We now calculate the expectation value
Only the field-even part of the action will yield a non-zero result, so that we have
Using the form of
shown in
Equation (A.2) we get for this expectation value
![\begin{eqnarray*}
\lefteqn
{
\left\langle
S_{V}[\vec{\varphi}']
\right\rang...
...arphi_{\mathfrak{N}}'^{4}(n_{\mu})
\right\rangle_{0}
\right\}.
\end{eqnarray*}](img319.png)
Most of the remaining expectation values can be written in terms of
and
, if we recall that it can be shown that
for
we have
while for
we have, in a similar way,
as one can find in Appendix B, Equation (B.8). Given all this, we may write for our expectation value
![\begin{eqnarray*}
\left\langle
S_{V}[\vec{\varphi}']
\right\rangle_{0}
& = &...
...}
+
\frac{3\lambda}{4}\,
\sigma_{\mathfrak{N}}^{4}
\right\}.
\end{eqnarray*}](img322.png)
The remaining expectation value of the sum shown can be found in Appendix B, Equation (B.15),
Using this result we get for our expectation value
![\begin{eqnarray*}
\left\langle
S_{V}[\vec{\varphi}']
\right\rangle_{0}
& = &...
...2}
+
\frac{3\lambda}{4}\,
\sigma_{\mathfrak{N}}^{4}
\right].
\end{eqnarray*}](img324.png)
Note that all the sums can now be done, so that we can write our result in the simpler form