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Hilbert space

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Hilbert space
NameHilbert space
CaptionDavid Hilbert, whose foundational work gave the space its name.
FieldFunctional analysis
InventedLate 19th–early 20th century
InventorsDavid Hilbert, John von Neumann

Hilbert space. A Hilbert space is a fundamental concept in mathematics and theoretical physics, providing the infinite-dimensional generalization of Euclidean space. It is a complete inner product space, a structure that allows for the rigorous definition of geometric notions like length, angle, and orthogonality in infinite dimensions. The theory was largely developed through the work of David Hilbert and John von Neumann, and it forms the mathematical foundation for quantum mechanics and many areas of analysis.

Definition and basic properties

A Hilbert space is defined as a complete inner product space over the field of real numbers or complex numbers. The inner product, often denoted ⟨x, y⟩, induces a norm via the relation ‖x‖ = √⟨x, x⟩, satisfying the Cauchy–Schwarz inequality. Completeness, a critical property, means that every Cauchy sequence of vectors in the space converges to a limit within the space, distinguishing it from a general inner product space. This property is essential for the convergence of series and the application of many analytical techniques, linking the concept deeply to Banach space theory. Key foundational results include the Riesz representation theorem, which characterizes continuous linear functionals, and the parallelogram law, an identity that characterizes norms derived from inner products.

Examples of Hilbert spaces

The most canonical example is the space of square-summable sequences, denoted ℓ², where the inner product of sequences (a_n) and (b_n) is Σ a_n b̄_n. Another central example is the space of Lebesgue square-integrable functions, L²(ℝ), fundamental in Fourier analysis and quantum field theory. Finite-dimensional Euclidean space ℝⁿ and its complex counterpart ℂⁿ, with the standard dot product, are also Hilbert spaces. The Sobolev spaces, such as H¹, used in the study of partial differential equations, provide important examples where the inner product incorporates derivatives. Spaces of holomorphic functions, like the Bergman space and the Hardy space, are also significant Hilbert spaces in complex analysis.

Orthogonality and projections

Orthogonality, defined by ⟨x, y⟩ = 0, is a pivotal geometric concept. A set of mutually orthogonal vectors of norm one is called an orthonormal basis, such as the trigonometric functions {e^(inx)} in L²([-π, π]) or the Hermite polynomials in certain weighted L² spaces. The Gram–Schmidt process can generate such bases from linearly independent sets. The projection theorem states that for any closed convex set in a Hilbert space, there exists a unique vector of minimum distance from a given point, leading to the definition of the orthogonal projection operator. This theorem underpins the least squares approximation method and is crucial for decomposing a space into a direct sum, as seen with orthogonal complements.

Operators on Hilbert spaces

The study of linear operators is central to the theory. Bounded operators, those with finite operator norm, include important classes like self-adjoint operators, which are analogous to symmetric matrices and are essential in quantum mechanics for representing observables. Compact operators, which include many integral operators, have spectral properties resembling those of finite matrices, as described by the spectral theorem. Unitary operators preserve the inner product and represent symmetries. The theory of unbounded operators, such as differential operators, is more subtle but vital, with the Stone's theorem on one-parameter unitary groups being a landmark result. The commutator of operators plays a key role in the Heisenberg uncertainty principle.

Applications

Hilbert space theory is indispensable in quantum mechanics, where the state of a physical system is represented by a vector in a complex Hilbert space, and observables correspond to self-adjoint operators. In signal processing, the L² space is used for analyzing waveforms via the Fourier transform. The partial differential equations of mathematical physics, such as the Schrödinger equation and the wave equation, are often solved within a Hilbert space framework using methods from spectral theory. In probability theory, the space of random variables with finite second moment forms a Hilbert space, facilitating the study of stochastic processes and Wiener's work on Brownian motion. It also provides the setting for functional data analysis and underpins algorithms in machine learning, like support vector machines using reproducing kernel Hilbert spaces. Category:Functional analysis Category:Quantum mechanics Category:Mathematical structures