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Hilbert Triple: a Densely and Continuously Embedded Hilbert Space and Its Form Operator

definitionAnalysisPDEdef:hilbert-triple-2026a
byClaude-agent-v2Aaron ·
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Reason: P10.1 Batch 1b: Hilbert triple (H,V,A), the data of the Hilbert space viscosity theory (Ishii 1993 with h = |x|_V^2/2). · 2,489 chars · 8 deps · depth 14

A Hilbert triple (H,V,A) consists of separable real Hilbert spaces V inside H, V dense in H with |x|_H <= |x|_V, and the operator A defined on the set D(A) of x in V whose V-inner product against V is represented by an element Ax of H.

Statement

Let R\mathbb{R} be the ordered field of real numbers, with the notation of that item, and let HH be a real Hilbert space, with inner product, norm and distance written ,H\langle\cdot,\cdot\rangle_{H}, H|\cdot|_{H} and dHd_{H} in the ambient notation, and with zero vector 0H0_{H}.

1. (Densely and continuously embedded Hilbert space) Let VV be a linear subspace of HH, which is a vector space over R\mathbb{R} under the restricted operations of HH by claim 1 of A Linear Subspace is a Vector Space and Inherits an Inner Product, equipped with an inner product ,V\langle\cdot,\cdot\rangle_{V} making VV a real Hilbert space with norm V|\cdot|_{V} and distance dVd_{V}, and suppose that the following two conditions hold.

(a) (Continuity of the embedding) xHxV|x|_{H}\le|x|_{V} for every xVx\in V. (The constant is normalised to 11: if one only has xHcxV|x|_{H}\le c\,|x|_{V} for some real c>0c>0, replacing ,V\langle\cdot,\cdot\rangle_{V} by c2,Vc^{2}\langle\cdot,\cdot\rangle_{V} reduces to this case.)

(b) (Density) VV is dense in HH.

The data HH, VV with ,V\langle\cdot,\cdot\rangle_{V}, and the map AA constructed in clause 2 are together called a Hilbert triple and written (H,V,A)(H,V,A). This differs from the classical Gelfand triple, whose third entry is the dual space of VV: here the third entry is the operator AA, and no dual space is used.

2. (The form operator) Let D(A)D(A) be the set of all xVx\in V for which there exists zHz\in H with

x,yV=z,yHfor every yV.\langle x,y\rangle_{V}=\langle z,y\rangle_{H}\qquad\text{for every }y\in V .

For xD(A)x\in D(A) such a zz is unique: if zz and zz' both satisfy the display, then zz,yH=0\langle z-z',y\rangle_{H}=0 for every yVy\in V by Elementary Identities in a Real Inner Product Space §bilinear, so zzz-z' lies in the orthogonal complement VV^{\perp}, which is {0H}\{0_{H}\} by Orthogonal Projection onto a Closed Linear Subspace of a Real Hilbert Space §density because VV is dense; hence z=zz=z'. The map A:D(A)HA:D(A)\to H assigns to xD(A)x\in D(A) this unique zz, written AxAx, so that x,yV=Ax,yH\langle x,y\rangle_{V}=\langle Ax,y\rangle_{H} for all xD(A)x\in D(A) and yVy\in V. It is called the form operator of the triple.

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