Chemistry Reference and  Research
           
 
Periodic Table
- standard table
- large table
 
Chemical Elements
- by name
- by symbol
- by atomic number
 
Chemical Properties
 
Chemical Reactions
 
Organic Chemistry
 
Branches of Chemistry
Analytical chemistry
Biochemistry
Computational Chemistry
Electrochemistry
Environmental chemistry
Geochemistry
Inorganic chemistry
Materials science
Medicinal chemistry
Nuclear chemistry
Organic chemistry
Pharmacology
Physical chemistry
Polymer chemistry
Supramolecular Chemistry
Thermochemistry

Projection-valued measure

In mathematics, projection-valued measures are used to express results in spectral theory. A projection-valued measure on a measurable space (X, M) is a mapping π from M to the set of self-adjoint projections on a Hilbert space H such that

\pi(X) = 1_H \quad

and for every ξ η ∈ H, the set-function

\operatorname{S}_\pi(\xi, \eta)(A) = \langle \pi(A)\xi \mid \eta \rangle

is a complex-valued countably additive measure on M.

If π is a projection-valued measure and

A \cap B = \emptyset,

then π(A), π(B) are orthogonal projections. From this follows that in general,

\pi(A) \pi(B) = \pi(A \cap B).

Example. Suppose (X, M, μ) is a measure space. Let π(A) be the operator of multiplication by 1A on L2(X). π is a projection-valued measure.

Extensions of projection-valued measures

If π is a additive projection-valued measure on (X, M), then the map

\mathbf{1}_A \mapsto \pi(A)

extends to a linear map on the vector space of step functions on X. In fact, it is easy to check that this map is a ring homomorphism. In fact this map extends in a canonical way to all bounded complex-valued Borel functions on X.

Theorem. For any bounded M-measurable function f on X, there is a unique bounded linear operator Tπ(f) such that

\langle \operatorname{T}_\pi(f) \xi \mid  \eta \rangle = \int_X f(x) d \operatorname{S}_\pi (\xi,\eta)(x)

for all ξ, η ∈ H. The map

f \mapsto \operatorname{T}_\pi(f)

is a homomorphism of rings.

Structure of projection-valued measures

First we provide a general example of projection-valued measure based on direct integrals. Suppose (X, M, μ) is a measure space and let {Hx}xX be a μ-measurable family of Hilbert spaces. For every AM, let π(A) be the operator of multiplication by 1A on the Hilbert space

\int_X^\oplus H_x \ d \mu(x).

Then π is a projection-valued measure on (X, M).

Suppose π ρ are projection-valued measures on (X, M) with values in the projections of H, K. π, ρ are unitarily equivalent iff there is a unitary operator U:HK such that

\pi(A) = U^* \rho(A) U \quad

for every AM.

Theorem. If (X, M) is a standard Borel space , then for every projection-valued measure π on (X, M), there is a Borel measure μ and a μ-measurable family of Hilbert spaces {Hx}xX , such that π is unitarily equivalent to multiplication by 1A on the Hilbert space

\int_X^\oplus H_x \ d \mu(x).

The measure class of μ and the measure equivalence class of the multiplicity function x → dim Hx completely characterize the projection-valued measure up to unitary equivalence.

A projection-valued measure π is homogeneous of multiplicity n iff the multiplicity function has constant value n. Clearly,

Theorem. Any projection-valued measure π is an orthogonal direct sum of homogeneous projection-valued measures:

\pi = \bigoplus_{1 \leq n \leq \omega} (\pi | H_n)

where

H_n = \int_{X_n}^\oplus H_x \ d (\mu | X_n) (x)

and

X_n = \{x \in X: \operatorname{dim} H_x = n\}.

References

  • G. W. Mackey, The Theory of Unitary Group Representations, The University of Chicago Press, 1976
  • V. S. Varadarajan, Geometry of Quantum Theory V2, Springer Verlag, 1970.
01-04-2007 01:16:19
The contents of this article are licensed from Wikipedia.org under the GNU Free Documentation License. How to see transparent copy