TheoremBase

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,ek⟩Hx_{k}=\langle x,e_{k}\rangle_{H} and likewise for other vectors of HH; by Orthonormal Expansions in a Real Hilbert Space (iv) the series βˆ‘k=1∞xk2\sum_{k=1}^{\infty}x_{k}^{2} converges with sum ∣x∣H2|x|_{H}^{2} for every x∈Hx\in H, and ⟨v,w⟩H=βˆ‘k=1∞vkwk\langle v,w\rangle_{H}=\sum_{k=1}^{\infty}v_{k}w_{k} for all v,w∈Hv,w\in H. By claim 1 of Elementary Arithmetic in an Ordered Field and transitivity each Ξ»k\lambda_{k} is positive. By orthonormality, ⟨ej,ek⟩H\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 (i) every eje_{j} lies in VV.

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

λjxj=⟨x,ej⟩V=⟨z,ej⟩H=zjfor every j∈N.\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 Ξ»j2xj2=zj2\lambda_{j}^{2}x_{j}^{2}=z_{j}^{2} for every jj, and the series βˆ‘k=1∞zk2\sum_{k=1}^{\infty}z_{k}^{2} converges, so βˆ‘k=1∞λk2xk2\sum_{k=1}^{\infty}\lambda_{k}^{2}x_{k}^{2} converges. Moreover Orthonormal Expansions in a Real Hilbert Space (iii) gives z=βˆ‘k=1∞zkek=βˆ‘k=1∞λkxkekz=\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 x∈Hx\in H and the series βˆ‘k=1∞λk2xk2\sum_{k=1}^{\infty}\lambda_{k}^{2}x_{k}^{2} converges. Multiplying 1≀λk1\le\lambda_{k} by the nonnegative number Ξ»kxk2\lambda_{k}x_{k}^{2}, using claim 5 of Elementary Arithmetic in an Ordered Field, gives 0≀λkxk2≀λk2xk20\le\lambda_{k}x_{k}^{2}\le\lambda_{k}^{2}x_{k}^{2} for every kk, so βˆ‘k=1∞λkxk2\sum_{k=1}^{\infty}\lambda_{k}x_{k}^{2} converges by Series of Nonnegative Real Numbers, Comparison, and the Geometric Series (iii) and x∈Vx\in V. By Orthonormal Expansions in a Real Hilbert Space (ii) applied to the coefficients Ξ»kxk\lambda_{k}x_{k}, the series βˆ‘k=1∞λkxkek\sum_{k=1}^{\infty}\lambda_{k}x_{k}e_{k} converges in HH; write zz for its sum, so that zj=Ξ»jxjz_{j}=\lambda_{j}x_{j} for every jj. For y∈Vy\in V the series βˆ‘k=1∞zkyk\sum_{k=1}^{\infty}z_{k}y_{k} and βˆ‘k=1∞λkxkyk\sum_{k=1}^{\infty}\lambda_{k}x_{k}y_{k} have the same terms and converge, the first with sum ⟨z,y⟩H\langle z,y\rangle_{H} and the second with sum ⟨x,y⟩V\langle x,y\rangle_{V} by The Weighted Coefficient Subspace Determined by an Orthonormal Basis and a Sequence of Weights (i). Hence ⟨x,y⟩V=⟨z,y⟩H\langle x,y\rangle_{V}=\langle z,y\rangle_{H} for every y∈Vy\in V, so x∈D(A)x\in D(A) and Ax=zAx=z by Hilbert Triple: a Densely and Continuously Embedded Hilbert Space and Its Form Operator (iv).

Claim 2. Fix j∈Nj\in\mathbb{N}. The terms of βˆ‘k=1∞λk2⟨ej,ek⟩H2\sum_{k=1}^{\infty}\lambda_{k}^{2}\langle e_{j},e_{k}\rangle_{H}^{2} vanish for kβ‰ jk\ne j and equal Ξ»j2\lambda_{j}^{2} for k=jk=j, so by claim 7 of Properties of Finite Sums every partial sum with j≀nj\le n equals Ξ»j2\lambda_{j}^{2}; such a sequence converges to Ξ»j2\lambda_{j}^{2}, since for a positive Ξ΅\varepsilon every such nn gives a difference of absolute value 0<Ξ΅0<\varepsilon. So the series converges and ej∈D(A)e_{j}\in D(A) by claim 1. By claim 1 again, AejAe_{j} is the sum of the series βˆ‘k=1∞λk⟨ej,ek⟩Hek\sum_{k=1}^{\infty}\lambda_{k}\langle e_{j},e_{k}\rangle_{H}e_{k}, whose terms vanish for kβ‰ jk\ne j and equal Ξ»jej\lambda_{j}e_{j} for k=jk=j; by claim 7 of Properties of Finite Sums of Vectors every partial sum with j≀nj\le n equals Ξ»jej\lambda_{j}e_{j}, and the same argument gives Aej=Ξ»jejAe_{j}=\lambda_{j}e_{j}.

Claim 3. Let z∈Hz\in H and put ck=1Ξ»kzkc_{k}=\tfrac{1}{\lambda_{k}}z_{k}. Multiplying 1≀λk1\le\lambda_{k} by the positive number 1Ξ»k\tfrac{1}{\lambda_{k}}, using claim 5 of Elementary Arithmetic in an Ordered Field, gives 0<1Ξ»k≀10<\tfrac{1}{\lambda_{k}}\le1, whence (1Ξ»k)2≀1(\tfrac{1}{\lambda_{k}})^{2}\le1 by claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field and 0≀ck2≀zk20\le c_{k}^{2}\le z_{k}^{2} by claim 5 of Elementary Arithmetic in an Ordered Field. Since βˆ‘k=1∞zk2\sum_{k=1}^{\infty}z_{k}^{2} converges, Series of Nonnegative Real Numbers, Comparison, and the Geometric Series (iii) shows that βˆ‘k=1∞ck2\sum_{k=1}^{\infty}c_{k}^{2} converges, and Orthonormal Expansions in a Real Hilbert Space (ii) shows that the series βˆ‘k=1∞ckek\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 Ξ»k2xk2=zk2\lambda_{k}^{2}x_{k}^{2}=z_{k}^{2} for every kk, so βˆ‘k=1∞λk2xk2\sum_{k=1}^{\infty}\lambda_{k}^{2}x_{k}^{2} converges and claim 1 gives x∈D(A)x\in D(A) with Ax=βˆ‘k=1∞λkxkek=βˆ‘k=1∞zkek=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 (iii). By Elementary Properties of a Hilbert Triple: the Embedding, the Riesz Map and the Form Operator (iii) the Riesz map satisfies J(Ax)=xJ(Ax)=x for every x∈D(A)x\in D(A), so Jz=J(Ax)=xJz=J(Ax)=x, which is the asserted identity.

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