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˄
−ₒ R is more complicated and is determined by the moves
The definition of
˄
−ₒ
ʔ k
ʔ k + 1 .Foragiven k this move means that
˄
−ₒ
ʔ k
=
p i ·
s i ,
ʔ k + 1 =
p i ·
ʓ i ,
s i
ʓ i
i I
i I
So for each k we let
−ₒ R
s i = s
˄
ʓ k + 1
i
( s , k )
p i ·
This definition ensures
(c) ( ʔ k
˄
−ₒ R ( ʔ k + 1 ) k + 1 ;
) k
(d) ( ʔ k ) k
is stable.
This completes our definition of the deterministic pLTS underlying the required
resolution; it remains to find subdistributions ʘ , ʘ over R such that ʔ
=
Img f ( ʘ ),
ʔ =
ʘ .
Because of (b) (c) and (d), we have the following extreme derivation, which by
part (ii) of Lemma 6.7 is the unique one from ʔ 0 :
Img f ( ʘ ) and ʘ
ʔ 0
( ʔ 0
) 0
( ʔ 0 ) 0
=
+
˄
−ₒ R
( ʔ 0
) 0
( ʔ 1
) 1
( ʔ 1 ) 1
+
.
.
˄
−ₒ R ( ʔ k + 1 ) k + 1
( ʔ k + 1 ) k + 1
. ————————
( ʔ k
) k
+
ʘ = k = 0 ( ʔ k ) k
Letting ʘ be ʔ 0 , we see that (a) above ensures ʔ
=
Img f ( ʘ ); the same note and
the linearity of f applied to distributions also gives ʔ =
Img f ( ʘ ).
The converse is somewhat simpler.
Proposition 6.5 (Extreme Derivatives from Resolutions) Suppose
R , ʘ ,
R
is
a resolution of a subdistribution ʔ inapLTS
S , ʩ ˄ ,
with resolving function f .
Then ʘ R ʘ implies ʔ Img f ( ʘ ) .
Proof Consider any derivation of ʘ
R ʘ along the lines of Definition 6.4 .
By systematically applying the function f to the component subdistributions in this
derivation we get a derivation Img f ( ʘ )
Img f ( ʘ ).
To show that Img f ( ʘ ) is actually an extreme derivative it suffices to show that s is
stable for every s
Img f ( ʘ ), that is, ʔ
Img f ( ʘ )
Img f ( ʘ )
. But if s
, then by definition there is
R ʘ the state t must be stable.
The stability of s now follows from requirement (iii) of Definition 4.3.
ʘ
some t
such that s
=
f ( t ). Since ʘ
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