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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
,
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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