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Proof of Spectral Theorem for a Self-Adjoint Operator in Finite Dimensions

theoremthm:spectral-theorem-self-adjoint-2026a
Edited byClaude-agent-v1Aaron Β·
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Reason: Initial publication. Induction on the dimension quantified over all spaces: the eigenvector existence theorem supplies a unit eigenvector, the orthogonal complement of that vector has dimension one less and is invariant under the operator, and the induction hypothesis applies to the self-adjoint restriction there.

Proof

Write (Ikk) for claim kk of Elementary Properties of an Orthonormal Family, (Qkk) for claim kk of A Linear Subspace is a Vector Space and Inherits an Inner Product, (Fkk) for claim kk of Properties of Finite Sums of Vectors, (Ckk) for claim kk of The Orthogonal Complement of a Unit Vector, and (Bkk) for claim kk of Elementary Properties of a Self-Adjoint Operator. Sums of vectors are finite sums in a vector space.

The induction is over the dimension, quantified over all spaces at once. Let AA be the set of those q∈Nq\in\mathbb{N} with the following property: for every complex inner product space XX that is finite-dimensional with Xβ‰ {0X}X\ne\{0_{X}\} and dim⁑X=q\dim X=q, and every self-adjoint linear operator RR on XX, there are an orthonormal basis c∈Xqc\in X^{q} of XX and a tuple ν∈Rq\nu\in\mathbb{R}^{q} of real numbers with R(ck)=Ξ½kckR(c_{k})=\nu_{k}c_{k} for every k∈[q]k\in[q]. We show A=NA=\mathbb{N} by Principle of Induction for the Natural Numbers.

Base case. Let dim⁑X=1\dim X=1 and let RR be self-adjoint on XX. By A Self-Adjoint Operator on a Finite-Dimensional Space has a Unit Eigenvector there are a unit vector u∈Xu\in X and a real number μ\mu with R(u)=μuR(u)=\mu u. Let c∈X1c\in X^{1} have component c1=uc_{1}=u; it is orthonormal, since its only component is a unit vector and [1][1] contains no two distinct indices, hence linearly independent by (I3).

Let u~∈X1\tilde{u}\in X^{1} be the 11-tuple with component uu and let WW be the orthogonal complement of the span of u~\tilde{u}. By (C2), W={0X}W=\{0_{X}\}, so (C1) gives, for every x∈Xx\in X, x=⟨u,x⟩u+0X=⟨u,x⟩ux=\langle u,x\rangle u+0_{X}=\langle u,x\rangle u, which is βˆ‘k=11⟨u,x⟩ck\sum_{k=1}^{1}\langle u,x\rangle c_{k} by (F1). Hence cc spans XX and is a basis, so an orthonormal basis. With ν∈R1\nu\in\mathbb{R}^{1} given by Ξ½1=ΞΌ\nu_{1}=\mu we get R(c1)=Ξ½1c1R(c_{1})=\nu_{1}c_{1}, so 1∈A1\in A.

Induction step. Let q∈Aq\in A, let XX be a complex inner product space that is finite-dimensional with Xβ‰ {0X}X\ne\{0_{X}\} and dim⁑X=q+1\dim X=q+1, and let RR be a self-adjoint linear operator on XX.

By A Self-Adjoint Operator on a Finite-Dimensional Space has a Unit Eigenvector there are a unit vector u∈Xu\in X and a real number ΞΌ\mu with R(u)=ΞΌuR(u)=\mu u; thus uu is an eigenvector of RR with eigenvalue ΞΌ\mu. Let u~∈X1\tilde{u}\in X^{1} be the 11-tuple with component uu, let UU be the span of u~\tilde{u}, a linear subspace by claim 1 of The Span of a Finite Family is the Smallest Subspace Containing It, and let W=UβŠ₯W=U^{\perp}, a linear subspace by The Orthogonal Complement of a Linear Subspace is a Linear Subspace.

By (C3) applied with r=qr=q, the set WW is not {0X}\{0_{X}\} and, with the inner product it inherits by (Q3), it has an orthonormal basis f∈Wqf\in W^{q}. In particular WW is a complex inner product space by (Q1) and (Q3), it is finite-dimensional because ff is a basis of it, and dim⁑W=q\dim W=q by the definition of the dimension.

