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with the integral pairing is a Hilbert space
Statement
Assume the Axiom of Countable Choice (The Axiom of Countable Choice ()). Let be a measure space and let be the quotient of by the almost-everywhere zero functions (The space as the quotient by null functions), with the quotient norm (The norm descends to the quotient and makes a normed space for ).
- On real the formula is a well-defined inner product, linear in both variables, positive definite, with ; with it is a real Hilbert space (Hilbert space). 2. On complex the formula is a well-defined inner product, linear in the first variable and conjugate-linear in the second, positive definite, with ; with it is a complex Hilbert space (Complex Lp classes and Euclidean test-function conventions).
In both cases the inner product induces exactly the established quotient norm.
Facts & Assumptions
For one has , so ; the integral is unchanged when a representative is replaced by an almost-everywhere equal one, and it is linear on (Cauchy-Schwarz inequality for , Two integrable functions are equal almost everywhere exactly when all of their indefinite integrals agree, The Lebesgue integral is linear on ).
is complete for , and is a norm on the quotient, so the quotient metrics are the ones in which completeness is asserted (Riesz-Fischer completeness of for , The norm descends to the quotient and makes a normed space for ).
For a nonnegative measurable , if and only if almost everywhere; consequently forces in (A nonnegative measurable function has integral exactly when it vanishes almost everywhere).
On complex the pairing is representative-independent, linear in the first variable, conjugate-linear in the second, conjugate symmetric, positive definite, satisfies and Cauchy–Schwarz, and complex is complete (Complex completeness, density, and inner product: the consumer interface).
An inner product is linear in the first variable, conjugate symmetric and positive definite, and induces the norm (Real and complex inner-product spaces and their induced length).
Proof
Given: Countable Choice and a measure space .
Real case: the pairing. For the product is integrable by [A1], so is defined and depends only on the classes of and by [A1]; the assignment is bilinear by linearity of the integral on and symmetric because multiplication of real functions is commutative.
Complex case. The published complex interface [A4] states that on complex the pairing is representative-independent, linear in the first variable, conjugate-linear in the second, conjugate symmetric and positive definite with , and that complex is complete for ; hence complex is a complex Hilbert space for that pairing, with the established quotient norm.
The real pairing is positive definite: vanishes exactly when almost everywhere, that is exactly when represents the zero class, by [A3]; moreover because the norm is the square root of and for real . Hence the real pairing is an inner product inducing the quotient norm.
The real quotient is complete for that norm by [A2], so with this inner product real is a real Hilbert space.
Steps 3.1 and 1.2 establish both claims for every measure space under Countable Choice, the norm in each case being the established quotient norm.
Depends on
- Hilbert space
- The space $L^p(\mu)$ as the quotient by null functions
- Cauchy-Schwarz inequality for $L^2$
- Riesz-Fischer completeness of $L^p$ for $1 \le p \le \infty$
- Complex Lp classes and Euclidean test-function conventions
- Complex completeness, density, and inner product: the consumer interface
- The Axiom of Countable Choice ($\mathrm{AC}_\omega$)
- Real and complex inner-product spaces and their induced length
- Two integrable functions are equal almost everywhere exactly when all of their indefinite integrals agree
- The Lebesgue integral is linear on $L^1(\mu)$
- A nonnegative measurable function has integral $0$ exactly when it vanishes almost everywhere
- The $L^p$ norm descends to the quotient and makes $L^p$ a normed space for $1 \le p \le \infty$
Used by
- A symmetric closed operator that is not self-adjoint Counterexample
- Backward heat amplifies small high-frequency errors Counterexample
- Continuous calculus does not contain discontinuous spectral projections Counterexample
- The unitary dual need not be Hausdorff Counterexample
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- Closed pointwise box of L2 controls Definition
- Dual source certificates for TV regularization Definition
- E-valued Dolbeault operators and their L2 structure Definition
- Incomplete tensor product of one-mode Hilbert spaces with a reference vector Definition
- L2-m-approximable causal Bernoulli shifts Definition
- Left and right regular representations on L2(G) Definition
- Linear coercive elliptic PDE control problem and reduced objective Definition
- Lipschitz polyhedral boundary, orientation, and trace spaces Definition
- States, tracial states and faithful normal traces on a von Neumann algebra Definition
- The Bergman space A²(Ω) and the Bergman kernel Definition
- The Hardy boundary space, Szegő projection and Szegő kernel on a smoothly bounded domain Definition
- The real H(curl) graph space on a polyhedron Definition
- The shifted elliptic solution operator Definition
- A broken P1 test exposes a nonzero consistency residual Example
- A Gaussian wavelet series at the Besov threshold Example
- A smooth Bessel-blur truth with an explicit TV source certificate Example
- A square-integrable linear shift with nonsummable physical dependence Example
- Abstract smoothing does not imply a spatial derivative without a PDE realisation Example
- Ball monomial norms, Bergman and Szegő kernels of the ball Example
- Circular Radon inversion at the zero truth Example
- Functional calculus for a multiplication operator Example
- Integral operator trace under a valid diagonal hypothesis Example
- Legendre polynomials from Gram–Schmidt Example
- Multiplication operators: domain, spectral measure and spectrum Example
- Multiplicity-two diagonal representation Example
- Pvm of a multiplication operator Example
- Sine modes decay under Dirichlet heat flow Example
- SOLIT for a Dirichlet second-antiderivative model Example
- The Haar orthonormal basis of L²((0,1)) Example
- The one-mode Schrödinger formulas and their phase Example
- The polydisc Bergman product and the different distinguished-torus Hardy kernel Example
- The positive-type Gaussian on the real line and its cyclic model Example
- The sectorial multiplication operator Example
- The square of the Volterra operator has zero trace Example
- Volterra operator is Hilbert Schmidt and quasinilpotent Example
…and 65 more results.
Dependency tree · two levels
65 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- Theo Bühler and Dietmar Salamon, Functional Analysis — §§1.3.3 and 5.3.1, pp.38–41 and 235–237 (standard reference, not scraped)
- Gerald Teschl, Topics in Real and Functional Analysis, version November 17, 2017 — §2.5, pp.63–64 (standard reference, not scraped)