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The Binary Case
When q = 0, a state description (1) cannot be expressed as a conjunction of
sentences each involving only one constant as it is in the unary case with atoms,
but it is possible to define binary atoms and proceed similarly 3 .
For this purpose, we define ʲ 1 ( x ) ,...,ʲ 2 p + q ( x ) to be the formulae
p
q
i =1 ±
i =1 ±
R i ( x )
Q i ( x, x )
and ʴ 1 ( x, y ) ,...,ʴ 2 q ( x, y ) to be the formulae i =1 ±
Q i ( x, y ) . We define the
binary atoms to be the formulae
ʳ [ k,c,h,d ] ( x, y )= ʲ k ( x ) ∧ ʲ c ( y ) ∧ ʴ h ( x, y ) ∧ ʴ d ( y,x )
1 ,..., 2 p + q
1 ,..., 2 q
where k,c
.
The state description (1) can then be also expressed as
∈{
}
and h, d
∈{
}
m
ʲ v j ( a j )
ʳ h j,l ( a j ,a l )
j =1
1
j<l
m
where v j ∈{
. There
is some redundancy in this expression but it is convenient for what follows.
We also need the concept of a partial state description which is a sentence
ʔ ( a 1 ,...,a m )oftheform
1 ,..., 2 p + q
}
and h j,l ∈{
[ v j ,v l ,h,d ]: h, d
∈{
1 ,..., 2 q
}}
m
ʲ v j ( a j )
ʳ h j,l ( a j ,a l )
(2)
j =1
j,l∈A
where v j and h j,l are as above and A
.
Clearly every state description is a partial state description. We define the
signature of the (partial) state description (2) to be mn such that
ↆ{
j, l
:1
j<l
m
}
m =
m 1 ,...,m 2 p + q
,
where m k is the number of j ∈{ 1 ,...,m} such that v j = k and
1 ,..., 2 p + q
1 ,..., 2 q
n =
n [ k,c,h,d ] : k,c
∈{
}
and h, d
∈{
}
,
where n [ k,c,h,d ] is the number of
j, l
A such that
h j,l =[ k,c,h,d ]or h j,l =[ c, k, d, h ] .
(3)
The atoms ʳ [ k,c,h,d ] and ʳ [ c,k,d,h ] are counted together because
ʳ [ k,c,h,d ] ( x, y )= ʳ [ c,k,d,h ] ( y,x )
(4)
3 The concepts and results in this section come from [9].
 
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