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Master Dissertation

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Of these properties, causality plays a key role in the method of Epstein<br />

and Glaser. Equation (5.4) leads to the condition stated in the following<br />

theorem.<br />

Theorem 5.1. If {x1, . . . , xm} > {xm+1, . . . , xn}, then<br />

Tn(x1, . . . , xn) = Tm(x1, . . . , xm)Tn−m(xm+1, . . . , xn),<br />

Before proving this result we first note that if (5.4) is satisfied,<br />

S(g1 + g2) =<br />

=<br />

∞<br />

n=0<br />

<br />

n 1<br />

λ<br />

n!<br />

d 4 x1 · · · d 4 xnTn(x1, . . . , xn)<br />

× (g1(x1) + g2(x1)) · · · (g1(xn) + g2(xn))<br />

∞ n<br />

λ n<br />

<br />

1<br />

m!(n − m)!<br />

n=0 m=0<br />

d 4 x1 · · · d 4 xnTn(x1, . . . , xn)<br />

× (g2(x1) · · · g2(xm)) · · · (g1(xm+1) · · · g1(xn)),<br />

as there are 2n terms from the product of the test-functions and<br />

ways to pick g2 m times. On the other hand<br />

S(g2)S(g1) =<br />

=<br />

=<br />

∞<br />

m=0<br />

<br />

m 1<br />

λ<br />

m!<br />

d 4 x1 · · · d 4 xmTm(x1, . . . , xm)<br />

× g2(x1) · · · g2(xm)<br />

∞<br />

<br />

k 1<br />

× λ<br />

k!<br />

k=0<br />

∞<br />

m=0 k=0<br />

∞<br />

n=0 m=0<br />

d 4 ˜x1 · · · d 4 ˜xkTk(˜x1, . . . , ˜xk)<br />

× g1(˜x1) · · · g1(˜xk)<br />

∞<br />

<br />

m+k 1<br />

λ<br />

m!k!<br />

d 4 x1 · · · d 4 xmd 4 ˜x1 · · · d 4 ˜xk<br />

× Tm(x1, . . . , xm)Tk(˜x1, . . . , ˜xk)<br />

n!<br />

m!(n−m)!<br />

× g2(x1) · · · g2(x1) · · · g2(xm)g1(˜x1) · · · g1(˜xk)<br />

n<br />

λ n<br />

<br />

1<br />

dx1 · · · dxnTm(x1, . . . , xm)<br />

m!(n − m)!<br />

× Tn−m(xm+1, . . . , xn)g2(x1) · · · g2(xm)<br />

× g1(xm+1) · · · g1(xn).<br />

From the definition of the metric on formal power series we know that<br />

31

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