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We will say that the field
is of an ``essentially RPA'' type if:
- The phase factors are statistically independent and uniformly
distributed variables up to
corrections, i.e.
![$\displaystyle {\cal P}^{(N)} \{s, \xi \} = {1 \over (2 \pi)^{N} } {\cal P}^{(N,a)} \{s \} \; [1 + O({\epsilon}^2)],$](img113.png) |
(17) |
where
 |
(18) |
is the
-mode amplitude PDF.
- The amplitude variables are almost independent is a sense that for
each
modes the
-mode amplitude PDF is equal to the
product of the one-mode PDF's up to
and
corrections,
![$\displaystyle {\cal P}^{(M)}_{j_1, j_2, \dots , j_M} = P^{(a)}_{j_1} P^{(a)}_{j_2} \dots P^{(a)}_{j_M} \; [1 + O(M/N) + O({\epsilon}^2)].$](img116.png) |
(19) |
Dr Yuri V Lvov
2007-01-23