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In [[computer science]], '''partial order reduction''' is a technique for reducing the size of the [[State transition system|state-space]] to be searched by a [[model checking]] algorithm. It exploits the commutativity of concurrently executed transitions, which result in the same state when executed in different orders.
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In explicit state space exploration, partial order reduction usually refers to the specific technique of expanding a representative subset of
all enabled transitions. This technique has also been described as model checking with representatives {{harv|Peled|1993}}.
There are various versions of the method, the so-called stubborn set method {{harv|Valmari|1990}}, ample set method {{harv|Peled|1993}}, and
persistent set method {{harv|Godefroid|1994}}.
 
== Ample sets ==
Ample sets are an example of model checking with representatives. Their formulation relies on a separate notion of ''dependency''.  Two transitions are considered '''independent''' only if whenever they are mutually enabled, they cannot disable another
and the execution of both results in a unique state regardless of the order in which they are executed.
Transitions that are not independent, are dependent.
In practice dependency is approximated using static analysis.
 
Ample sets for different purposes can be defined by giving conditions as to when a set
of transitions is "ample" in a given state.
 
'''C0''' <math> {ample(s)=\empty} \iff {enabled(s)=\empty} </math>
 
'''C1''' If a transition <math> \alpha </math> depends on some transition relation in ample(s), this transition cannot be invoked until some transition in the ample set executed.
 
Conditions C0 and C1 are sufficient for preserving all the deadlocks in the state space.
Further restrictions are needed in order to preserve more nuanced properties. For instance,
in order to preserve properties of linear temporal logic, the following two conditions are needed:
 
'''C2''' If <math> enabled(s) \neq ample(s) </math>, each transition in the ample set is invisible
 
'''C3''' A cycle is not allowed if it contains a state in which some transition <math>\alpha</math>  is enabled, but is never included in ample(s) for any states s on the cycle.
 
These conditions are sufficient for an ample set, but not necessary conditions {{harv|Clarke|1999}}.
 
== Stubborn sets ==
Stubborn sets make no use of an explicit independence relation. Instead they are defined solely through commutativity over
sequences of actions. A set <math>T(s)</math> is (weakly) stubborn at s, if the following hold.
 
'''D0''' <math>\forall a \in T(s) \forall b_1,...,b_n \notin T(s) </math>, if execution of the sequence <math>b_1,...,b_n,a</math> is possible and leads to the state <math>s'</math>, then execution of the sequence <math>a, b_1,...,b_n</math> is possible and will lead to state <math>s'</math>
 
'''D1''' Either <math>s</math> is a deadlock, or <math>\exists a \in T(s)</math> such that <math>\forall b_1,...,b_n \notin T(s) </math>, the execution of <math>b_1,...,b_n,a</math> is possible.
 
These conditions are sufficient for preserving all deadlocks, just like C0 and C1 are in the ample set method.
They are, however, somewhat weaker, and as such may lead to smaller sets. The conditions C2 and C3 can also be
further weakened from what they are in the ample set method, but the stubborn set method is compatible with C2 and C3.
== Others ==
 
There are also other notations for partial order reduction. One of the commonly used is the persistent set/sleep set algorithm.
Detailed information can be found in Patrice Godefroid's thesis {{harv|Godefroid|1994}}.
 
In symbolic model checking, partial order reduction can be achieved by adding more constraints (guard strengthening).
 
== References ==
* {{Cite book | first=Antti |last=Valmari |chapter=Stubborn sets for reduced state space generation | title=Advances in Petri Nets 1990, LNCS 483, Springer 1991 |year=1990| pages=491–515|ref=harv}}
* {{Cite book |first=Doron A. |last=Peled |chapter=All from One, One for All: Model Checking Using Representatives |title=Proceedings of CAV'93, LNCS 697, Springer 1993 |year=1993 |pages=409–423 |ref=harv}}
* {{cite book |first=Edmund M |last=Clarke |coauthors=Orna Grumberg and Doron A. Peled |title=Model Checking |publisher=MIT Press |year=1999 |ref=harv}}
* {{cite journal |first=Patrice |last=Godefroid |title=Partial-Order Methods for the Verification of Concurrent Systems -- An Approach to the State-Explosion Problem |type=PhD. thesis |publisher=University of Liege, Computer Science Department |year=1994 |url=http://cm.bell-labs.com/who/god/public_psfiles/thesis.ps |format=PostScript |ref=harv}}
* {{cite book |url=http://spinroot.com/spin/Doc/Book_extras/ |title=The Spin Model Checker: Primer and Reference Manual |first=Gerard J |last=Holzmann |author-link=Gerard J. Holzmann |year=1993 |publisher=Addison-Wesley |isbn=0-321-22862-6}}
 
[[Category:Model checking]]

Revision as of 09:54, 12 February 2014

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