2}|P|_{H}^{2}, so Tyδ2PH2T_{y}\ge-\tfrac{\delta}{2}|P|_{H}^{2}. Moreover h(x)+h(y)0h(x)+h(y)\ge0 by The Penalty Function h=12V2h=\tfrac12|\cdot|_V^2 of a Hilbert Triple: Expansion Identities, Closed Sublevel Sets, Density and Local Bounds §nonneg together with claim 2 of Elementary Arithmetic in an Ordered Field, αxyV20\alpha|x-y|_{V}^{2}\ge0, and g(y)g(x)g(x)g(y)ωg(xyH)g(y)-g(x)\ge-|g(x)-g(y)|\ge-\omega_{g}\bigl(|x-y|_{H}\bigr) by hypothesis. Since PH2=α2xyH2|P|_{H}^{2}=\alpha^{2}|x-y|_{H}^{2}, we conclude

Fδ(x,r,P,X)Fδ+(y,r,P,Y)  ωg(xyH)34δα2xyH2=ωg(xyH)ω2(αxyH2)ω3(δα2xyH2).F^{-}_{\delta}(x,r,P,X)-F^{+}_{\delta}(y,r,P,Y)\ \ge\ -\omega_{g}\bigl(|x-y|_{H}\bigr)-\tfrac{3}{4}\delta\alpha^{2}|x-y|_{H}^{2}=-\omega_{g}\bigl(|x-y|_{H}\bigr)-\omega_{2}\bigl(\alpha|x-y|_{H}^{2}\bigr)-\omega_{3}\bigl(\delta\alpha^{2}|x-y|_{H}^{2}\bigr).

No restriction on rr was used, so (ωg,ω2,ω3)(\omega_{g},\omega_{2},\omega_{3}) is a structure triple for FF at every positive RR.

Claim 4. Let δ,R\delta,R satisfy 0<δ<10<\delta<1 and 0<R0<R. Recall from Test Data for a Second-Order Equation Operator on a Hilbert Triple and the Admissible Sets §bounded that an RR-bounded datum (x,r,p,X)(x,r,p,X) satisfies h(x)<Rh(x)<R, r<R|r|<R and pH<R|p|_{H}<R.

(a) An upper bound for Fδ+F^{+}_{\delta}. For RR-bounded η=(y,s,p,X)\eta=(y,s,p',X'), expanding as above,

Fδ+(η)=λ0sλ0δh(y)+12pH2δp,AyH+δ22AyH2+Ay,pHδAyH2g(y).F^{+}_{\delta}(\eta)=\lambda_{0}s-\lambda_{0}\delta h(y)+\tfrac12|p'|_{H}^{2}-\delta\langle p',Ay\rangle_{H}+\tfrac{\delta^{2}}{2}|Ay|_{H}^{2}+\langle Ay,p'\rangle_{H}-\delta|Ay|_{H}^{2}-g(y).

Here λ0sλ0R\lambda_{0}s\le\lambda_{0}R, λ0δh(y)0-\lambda_{0}\delta h(y)\le0, 12pH212R2\tfrac12|p'|_{H}^{2}\le\tfrac12R^{2}, δp,AyHRAyH-\delta\langle p',Ay\rangle_{H}\le R|Ay|_{H}, Ay,pHRAyH\langle Ay,p'\rangle_{H}\le R|Ay|_{H}, δ22AyH2δAyH2δ2AyH2\tfrac{\delta^{2}}{2}|Ay|_{H}^{2}-\delta|Ay|_{H}^{2}\le-\tfrac{\delta}{2}|Ay|_{H}^{2} and g(y)Cg-g(y)\le C_{g}, so

Fδ+(η)λ0R+12R2+Cg+2RAyHδ2AyH2.(2)F^{+}_{\delta}(\eta)\le\lambda_{0}R+\tfrac12R^{2}+C_{g}+2R|Ay|_{H}-\tfrac{\delta}{2}|Ay|_{H}^{2}. \tag{2}

Since δ2(AyH2Rδ)20\tfrac{\delta}{2}\bigl(|Ay|_{H}-\tfrac{2R}{\delta}\bigr)^{2}\ge0 gives 2RAyHδ2AyH22R2δ2R|Ay|_{H}-\tfrac{\delta}{2}|Ay|_{H}^{2}\le\tfrac{2R^{2}}{\delta}, we obtain Fδ+(η)ΣF^{+}_{\delta}(\eta)\le\Sigma, where Σ=λ0R+12R2+Cg+2R2δ\Sigma=\lambda_{0}R+\tfrac12R^{2}+C_{g}+\tfrac{2R^{2}}{\delta}.

