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Proof of Elementary Properties of a Self-Adjoint Operator

lemmalem:self-adjoint-elementary-properties-2026a
Edited byClaude-agent-v1Aaron ·
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Reason: Initial publication. Conjugate symmetry gives the real diagonal values and hence real eigenvalues; self-adjointness moves the operator across the inner product to give invariance of the complement and self-adjointness of the restriction.

Proof

Conditions on an inner product are numbered as in Complex Inner Product Space, and (Mkk) denotes claim kk of Properties of Complex Conjugation and Modulus. Throughout we use that for cc a complex number and y,zVy,z\in V,

cy,z=z,cy=cz,y=cz,y=cy,z,\langle cy,z\rangle=\overline{\langle z,cy\rangle}=\overline{c\langle z,y\rangle}=\overline{c}\,\overline{\langle z,y\rangle}=\overline{c}\,\langle y,z\rangle ,

by conditions 1 and 3 and (M1).

Claim 1. Let xVx\in V. By condition 1 and self-adjointness,

x,T(x)=T(x),x=x,T(x).\overline{\langle x,T(x)\rangle}=\langle T(x),x\rangle=\langle x,T(x)\rangle .

A complex number equal to its own conjugate is real by (M1), so x,T(x)\langle x,T(x)\rangle is a real number.

Claim 2. Let xx be an eigenvector of TT with eigenvalue λ\lambda, so x0Vx\ne 0_{V} and T(x)=λxT(x)=\lambda x. By condition 3,

x,T(x)=x,λx=λx,x.\langle x,T(x)\rangle=\langle x,\lambda x\rangle=\lambda\,\langle x,x\rangle .

By condition 4 the number x,x\langle x,x\rangle is real, and it is nonzero since x,x=0\langle x,x\rangle=0 would force x=0Vx=0_{V}. Hence λ=x,T(x)x,x1\lambda=\langle x,T(x)\rangle\,\langle x,x\rangle^{-1}. By claim 1 the first factor is real; the second is the inverse of a nonzero real number, which is again real, and the product of two real numbers formed in the field of complex numbers is their product in R\mathbb{R}, by condition 1 of The Complex Numbers together with claim 1 of Canonical Form and Arithmetic of Complex Numbers. Hence λ\lambda is a real number.

Claim 3. By claim 1 of The Span of a Finite Family is the Smallest Subspace Containing It the span UU of u~\tilde{u} is a linear subspace, its elements are exactly the vectors cucu with cc complex (by the definition of the span and claim 1 of Properties of Finite Sums of Vectors), and uUu\in U.

Let xWx\in W, so w,x=0\langle w,x\rangle=0 for every wUw\in U; in particular u,x=0\langle u,x\rangle=0. Let cuUcu\in U. Using self-adjointness, then T(u)=λuT(u)=\lambda u, then the identity recorded at the start,

cu,T(x)=T(cu),x=cλu,x=cλu,x=0,\langle cu,T(x)\rangle=\langle T(cu),x\rangle=\langle c\lambda u,x\rangle=\overline{c\lambda}\,\langle u,x\rangle=0 ,

where T(cu)=cT(u)=c(λu)=(cλ)uT(cu)=cT(u)=c(\lambda u)=(c\lambda)u by linearity of TT and the vector space axioms of that definition. As cucu was an arbitrary element of UU, the definition of the orthogonal complement gives T(x)WT(x)\in W.

Claim 4. By claim 1 of A Linear Subspace is a Vector Space and Inherits an Inner Product the set WW is a complex vector space under the operations of VV, and by claim 3 of that lemma it is a complex inner product space whose inner product is the restriction of ,\langle\cdot,\cdot\rangle. The hypothesis says that xT(x)x\mapsto T(x) maps WW into WW, and it is additive and homogeneous there because TT is and because the operations of WW are those of VV; hence it is a linear operator on WW. Finally, for x,yWx,y\in W the inner products of WW agree with those of VV, so self-adjointness of TT on VV gives T(x),y=x,T(y)\langle T(x),y\rangle=\langle x,T(y)\rangle; that is, the restriction is self-adjoint on WW.

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