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Proof of The Form Operator and the Riesz Map of a Diagonal Hilbert Triple

lemmalem:diagonal-hilbert-triple-2026a
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· 4,775 chars · 10 deps · depth 23 Reason: Proof of the new lemma describing the domain and action of the form operator, the eigenvectors, and the Riesz map of a diagonal Hilbert triple.

Testing the defining identity of the form operator against the basis vectors identifies the coefficients of the image, and the Riesz-Fischer criterion turns the resulting summability condition into a description of the domain; the Riesz map is then read off from the fact that it inverts the form operator.

Proof

Each result cited is universally quantified over the data in its own statement. Throughout, xk=x,ekHx_{k}=\langle x,e_{k}\rangle_{H} and likewise for other vectors of HH; by Orthonormal Expansions in a Real Hilbert Space §parseval the series k=1xk2\sum_{k=1}^{\infty}x_{k}^{2} converges with sum xH2|x|_{H}^{2} for every xHx\in H, and v,wH=k=1vkwk\langle v,w\rangle_{H}=\sum_{k=1}^{\infty}v_{k}w_{k} for all v,wHv,w\in H. By claim 1 of Elementary Arithmetic in an Ordered Field and transitivity each λk\lambda_{k} is positive. By orthonormality, ej,ekH\langle e_{j},e_{k}\rangle_{H} is 11 if k=jk=j and 00 otherwise, and by The Weighted Coefficient Subspace Determined by an Orthonormal Basis and a Sequence of Weights §subspace every eje_{j} lies in VV.

Claim 1. Suppose first that xD(A)x\in D(A) and put z=Axz=Ax, so that x,yV=z,yH\langle x,y\rangle_{V}=\langle z,y\rangle_{H} for every yVy\in V by Hilbert Triple: a Densely and Continuously Embedded Hilbert Space and Its Form Operator §operator. Taking y=ejy=e_{j} and using The Weighted Coefficient Subspace Determined by an Orthonormal Basis and a Sequence of Weights §coefficients gives

λjxj=x,ejV=z,ejH=zjfor every jN.\lambda_{j}x_{j}=\langle x,e_{j}\rangle_{V}=\langle z,e_{j}\rangle_{H}=z_{j}\qquad\text{for every }j\in\mathbb{N}.

Hence λj2xj2=zj2\lambda_{j}^{2}x_{j}^{2}=z_{j}^{2} for every jj, and the series k=1zk2\sum_{k=1}^{\infty}z_{k}^{2} converges, so k=1λk2xk2\sum_{k=1}^{\infty}\lambda_{k}^{2}x_{k}^{2} converges. Moreover Orthonormal Expansions in a Real Hilbert Space §expansion gives z=k=1zkek=k=1λkxkekz=\sum_{k=1}^{\infty}z_{k}e_{k}=\sum_{k=1}^{\infty}\lambda_{k}x_{k}e_{k}, the two series having the same terms.

Conversely, suppose xHx\in H and the series k=1λk2xk2\sum_{k=1}^{\infty}\lambda_{k}^{2}x_{k}^{2} converges. Multiplying 1λk1\le\lambda_{k} by the nonnegative number λkxk2\lambda_{k}x_{k}^{2}, using claim 5 of Elementary Arithmetic in an Ordered Field, gives 0λkxk2λk2xk20\le\lambda_{k}x_{k}^{2}\le\lambda_{k}^{2}x_{k}^{2} for every kk, so k=1λkxk2\sum_{k=1}^{\infty}\lambda_{k}x_{k}^{2} converges by Series of Nonnegative Real Numbers, Comparison, and the Geometric Series §comparison and xVx\in V. By Orthonormal Expansions in a Real Hilbert Space §riesz-fischer applied to the coefficients λkxk\lambda_{k}x_{k}, the series k=1λkxkek\sum_{k=1}^{\infty}\lambda_{k}x_{k}e_{k} converges in HH; write zz for its sum, so that zj=λjxjz_{j}=\lambda_{j}x_{j} for every jj. For yVy\in V the series k=1zkyk\sum_{k=1}^{\infty}z_{k}y_{k} and k=1λkxkyk\sum_{k=1}^{\infty}\lambda_{k}x_{k}y_{k} have the same terms and converge, the first with sum z,yH\langle z,y\rangle_{H} and the second with sum x,yV\langle x,y\rangle_{V} by The Weighted Coefficient Subspace Determined by an Orthonormal Basis and a Sequence of Weights §subspace. Hence x,yV=z,yH\langle x,y\rangle_{V}=\langle z,y\rangle_{H} for every yVy\in V, so xD(A)x\in D(A) and Ax=zAx=z by Hilbert Triple: a Densely and Continuously Embedded Hilbert Space and Its Form Operator §operator.

