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Measure, Integration & Real Analysis, 2021a

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332 Chapter 10 Linear Maps on Hilbert Spaces<br />

Singular Value Decomposition<br />

The next result provides an important generalization of 10.106(b) to arbitrary compact<br />

operators that need not be self-adjoint or normal. This generalization requires two<br />

orthonormal families, as compared to the single orthonormal family in 10.106(b).<br />

10.113 Singular Value Decomposition<br />

Suppose T is a compact operator on a Hilbert space V. Then there exist a<br />

countable set Ω, orthonormal families {e k } k∈Ω and {h k } k∈Ω in V, and a family<br />

{s k } k∈Ω of positive numbers such that<br />

10.114 Tf = ∑ s k 〈 f , e k 〉h k<br />

k∈Ω<br />

for every f ∈ V.<br />

Proof<br />

If α is an eigenvalue of T ∗ T, then (T ∗ T) f = α f for some f ̸= 0 and<br />

α‖ f ‖ 2 = 〈α f , f 〉 = 〈T ∗ Tf, f 〉 = 〈Tf, Tf〉 = ‖Tf‖ 2 .<br />

Thus α ≥ 0. Hence all eigenvalues of T ∗ T are nonnegative.<br />

Apply 10.106(b) and the conclusion of the paragraph above to the self-adjoint<br />

compact operator T ∗ T, getting a countable set Ω, an orthonormal family {e k } k∈Ω in<br />

V, and a family {s k } k∈Ω of positive numbers (take s k = √ α k ) such that<br />

10.115 (T ∗ T) f = ∑ s 2 k 〈 f , e k 〉e k<br />

k∈Ω<br />

for every f ∈ V. The equation above implies that (T ∗ T)e j = s 2 j e j for each j ∈ Ω.<br />

For k ∈ Ω, let<br />

h k = Te k<br />

.<br />

s k<br />

For j, k ∈ Ω,wehave<br />

〈h j , h k 〉 = 1<br />

s j s k<br />

〈Te j , Te k 〉 = 1<br />

s j s k<br />

〈T ∗ Te j , e k 〉 = s j<br />

s k<br />

〈e j , e k 〉.<br />

The equation above implies that {h k } k∈Ω is an orthonormal family in V.<br />

If f ∈ span {e k } k∈Ω , then<br />

)<br />

Tf = T(<br />

∑ 〈 f , e k 〉e k = ∑ 〈 f , e k 〉Te k = ∑ s k 〈 f , e k 〉h k ,<br />

k∈Ω<br />

k∈Ω<br />

k∈Ω<br />

showing that 10.114 holds for such f .<br />

If f ∈ ( span {e k } k∈Ω<br />

) ⊥, then 10.115 shows that (T ∗ T) f = 0, which implies<br />

that Tf = 0 (because 0 = 〈T ∗ Tf, f 〉 = ‖Tf‖ 2 ); thus both sides of 10.114 are 0.<br />

Hence the two sides of 10.114 agree for f in a closed subspace of V and for f in<br />

the orthogonal complement of that closed subspace, which by linearity implies that<br />

the two sides of 10.114 agree for all f ∈ V.<br />

<strong>Measure</strong>, <strong>Integration</strong> & <strong>Real</strong> <strong>Analysis</strong>, by Sheldon Axler

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