370 Handbook of Discrete-Valued Time Series
where β =(k
B
T)
−1
≥0with T denoting the Kelvin temperature and k
B
denoting the
Boltzmann constant, while Z
β
= exp{−βH(y)} is a partition function (or, normalizing
y
constant). When the parameter β in (17.8) surpasses a threshold value, a phase transition
from short-range to long-range interactions would occur, resulting in an ordered phase
with nonzero limiting correlation (see, e.g., Pickard, 1976, 1977).
17.1.2 Spatio-Temporal Autologistic Model
For spatio-temporal binary data, let Y
i,t
∈{±1} denote the binary response variable with
y
i,t
denoting a realization at site i = 1, ..., n and time t.Let Y
t
= (Y
1,t
, ..., Y
n,t
)
denote the
vector of binary responses with realizations y
t
= (y
1,t
, ..., y
n,t
)
at all sites and a given time
point t. Bartlett (1971, 1972) developed a Markov process with
P(Y
i,t+t
= y
i,t
|y
t
) = 1 − λ(t){1 − F
i
(y
t
)}, (17.9)
where λ ≥ 0, t ≥ 0, and F
i
(y
t
) is a function of y
t
. The joint probability density of Y
t
, when
the Markov process is at equilibrium, is
n n
p(y
t
) = c(α, θ) exp
−α
y
i,t
− θ y
i,t
z
i,t
, (17.10)
i=1 i=1
where α and θ are two coefcients, under the condition that
n n
∗
{1 − F
i
(y
t
)}= {1 − F
i
(y˜
i,t
)}exp(2αy
i,t
+ 4θy
i,t
z
i,t
), (17.11)
i=1 i=1
where z
i,t
denotes a linear combination of y
j,t
for j = i, z
i
∗
,t
is a symmetrized form of z
i,t
(e.g., in the one-dimensional space, if z
i,t
= y
i−1,t
, then 2z
i
∗
,t
= y
i−1,t
+ y
i+1,t
), and y˜
i,t
=
(y
1,t
, ..., y
i−1,t
, −y
i,t
, y
i+1,t
, ..., y
n,t
)
.
A direct and symmetric solution to Equation (17.11) is
1 − F
i
(y
t
) = exp(αy
i,t
+ 2θy
i,t
z
∗
i,t
)f (αy
i,t
, θy
i,t
z
∗
i,t
), (17.12)
where f is a suitable, positive function, and even in both y
i,t
and y
i,t
z
i
∗
,t
.
Now, on a square lattice, let Y
i,i
,t
∈{0, 1} denote the binary response with a realization
y
i,i
,t
at row i, column i
,and time t. Besag (1972) proposed a Markov process of binary
responses developing through time on the square lattice, which can be viewed as a special
case of Bartlett (1971, 1972). In particular, for xed α
y
, θ
y,1
,and θ
y,2
,
P
Y
i,i
,t+t
= y|Y
i,i
,t
= y, y
·,·,t
:t
≤t+t
, excluding y
i,i
,t+t
=
1 + t exp
α
y
+ θ
y,1
(y
i−1,i
,t
+ y
i+1,i
,t
) + θ
y,2
(y
i,i
−1,t
+ y
i,i
+1,t
)
−1
+ o(t)
= 1 − t exp
α
y
+ θ
y,1
(y
i−1,i
,t
+ y
i+1,i
,t
) + θ
y,2
(y
i,i
−1,t
+ y
i,i
+1,t
)
+ o(t), (17.13)