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Simple pvm integral is representation independent

Statement

Assume Countable Choice. Let (X,Σ) be a measurable space, let H be a complex Hilbert space, let E be a projection valued measure on (X,Σ), and let s:XC be a complex simple function. Then:

  1. the operator sdE of Integral of a simple function against a pvm is independent of the disjoint normal form of s;
  2. for all x,yH, (sdE)x,y=sdEx,y, the scalar integral against the complex measure Ex,y;
  3. for every xH, (sdE)x2=s2dEx, and sdEMs.

Here Ms:=max({0}{s(t):tX}); thus Ms=maxtXs(t) when X, and Ms=0 when X=.

Facts & Assumptions

[A1]

For a disjoint normal form s=j=1maj1Bj with B1,,Bm pairwise disjoint and covering X, the integral is sdE=jajE(Bj) (Integral of a simple function against a pvm).

[A2]

E()=0, E(X)=I, E(BC)=E(B)E(C), each E(B) satisfies E(B)2=E(B)=E(B) and is contractive, and for pairwise disjoint (Dn) with union D one has E(D)x=nE(Dn)x in norm (Projection valued measure).

[A3]

Ex,y(B)=E(B)x,y is a finite complex measure, Ex(B)=E(B)x,x=E(B)x2 is a positive measure of mass x2, Ex,y(X)xy, and Ey,x=Ex,y (Scalar and complex measures from a pvm).

[A4]

For a complex measure ν and a complex simple function whose nonzero level sets have finite total variation, presented over the nonzero level sets, the scalar simple integral is sdν=jcjν(Ej), and the value is unchanged by deleting empty level sets (The simple integral against a signed or complex measure, Complex simple functions as finite sums of measurable indicators).

[A5]

The pairing is linear in the first argument and conjugate-linear in the second, so jzj,y=jzj,y and z,w=w,z (Real and complex inner-product spaces and their induced length). The adjoint identity is Pu,v=u,Pv (The Hilbert-space adjoint of a bounded operator).

[A6]

Countable Choice is the declared standing hypothesis of this block of the page (The Axiom of Countable Choice (ACω)).

[A8]

Total variation is the supremum of the nonnegative sums over countable measurable partitions (The total variation |nu|(E) from countable measurable partitions).

Proof

technique · direct

Given: A measurable space (X,Σ), a complex Hilbert space H, a projection valued measure E, a complex simple function s with two disjoint normal forms s=j=1maj1Bj=k=1nbk1Ck covering X, and vectors x,yH.

1.1

Finite additivity follows by padding a finite disjoint family with empty sets in strong countable additivity. The scalar measures also have finite additivity. Every measurable subset has finite Ex,y-variation: a countable partition of that subset extends to one of X by adding its complement, so its sum is at most Ex,y(X)xy. In particular the scalar simple integrals below are defined; for Ex=Ex,x the same argument applies.

A2A3A4A8
2.1

The intersections BjCk form a disjoint cover of X. If an intersection is nonempty then aj=bk, and if empty its projection value is zero. Finite additivity therefore gives jajE(Bj)=j,kajE(BjCk)=j,kbkE(BjCk)=kbkE(Ck). This proves representation independence.

step 1.1A1A2algebra
3.1

Expanding the pairing gives (sdE)x,y=jajEx,y(Bj). Discard empty cells and regroup the remaining indices by cs(X). Finite additivity gives jajEx,y(Bj)=cs(X)cEx,y(s1({c}))=sdEx,y, where the zero-value term is zero. If X is empty all cells and sums contribute zero.

step 1.1step 2.1A1A3A4A5algebra
3.2

The adjoint identity and the projection rules give E(Bj)x,E(Bk)x=E(Bk)E(Bj)x,x=E(BkBj)x,x. Thus expansion of the squared norm leaves only diagonal terms: (sdE)x2=jaj2Ex(Bj). Regrouping the nonempty cells by the value d=aj2, finite additivity identifies this sum with ds2(X)dEx((s2)1({d}))=s2dEx; the zero term vanishes.

step 1.1step 2.1A1A2A3A4A5algebra
4.1

Empty cells contribute zero to the sum in step 3.2. On every nonempty Bj, ajMs because aj is a value of s. Positivity and finite additivity give (sdE)x2Ms2jEx(Bj)=Ms2x2. Taking nonnegative square roots and then the unit-ball supremum gives sdEMs. When X=, all projection values are zero and the integral is zero, so the same bound with Ms=0 holds.

step 1.1step 3.2A2A3A7algebra
5.1

The integral is independent of the presentation, has the asserted scalar pairings and squared-norm identity, and satisfies the stated bound, including the empty-space case.

step 2.1step 3.1step 3.2step 4.1A6

Depends on

Used by

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Sources