Claim 2. Fix jNj\in\mathbb{N}. The terms of k=1λk2ej,ekH2\sum_{k=1}^{\infty}\lambda_{k}^{2}\langle e_{j},e_{k}\rangle_{H}^{2} vanish for kjk\ne j and equal λj2\lambda_{j}^{2} for k=jk=j, so by claim 7 of Properties of Finite Sums every partial sum with jnj\le n equals λj2\lambda_{j}^{2}; such a sequence converges to λj2\lambda_{j}^{2}, since for a positive ε\varepsilon every such nn gives a difference of absolute value 0<ε0<\varepsilon. So the series converges and ejD(A)e_{j}\in D(A) by claim 1. By claim 1 again, AejAe_{j} is the sum of the series k=1λkej,ekHek\sum_{k=1}^{\infty}\lambda_{k}\langle e_{j},e_{k}\rangle_{H}e_{k}, whose terms vanish for kjk\ne j and equal λjej\lambda_{j}e_{j} for k=jk=j; by claim 7 of Properties of Finite Sums of Vectors every partial sum with jnj\le n equals λjej\lambda_{j}e_{j}, and the same argument gives Aej=λjejAe_{j}=\lambda_{j}e_{j}.

Claim 3. Let zHz\in H and put ck=1λkzkc_{k}=\tfrac{1}{\lambda_{k}}z_{k}. Multiplying 1λk1\le\lambda_{k} by the positive number 1λk\tfrac{1}{\lambda_{k}}, using claim 5 of Elementary Arithmetic in an Ordered Field, gives 0<1λk10<\tfrac{1}{\lambda_{k}}\le1, whence (1λk)21(\tfrac{1}{\lambda_{k}})^{2}\le1 by claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field and 0ck2zk20\le c_{k}^{2}\le z_{k}^{2} by claim 5 of Elementary Arithmetic in an Ordered Field. Since k=1zk2\sum_{k=1}^{\infty}z_{k}^{2} converges, Series of Nonnegative Real Numbers, Comparison, and the Geometric Series §comparison shows that k=1ck2\sum_{k=1}^{\infty}c_{k}^{2} converges, and Orthonormal Expansions in a Real Hilbert Space §riesz-fischer shows that the series k=1ckek\sum_{k=1}^{\infty}c_{k}e_{k} converges in HH; write xx for its sum, so that xk=ckx_{k}=c_{k} for every kk.

Then λk2xk2=zk2\lambda_{k}^{2}x_{k}^{2}=z_{k}^{2} for every kk, so k=1λk2xk2\sum_{k=1}^{\infty}\lambda_{k}^{2}x_{k}^{2} converges and claim 1 gives xD(A)x\in D(A) with Ax=k=1λkxkek=k=1zkek=zAx=\sum_{k=1}^{\infty}\lambda_{k}x_{k}e_{k}=\sum_{k=1}^{\infty}z_{k}e_{k}=z, the last equality by Orthonormal Expansions in a Real Hilbert Space §expansion. By Elementary Properties of a Hilbert Triple: the Embedding, the Riesz Map and the Form Operator §range the Riesz map satisfies J(Ax)=xJ(Ax)=x for every xD(A)x\in D(A), so Jz=J(Ax)=xJz=J(Ax)=x, which is the asserted identity.

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