In the mathematical literature, one may also find other results that bear Naimark's name.
Spelling
In the physics literature, it is common to see the spelling “Neumark” instead of “Naimark.” The latter variant is according to the romanization of Russian used in translation of Soviet journals, with diacritics omitted. The former is according to the etymology of the surname.
E is called self-adjoint if E is self-adjoint for all B.
E is called spectral if it is self-adjoint and for all.
We will assume throughout that E is regular. Let C denote the abelian C*-algebra of continuous functions on X. If E is regular and bounded, it induces a map in the obvious way: The boundedness of E implies, for all h of unit norm This shows is a bounded operator for all f, and itself is a bounded linear map as well. The properties of are directly related to those of E:
If E is positive, then, viewed as a map between C*-algebras, is also positive.
is a homomorphism if, by definition, for all continuous f on X and,
The LHS is and the RHS is So, taking f a sequence of continuous functions increasing to the indicator function of B, we get, i.e. E is self adjoint.
Combining the previous two facts gives the conclusion that is a *-homomorphism if and only if E is spectral and self adjoint.
Naimark's theorem
The theorem reads as follows: Let E be a positive L-valued measure on X. There exists a Hilbert space K, a bounded operator, and a self-adjoint, spectral L-valued measure on X, F, such that
Proof
We now sketch the proof. The argument passes E to the induced map and uses Stinespring's dilation theorem. Since E is positive, so is as a map between C*-algebras, as explained above. Furthermore, because the domain of, C, is an abelian C*-algebra, we have that is completely positive. By Stinespring's result, there exists a Hilbert space K, a *-homomorphism, and operator such that Since π is a *-homomorphism, its corresponding operator-valued measure F is spectral and self adjoint. It is easily seen that F has the desired properties.
Finite-dimensional case
In the finite-dimensional case, there is a somewhat more explicit formulation. Suppose now, therefore C is the finite-dimensional algebra, and H has finite dimension m. A positive operator-valued measureE then assigns each i a positive semidefinitem × m matrix. Naimark's theorem now states that there is a projection-valued measure on X whose restriction is E. Of particular interest is the special case when where I is the identity operator. In this case, the induced map is unital. It can be assumed with no loss of generality that each is a rank-one projection onto some. Under such assumptions, the case is excluded and we must have either
and E is already a projection-valued measure,
and does not consist of mutually orthogonal projections.
For the second possibility, the problem of finding a suitable projection-valued measure now becomes the following problem. By assumption, the non-square matrix is an isometry, that is. If we can find a matrix N where is a n × n unitary matrix, the projection-valued measure whose elements are projections onto the column vectors of U will then have the desired properties. In principle, such a N can always be found.