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3.3
Lifting Relations
In the probabilistic setting, formal systems are usually modelled as distributions over
states. To compare two systems involves the comparison of two distributions. So we
need a way of lifting relations on states to relations on distributions. This is used,
for example, to define probabilistic bisimulation as we shall see in Sect. 3.5 . A few
approaches of lifting relations have appeared in the literature. We will take the one
from [ 22 ], and show its coincidence with two other approaches.
Definition 3.2
Given two sets S and T and a binary relation
R
S
×
T , the lifted
relation
R
D
( S )
× D
( T ) is the smallest relation that satisfies:
t .
(1) s
R
t implies s
R
I implies ( i I p i ·
( i I p i ·
ʘ i for all i
(2) (Linearity) ʔ i
R
ʔ i )
R
ʘ i ),
where I is a finite index set and i I p i =
1.
The are alternative presentations of Definition 3.2 . The following is used in many
proofs.
Proposition 3.1
Let ʔ and ʘ be two distributions over S and T , respectively, and
R
×
R
ʘ if and only if there are two collections of states,
{
s i } i I
S
T . Then ʔ
{
t i } i I , and a collection of probabilities
{
p i } i I , for some finite index set I , such
and
that i I p i =
1 and ʔ , ʘ can be decomposed as follows:
1. ʔ = i I p i · s i .
2. ʘ = i I p i · t i .
3. For each i I we have s i Rt i .
= i I p i ·
Proof
(
) Suppos e we can decompose ʔ and ʘ as follows: (i) ʔ
s i ,
= i I p i ·
(ii) ʘ
t i , a n d (ii i) s i R
t i for each i
I . By (iii) and the first rule in
t i for each i
Definition 3.2 ,wehave s i R
I . By the second rule in Definition 3.2
we obtain that ( i I p i ·
( i I p i ·
ʘ .
s i )
R
t i ), that is ʔ
R
(
) We proceed by rule induction.
ʘ because ʔ
• f ʔ
R
=
s , ʘ
=
t and s
R
t , then we can simply take I to be the
singleton set
{
i
}
with p i =
1 and ʘ i =
ʘ .
= i I p i ·
ʔ i , ʘ i = i I p i ·
ʘ because of the conditions ʔ
• f ʔ
R
ʘ i for
some index set I , and ʔ i
R
ʘ i for each i
I , the n by induction hyp ot hesis
there are index sets J i such that ʔ i = j J i p ij ·
s ij , ʘ i = j J i p ij ·
t ij , and
= i I j J i p i p ij ·
s ij R
t ij for each i
I an d j
J i . It follows that ʔ
s ij ,
= i I j J i p i p ij ·
ʘ
t ij , and s ij R
t ij for each i
I and j
J i . Therefore, it
suffices to take
{
ij
|
i
I , j
J i }
to be the index set and
{
p i p ij |
i
I , j
J i }
be the collection of probabilities.
An important point here is that in the decomposition of ʔ into i I p i ·
s i , the states
s i are not necessarily distinct : that is, the decomposition is not in general unique.
Thus when establishing the relationship between ʔ and ʘ , a given state s in ʔ may
play a number of different roles. This is reflected in the following property.
 
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