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F
ij
(
x
)
0, elsewhere.
Eventually, we define the random global dynamic frustration
D
by:
¼
Dx
ðÞ¼Σ
i ; j2f
1
;ng
D
ij
ð
ð
t
x
ð
t
ÞÞ;
where
D
ij
is the local dynamic frustration of the pair (
i
,
j
) defined by:
D
ij
ð
x
ð
t
ÞÞ ¼
;
α
ij
¼
;
x
i
ð
t
Þ 6¼
h
ðΣ
j
2Ni
w
ij
x
j
ð
t
Þθ
i
Þ
α
ij
¼
;
1
if
1
or
1
x
i
ð
t
Þ¼
h
ðΣ
j
2Ni
w
ij
x
j
ð
t
Þθ
i
Þ;
D
ij
(
x
(
t
))
0, elsewhere.
Then we prove the following Proposition 1:
¼
Proposition 1.
Let us consider the random energy U and the random frustration F
of a getBren N having a constant absolute value w for its interaction weights, null
threshold
Θ
, temperature T equal to 1 and being sequentially updated, then:
1.
U(x)
F(x),
where Q
+
(N) is the number of positive
edges in the interaction graph G of the network
2.
E
μ
(
U
)
¼ Σ
i, j2{1,n}
α
ij
x
i
x
j
¼
Q
+
(N)
¼
∂
log
Z/
w, where the free energy
log
Z is equal to the quantity
log(
Σ
y2Ω
∂
exp(
Σ
j2y,k2y
w
ij
y
j
y
k
))
and
μ
is the invariant Gibbs measure defined by:
8
x
2Ω
,
μ
({
x
})
¼
exp(
Σ
i2x,j2x
w
ij
x
i
x
j
)/Z
3.
Var
μ
U
¼
Var
μ
F
¼
∂
E
μ
/
log
w, where E
μ
¼Σ
x2Ω
μ
({
x
})log(
μ
({
x
}))
¼
∂
log
Z
-
wE(U) is the entropy of
μ
, maximal among entropies corresponding to all
probability distributions
for the U's having the same given expectation
ν
E
ν
(U)
¼
E
μ
(U).
Proof.
1. It is easy to check that:
U
(
x
)
F
(
x
)
,
2. The expectation of
U
, denoted
E
μ
(
U
), is given by:
¼
Q
+
(
N
)
E
μ
ð
U
Þ¼Σ
x2Ω
Σ
i2x; j2x
α
ij
x
i
x
j
exp
ðΣ
i2x; j2x
wx
i
x
j
Þ=
Z
¼ @
log
Z
=@
w
3. Following Demongeot and Waku (
2012a
,
b
and
submitted
), we have Var
μ
U
¼
Var
μ
F
log
w
, and according to Demongeot et al. (
2008b
),
Demongeot and Sen´ (
2008
), Demetrius (
1983
,
1997
), K¨hn (
2010
), and
Fogelman Souli´ et al. (
1989
),
E
μ
¼
∂
E
μ
/
∂
is maximal among the proposed set of
entropies.
∎
Proposition 2.
Let us consider the getBren N with T
¼
0, sequentially or synchro-
nously updated, defined from a potential P defined by:
t
xA
k
x
t
xWx
8
x
2 Ω;
P
ð
x
Þ¼Σ
k
ð
Þ
x
k
þ
þ Θ
x
;
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