Volume 2 - LENR-CANR

2 16 2
gc
27 3
So, a solution for the ideal plasma exists. More in detail, we can define:
k k
a
(11)
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2
g0
3
In this case the coupling critical constant is:
k g0 Ak
(12)
i
A k A
k g0
k
2
(13)
so to admit the following holding quantity:
A A A A *
*
i
Q A
k Ak
k k k k
kk
*
*
2
(14)
while for the Hamiltonian’s it is easy to compute:
*
*
A A
E
N
p
1
*
H Q A
k A
k ig
2
k k k
k
(15)
With the aim of seeing if there are any externals solutions, we write
k
i
uke
(16)
i
Ak Auke
(17)
where and A are positive constants and uk is a complex vector.
Changing these ones in (12) and (13) we have:
2
(18)
A
g0
(19)
1 2
3 2
g0
2
0
(20)
and by the condition Q=0 (we cannot have a net charge flow in a plasma), we have:
2
0 1 2
g
0
In this case it is easy to observe that for
(18) and (19) are satisfied.
g
0
2
3
558
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it is unlikely that both the equations
(21)