1942 CHAPTER 59. BASIC PROBABILITY

That is, for all f ∈S,∫Rn

f (y)dµ (y) =1

(2π)n/2

∫Rn

F (ψ)(y) f (y)dy

=1

(2π)n

∫Rn

f (y)(∫

Rne−iy·x

ψ (x)dx)

dy. (59.21.56)

I will show

f → 1(2π)n

∫Rn

f (y)(∫

Rne−iy·x

ψ (x)dx)

dy

is a positive linear functional and then it will follow from 59.21.56 that µ is unique. Thus itis needed to show the inside integral in 59.21.56 is nonnegative. First note that the integrandis a positive definite function of x for each fixed y. This follows from

∑k, j

e−iy·(xk−x j)ψ (xk−x j)αkα j

= ∑k, j

ψ (xk−x j)(

e−iy·(xk)αk

)e−iy·(x j)α j ≥ 0.

Let t > 0 and

h2t (x)≡1

(4πt)1/2 e−14t |x|

2.

Then by dominated convergence theorem,∫Rn

e−iy·xψ (x)dx = lim

t→∞

∫Rn

e−iy·xψ (x)h2t (x)dx

Letting dη2t = h2t (x)dx, it follows from Lemma 59.21.5 η2t = η t ∗η t and since these aresymmetric measures, it follows from Lemma 59.21.4 the above equals

limt→∞

∫Rn

e−iy·xψ (x)d (η t ∗η t)≥ 0

Thus the above functional is a positive linear functional and so there exists a unique Radonmeasure, µ satisfying∫

Rnf (y)dµ (y) =

1

(2π)n/2

∫Rn

F (ψ)(y) f (y)dy

=1

(2π)n

∫Rn

f (y)(∫

Rne−iy·x

ψ (x)dx)

dy

=1

(2π)n/2

∫Rn

ψ (x)

(1

(2π)n/2

∫Rn

f (y)e−iy·xdy

)dx

1942 CHAPTER 59. BASIC PROBABILITYThat is, for all f EG,1LfO)dHO) = oa LPM aay_ oar I Sly) ( [et wes)ar) ay (59.21.56)I will showfo oar [of (wear) dyis a positive linear functional and then it will follow from 59.21.56 that U is unique. Thus itis needed to show the inside integral in 59.21.56 is nonnegative. First note that the integrandis a positive definite function of x for each fixed y. This follows fromYe PO) y (x —x;) oeKy= x, — Xj —y k ev J ; > 0.Finn) (ela F 2kjLet t > 0 and1 1 |x|?hy (x) = (am)? e4¥Then by dominated convergence theorem,f ey (x)dx=lim |e *y(x) hy (x) dxJR"too JipnLetting d1], = hz; (x) dx, it follows from Lemma 59.21.5 1, = 1; * 1, and since these aresymmetric measures, it follows from Lemma 59.21.4 the above equalslim e Y*y(x)d (n,*,) =0too JIRnThus the above functional is a positive linear functional and so there exists a unique Radonmeasure, jl satisfyingsom ha WOITO)4= op ff ( [Lev ax) dyI —iy-x= aay he V8 (stn rend WE y ‘) dx[fan5