(b) A lower bound for FδF^{-}_{\delta}. For RR-bounded ξ=(x,r,p,X)\xi=(x,r,p,X), in the same way,

Fδ(ξ)  λ0RRAxHRAxH+δAxH2Cg=δAxH22RAxHλ0RCg,(3)F^{-}_{\delta}(\xi)\ \ge\ -\lambda_{0}R-R|Ax|_{H}-R|Ax|_{H}+\delta|Ax|_{H}^{2}-C_{g}=\delta|Ax|_{H}^{2}-2R|Ax|_{H}-\lambda_{0}R-C_{g}, \tag{3}

using λ0δh(x)0\lambda_{0}\delta h(x)\ge0, 12pH20\tfrac12|p|_{H}^{2}\ge0 and δ22AxH20\tfrac{\delta^{2}}{2}|Ax|_{H}^{2}\ge0. Since δ(AxHRδ)20\delta\bigl(|Ax|_{H}-\tfrac{R}{\delta}\bigr)^{2}\ge0 gives δAxH22RAxHR2δ\delta|Ax|_{H}^{2}-2R|Ax|_{H}\ge-\tfrac{R^{2}}{\delta}, we obtain Fδ(ξ)ΞF^{-}_{\delta}(\xi)\ge\Xi, where Ξ=R2δλ0RCg\Xi=-\tfrac{R^{2}}{\delta}-\lambda_{0}R-C_{g}.

(c) A bound on AxH|Ax|_{H} for admissible data. Let ξ=(x,r,p,X)Sδ,R\xi=(x,r,p,X)\in S^{-}_{\delta,R}. By Test Data for a Second-Order Equation Operator on a Hilbert Triple and the Admissible Sets §admissible there is an RR-bounded η\eta with Fδ(ξ)<R+Fδ+(η)R+ΣF^{-}_{\delta}(\xi)<R+F^{+}_{\delta}(\eta)\le R+\Sigma, so by (3)

δAxH22RAxHK,K=R+Σ+λ0R+Cg  (0).\delta|Ax|_{H}^{2}-2R|Ax|_{H}\le K,\qquad K=R+\Sigma+\lambda_{0}R+C_{g}\ \ (\ge0).

As 2RAxHδ2AxH2+2R2δ2R|Ax|_{H}\le\tfrac{\delta}{2}|Ax|_{H}^{2}+\tfrac{2R^{2}}{\delta}, this gives δ2AxH2K+2R2δ\tfrac{\delta}{2}|Ax|_{H}^{2}\le K+\tfrac{2R^{2}}{\delta}, so AxHΛ1|Ax|_{H}\le\Lambda_{1}, the nonnegative square root of 2δ(K+2R2δ)\tfrac{2}{\delta}\bigl(K+\tfrac{2R^{2}}{\delta}\bigr).

Let now η=(y,s,p,X)Sδ,R+\eta=(y,s,p',X')\in S^{+}_{\delta,R}. There is an RR-bounded ξ\xi with Fδ+(η)>Fδ(ξ)RΞRF^{+}_{\delta}(\eta)>F^{-}_{\delta}(\xi)-R\ge\Xi-R, so by (2)

δ2AyH22RAyHK,K=λ0R+12R2+CgΞ+R  (0),\tfrac{\delta}{2}|Ay|_{H}^{2}-2R|Ay|_{H}\le K',\qquad K'=\lambda_{0}R+\tfrac12R^{2}+C_{g}-\Xi+R\ \ (\ge0),

and since 2RAyHδ4AyH2+4R2δ2R|Ay|_{H}\le\tfrac{\delta}{4}|Ay|_{H}^{2}+\tfrac{4R^{2}}{\delta} we get AyHΛ2|Ay|_{H}\le\Lambda_{2}, the nonnegative square root of 4δ(K+4R2δ)\tfrac{4}{\delta}\bigl(K'+\tfrac{4R^{2}}{\delta}\bigr).

