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Real L2 kernels define bounded operators and represent rank-one tensors

Statement

Let I=[0,1] with its Borel sigma-algebra and Lebesgue measure dt, and let H=L2(I,dt;R) and K=L2(I2,dt×dt;R) be the quotient spaces by null functions. Assume Countable Choice, so these L2 spaces have their usual real Hilbert-space structures. For k∈K and f∈H, define, for almost every u, (Tkf)(u)=∫01k(u,v)f(v) dv. This defines a bounded linear operator Tk:H→H and ∥Tk∥≤∥k∥K. For x,y∈H, the class x⊠y represented by x(u)y(v) is well-defined in K, satisfies ∥x⊠y∥K=∥x∥H∥y∥H, and Tx⊠y=x⊗y, where (x⊗y)h=⟨h,y⟩Hx. For x,y,g,h∈H the product-kernel inner product also satisfies ⟨x⊠y,g⊠h⟩K=⟨x,g⟩H⟨y,h⟩H.

Facts & Assumptions

Given: Countable Choice; the Borel probability space (I,B,dt); the product measure dt×dt on I2; and the real L2 quotient spaces H and K.

[A1]

Countable Choice is assumed for the Hilbert-space L2 interfaces (The Axiom of Countable Choice (ACω), L2 with the integral pairing is a Hilbert space).

[F1]

The product measure is sigma-finite and satisfies (dt×dt)(A×B)=dt(A)dt(B) for Borel A,B (For sigma-finite factors, the product measure exists, has the rectangle formula, is sigma-finite, and is unique, Finite, sigma-finite, and semifinite measures).

[F2]

Tonelli applies to nonnegative Borel functions on I2 and makes their section integrals measurable (Tonelli's theorem for nonnegative measurable functions on a sigma-finite product).

[F3]

If a product-measurable function is in L1(dt×dt), its sections are integrable almost everywhere, the section-integral function is measurable after zero extension on the exceptional null set, and its integral equals the product integral (Fubini's theorem for L^1 functions on a sigma-finite product).

[F4]

The real L2 quotient has inner product ⟨f,g⟩=∫fg dt and satisfies Cauchy–Schwarz (L2 with the integral pairing is a Hilbert space, The space Lp(μ) as the quotient by null functions, Real and complex inner-product spaces and their induced length).

Proof

Given: The spaces, functions, and conventions in the Statement and Facts & Assumptions.

1.1A1F1F2F4

Choose measurable representatives of x and y. By [F1]–[F2], ∫I2∣x(u)y(v)∣2 d(dt×dt)=(∫I∣x(u)∣2 du)(∫I∣y(v)∣2 dv)<∞. Changing either representative changes the product only on (N×I)∪(I×M) for null sets N,M⊂I; [F1] gives this union product measure zero. Hence x⊠y is a well-defined class in K and the displayed integral proves its norm identity.

1.2F1F2F3F4algebra

Choose Borel representatives of k and f. The function (u,v)↦k(u,v)f(v) is product-measurable and belongs to L1(dt×dt), since Cauchy–Schwarz on I2 gives ∫I2∣k(u,v)f(v)∣ du dv≤∥k∥K(∫I2∣f(v)∣2 du dv)1/2=∥k∥K∥f∥H. By [F3] its section integrals are defined almost everywhere and have a measurable representative. For almost every u, sectionwise Cauchy–Schwarz and [F2] give ∣(Tkf)(u)∣2≤∥f∥H2∫I∣k(u,v)∣2 dv,∥Tkf∥H2≤∥k∥K2∥f∥H2. If f is changed on a dt-null set, its section integral is unchanged for every u whose k(u,⋅) is square-integrable. If k is changed on a (dt×dt)-null set, the difference times f(v) is in L1 by the same Cauchy–Schwarz estimate, so [F3] makes its section integral zero for almost every u. Thus Tk is well-defined on the quotients. Linearity follows from linearity of the section integral, and the second estimate proves boundedness and ∥Tk∥≤∥k∥K.

2.1step 1.1step 1.2F4algebra

For k=x⊠y and almost every u, the section is integrable by step 1.2 and (Tx⊠yf)(u)=x(u)∫Iy(v)f(v) dv=x(u)⟨f,y⟩H=((x⊗y)f)(u). Thus Tx⊠y=x⊗y as operators on H. This includes x=0 or y=0, when both operators are zero.

3.1F1F3F4step 1.1algebra∎

For x,y,g,h∈H, [F3] applies to x(u)y(v)g(u)h(v) because Cauchy–Schwarz on I2 bounds its absolute integral by ∥x∥H∥g∥H∥y∥H∥h∥H. Fubini then factors the integral into ⟨x,g⟩H⟨y,h⟩H, proving the stated inner-product identity.

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