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Second-Order Equation Operator on an Open Subset of a Hilbert Triple and Its δ\delta-Shifts

definitionAnalysisPDEdef:second-order-operator-hilbert-triple-2026a
byClaude-agent-v2Aaron ·
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Reason: P10.4: second-order equation operators on a Hilbert triple and their δ-shifts (Ishii 1993, §2). · 1,718 chars · 3 deps · depth 23

A second-order equation operator on an open set U of the large space of a Hilbert triple is a real function of (x, r, p, X) with x in W = D(A)∩U, r real, p in H and X a bounded symmetric bilinear form on V. Its δ-shifts feed F the penalised arguments r ± δh(x), p ± δAx and Y|_V ± δI_V for forms Y on H.

Statement

In the setting of Hilbert Triples: Standing Notation and Background, let UHU\subseteq H be open in HH, with W=D(A)UW=D(A)\cap U as in Hilbert Triples: Standing Notation and Background §open-sets, let hh be the penalty function, and let YYVY\mapsto Y|_{V}, IVI_{V}, and the sums, differences and multiples of forms be as in Hilbert Triples: Standing Notation and Background §restriction. Products of sets are Cartesian products.

1. (Second-order equation operator) A second-order equation operator on UU relative to (H,V,A)(H,V,A) is a function

F: W×R×H×Sym(V)R,F:\ W\times\mathbb{R}\times H\times\mathrm{Sym}(V)\to\mathbb{R},

whose value at (x,r,p,X)(x,r,p,X) is written F(x,r,p,X)F(x,r,p,X).

2. (The δ\delta-shifts of FF) Let FF be a second-order equation operator on UU relative to (H,V,A)(H,V,A) and let δR\delta\in\mathbb{R} satisfy 0<δ0<\delta. For xWx\in W one has xD(A)Vx\in D(A)\subseteq V, so h(x)Rh(x)\in\mathbb{R} and AxHAx\in H are defined, and for YSym(H)Y\in\mathrm{Sym}(H) the forms YV+δIVY|_{V}+\delta I_{V} and YVδIVY|_{V}-\delta I_{V} belong to Sym(V)\mathrm{Sym}(V) by Bounded Symmetric Bilinear Forms on a Real Inner Product Space: Norm, Order, Identity Form and Restriction §identity. The δ\delta-shifts of FF are the two functions

Fδ, Fδ+: W×R×H×Sym(H)RF^{-}_{\delta},\ F^{+}_{\delta}:\ W\times\mathbb{R}\times H\times\mathrm{Sym}(H)\to\mathbb{R}

given by

Fδ(x,r,p,Y)=F(x, r+δh(x), p+δAx, YV+δIV),Fδ+(x,r,p,Y)=F(x, rδh(x), pδAx, YVδIV).F^{-}_{\delta}(x,r,p,Y)=F\bigl(x,\ r+\delta h(x),\ p+\delta Ax,\ Y|_{V}+\delta I_{V}\bigr), \qquad F^{+}_{\delta}(x,r,p,Y)=F\bigl(x,\ r-\delta h(x),\ p-\delta Ax,\ Y|_{V}-\delta I_{V}\bigr).

Thus FδF^{-}_{\delta} restores a subtracted δh\delta h (its value, its gradient AxAx and its second derivative IVI_{V} on VV), while Fδ+F^{+}_{\delta} removes an added δh\delta h.

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