(d) The shift modulus. Put Λ=Λ1+Λ2\Lambda=\Lambda_{1}+\Lambda_{2}, c=R+2Λc=R+2\Lambda and let ω\omega have value ct+12t2ct+\tfrac12t^{2} at a nonnegative tt. Then ω\omega is a modulus of continuity: its values are nonnegative, and for positive ϵ\epsilon every tt with 0tτ0\le t\le\tau, where τ\tau is the smaller of 11 and ϵc+1\tfrac{\epsilon}{c+1}, satisfies 12t212t\tfrac12t^{2}\le\tfrac12 t and hence ω(t)(c+1)tϵ\omega(t)\le(c+1)t\le\epsilon. Note also that ω\omega is nondecreasing on the nonnegative reals, since c0c\ge0.

Let qHq\in H and YSym(H)Y\in\mathrm{Sym}(H). For ξ=(x,r,p,X)Sδ,R\xi=(x,r,p,X)\in S^{-}_{\delta,R} we have Fδ(x,r,p+q,X+Y)=Fδ(x,r,p+q,X)F^{-}_{\delta}(x,r,p+q,X+Y)=F^{-}_{\delta}(x,r,p+q,X) by A First-Order Equation Operator is Degenerate Elliptic and Its δ\delta-Shifts Ignore the Form Argument §shifts and claim 1, and, expanding the norm,

Fδ(x,r,p+q,X)Fδ(x,r,p,X)=p+δAx,qH+12qH2+Ax,qH  (R+Λ+Λ)qH+12qH2=ω(qH),F^{-}_{\delta}(x,r,p+q,X)-F^{-}_{\delta}(x,r,p,X)=\langle p+\delta Ax,q\rangle_{H}+\tfrac12|q|_{H}^{2}+\langle Ax,q\rangle_{H}\ \le\ \bigl(R+\Lambda+\Lambda\bigr)|q|_{H}+\tfrac12|q|_{H}^{2}=\omega\bigl(|q|_{H}\bigr),

using pH<R|p|_{H}<R, δ<1\delta<1 and AxHΛ1Λ|Ax|_{H}\le\Lambda_{1}\le\Lambda. Since ω\omega is nondecreasing, ω(qH)ω(qH+Y)\omega(|q|_{H})\le\omega\bigl(|q|_{H}+\lVert Y\rVert\bigr), which is the first condition of The Shift-Continuity Condition on Admissible Test Data §modulus.

For η=(y,s,p,X)Sδ,R+\eta=(y,s,p',X')\in S^{+}_{\delta,R} we have Fδ+(y,s,p+q,X+Y)=Fδ+(y,s,p+q,X)F^{+}_{\delta}(y,s,p'+q,X'+Y)=F^{+}_{\delta}(y,s,p'+q,X'), again by A First-Order Equation Operator is Degenerate Elliptic and Its δ\delta-Shifts Ignore the Form Argument §shifts and claim 1, and the same computation gives

Fδ+(y,s,p+q,X+Y)Fδ+(y,s,p,X)=pδAy,qH+12qH2+Ay,qH  (R+Λ+Λ)qH  ω(qH+Y),F^{+}_{\delta}(y,s,p'+q,X'+Y)-F^{+}_{\delta}(y,s,p',X')=\langle p'-\delta Ay,q\rangle_{H}+\tfrac12|q|_{H}^{2}+\langle Ay,q\rangle_{H}\ \ge\ -\bigl(R+\Lambda+\Lambda\bigr)|q|_{H}\ \ge\ -\omega\bigl(|q|_{H}+\lVert Y\rVert\bigr),

using 12qH20\tfrac12|q|_{H}^{2}\ge0 and AyHΛ2Λ|Ay|_{H}\le\Lambda_{2}\le\Lambda. Hence ω\omega is a shift modulus for FF at (δ,R)(\delta,R), and as δ\delta and RR were arbitrary, FF satisfies the shift-continuity condition.

Claim 5. By claims 1 to 4 the operator FF satisfies all hypotheses on the operator in A Comparison Principle on a Hilbert Triple under the First-Order Structure Condition, and uu, vv, CC satisfy the remaining ones, so A Comparison Principle on a Hilbert Triple under the First-Order Structure Condition §comparison gives u(x)v(x)u(x)\le v(x) for every xVx\in V.

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