Physics:Quantum Mathematical Foundations of Quantum Theory

Hilbert space
A Hilbert space is a vector space equipped with an inner product and complete with respect to the norm induced by that inner product.[1] It provides the natural mathematical setting for quantum mechanics, where physical states are represented by vectors or, more precisely, by rays in a complex Hilbert space.[2] The geometry of Hilbert space generalizes the familiar Euclidean notions of length, angle, orthogonality, and projection to spaces of finite or infinite dimension.
Definition
A Hilbert space is a vector space over or together with an inner product
such that the induced norm
makes a complete metric space.[3]
In quantum theory, Hilbert spaces are usually taken to be complex. A normalized state vector satisfies
Geometric interpretation
Hilbert space extends the geometry of ordinary three-dimensional space to possibly infinitely many dimensions. The inner product determines:
- the length of a vector through its norm;
- the angle between vectors through their overlap;
- the notion of orthogonality, when ;
- the projection of one vector onto another or onto a subspace.
These ideas are central in quantum mechanics.[4]
Examples
Euclidean space
The finite-dimensional space with the standard dot product is a simple example of a Hilbert space. Likewise, with
is the standard Hilbert space of finite-dimensional quantum systems.[5]
Function spaces
An important infinite-dimensional example is the space of square-integrable functions. The inner product is
Wavefunctions in nonrelativistic quantum mechanics are elements of such spaces.[6]
Sequence spaces
Another standard example is the space of square-summable sequences.
Basis and expansion
A Hilbert space may have an orthonormal basis , meaning
Any vector can be expanded as
These expansions generalize Fourier series.[7]

Hilbert space in quantum mechanics
Hilbert space provides the formal setting for quantum states.[8]
The probability amplitude between two states is
and probabilities are given by its squared magnitude.
Operators and observables
Physical quantities are represented by operators acting on Hilbert space.[9]
Observables correspond to self-adjoint operators with real eigenvalues.[10]
The expectation value is
Commutators
The commutator
leads to the uncertainty principle.[11]
Spectral theorem
The spectral theorem decomposes self-adjoint operators into projection operators.[12]
This provides the mathematical basis for quantum measurement.
Density matrices
A general quantum state is described by a density operator .[13]
Pure states satisfy , while mixed states satisfy .
See also
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References
- ↑ Reed, Michael; Simon, Barry (1980). Methods of Modern Mathematical Physics, Vol. 1: Functional Analysis. Academic Press. ISBN 9780125850506.
- ↑ Dirac, P. A. M. (1930). The Principles of Quantum Mechanics. Oxford University Press. https://archive.org/details/principlesofquan0000dira.
- ↑ Hall, Brian C. (2013). Quantum Theory for Mathematicians. Springer. https://link.springer.com/book/10.1007/978-1-4614-7116-5.
- ↑ Griffiths, David J. (2018). Introduction to Quantum Mechanics. Pearson.
- ↑ Nielsen, Michael A.; Chuang, Isaac L. (2010). Quantum Computation and Quantum Information. Cambridge University Press. https://doi.org/10.1017/CBO9780511976667.
- ↑ Sakurai, J. J. (1994). Modern Quantum Mechanics. Addison-Wesley.
- ↑ Reed, Michael; Simon, Barry (1980). Methods of Modern Mathematical Physics. Academic Press.
- ↑ von Neumann, John (1955). Mathematical Foundations of Quantum Mechanics. Princeton University Press. https://archive.org/details/mathematicalfoun0000vonn.
- ↑ Dirac, P. A. M. (1930). The Principles of Quantum Mechanics. Oxford University Press.
- ↑ Hall, Brian C. (2013). Quantum Theory for Mathematicians. Springer.
- ↑ Griffiths, David J. (2018). Introduction to Quantum Mechanics. Pearson.
- ↑ Reed, Michael; Simon, Barry (1980). Methods of Modern Mathematical Physics. Academic Press.
- ↑ Nielsen, Michael A.; Chuang, Isaac L. (2010). Quantum Computation and Quantum Information. Cambridge University Press.
