Volume 2 - LENR-CANR

For a system with N charge Q of m mass within a V volume the plasma frequency can be
written as:
Qe
k p
m
N
V
(1)
Introducing the dimensional variable t we can rewrite the above equations as follows:
1 *
n ( )
n kr
kra
kr
kra
n
n
( )
2
k
nr
p
p
1
kr i kr mkr
2
Defining the state as:
i *
*
kr
n a n
n ( t)
n(
)
2
nn
(3)
( ) n
n
n
and the e.m. field amplitude as:
A d k
kr
kr
3 (5)
8
r
we can rewrite as follows:
t
2
Aa A a
3
(6)
i
A A imA
a
2
2
3
(7)
If we only concentrate on a short time dynamics, we can write:
( 0)
0
(8)
then, creating a difference in the (6) and using the (7) with 0 , we can easily obtain:
i 2
A
j A
j
0 a j,
al
0
2 3
(9)
2
Al
Aj 3
(10)
This has the same form of the equations of the coherence domains as the case in which:
0
0
2 2
g
3
557
(2)
(4)