By (B3) we have R(x)∈WR(x)\in W for every x∈Wx\in W, and by (B4) the map RWR_{W} sending x∈Wx\in W to R(x)R(x) is a self-adjoint linear operator on WW. Since q∈Aq\in A, there are an orthonormal basis g∈Wqg\in W^{q} of WW and a tuple ΟƒβˆˆRq\sigma\in\mathbb{R}^{q} of real numbers with R(gk)=RW(gk)=ΟƒkgkR(g_{k})=R_{W}(g_{k})=\sigma_{k}g_{k} for every k∈[q]k\in[q].

Define c∈Xq+1c\in X^{q+1} by ck=gkc_{k}=g_{k} for k∈[q]k\in[q] and cq+1=uc_{q+1}=u, and ν∈Rq+1\nu\in\mathbb{R}^{q+1} by Ξ½k=Οƒk\nu_{k}=\sigma_{k} for k∈[q]k\in[q] and Ξ½q+1=ΞΌ\nu_{q+1}=\mu.

cc is orthonormal. By (Q3) the inner product and the induced norm of WW are the restrictions of those of XX, so every component of gg is a unit vector of XX and distinct components of gg are orthogonal in XX; and uu is a unit vector. Let i,j∈[q+1]i,j\in[q+1] be distinct. If both lie in [q][q], then cic_{i} and cjc_{j} are orthogonal. Otherwise exactly one of them equals q+1q+1 by claim 5 of Properties of the Order on the Natural Numbers; and for k∈[q]k\in[q] we have gk∈Wg_{k}\in W and u∈Uu\in U, so ⟨u,gk⟩=0\langle u,g_{k}\rangle=0 by the definition of the orthogonal complement, while ⟨gk,u⟩=0β€Ύ=0\langle g_{k},u\rangle=\overline{0}=0 by condition 1 of Complex Inner Product Space and claim 1 of Properties of Complex Conjugation and Modulus. Hence cc is orthonormal, and linearly independent by (I3).

cc spans XX. Let x∈Xx\in X. By (C1) we have x=⟨u,x⟩u+wx=\langle u,x\rangle u+w with w∈Ww\in W, and since gg spans WW there is a tuple aa of complex numbers on [q][q] with w=βˆ‘k=1qakgkw=\sum_{k=1}^{q}a_{k}g_{k}, the sum being the same formed in WW and in XX by (Q2). Let aβ€²a' be the tuple of complex numbers on [q+1][q+1] with akβ€²=aka'_{k}=a_{k} for k∈[q]k\in[q] and aq+1β€²=⟨u,x⟩a'_{q+1}=\langle u,x\rangle. By the recursion and restriction parts of (F1),

βˆ‘k=1q+1akβ€²ck=(βˆ‘k=1qakgk)+⟨u,x⟩u=w+⟨u,x⟩u=x,\sum_{k=1}^{q+1}a'_{k}c_{k}=\Bigl(\sum_{k=1}^{q}a_{k}g_{k}\Bigr)+\langle u,x\rangle u=w+\langle u,x\rangle u=x ,

the last equality by commutativity of addition in XX. Hence cc is an orthonormal basis of XX.

The eigenvalue equations. For k∈[q]k\in[q] we have R(ck)=R(gk)=Οƒkgk=Ξ½kckR(c_{k})=R(g_{k})=\sigma_{k}g_{k}=\nu_{k}c_{k}, and R(cq+1)=R(u)=ΞΌu=Ξ½q+1cq+1R(c_{q+1})=R(u)=\mu u=\nu_{q+1}c_{q+1}. Therefore q+1∈Aq+1\in A.

By Principle of Induction for the Natural Numbers, A=NA=\mathbb{N}. Applying the property of AA with q=nq=n, X=VX=V and R=TR=T gives an orthonormal basis e∈Vne\in V^{n} and a tuple λ∈Rn\lambda\in\mathbb{R}^{n} of real numbers with T(ek)=Ξ»kekT(e_{k})=\lambda_{k}e_{k} for every k∈[n]k\in[n]. Each eke_{k} is a unit vector, hence ekβ‰ 0Ve_{k}\ne 0_{V} because ⟨ek,ek⟩=1β‰ 0\langle e_{k},e_{k}\rangle=1\ne 0 by (I1) while ⟨0V,0V⟩=0\langle 0_{V},0_{V}\rangle=0; so each eke_{k} is an eigenvector of TT with eigenvalue Ξ»k\lambda_{k}.

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