Difference between revisions of "Tree level"

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(Created page with "In the context of perturbation theory, a '''tree-level''' Feynman diagram is a topology contributing to the probability amplitude for a scattering process which contai...")
 
 
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[[Category:Perturbation theory]]
 
In the context of [[perturbation theory]], a '''tree-level''' [[Feynman diagram]] is a topology contributing to the probability amplitude for a scattering process which contains no closed [[loops]]. If the [[S-matrix]] elements for a process with given initial and final states receive contributions from tree-level diagrams (i.e. the tree-level diagrams are also the lowest order in perturbation theory in which this process is first described), such graphs also constitute the [[leading-order]] diagrams.
 
In the context of [[perturbation theory]], a '''tree-level''' [[Feynman diagram]] is a topology contributing to the probability amplitude for a scattering process which contains no closed [[loops]]. If the [[S-matrix]] elements for a process with given initial and final states receive contributions from tree-level diagrams (i.e. the tree-level diagrams are also the lowest order in perturbation theory in which this process is first described), such graphs also constitute the [[leading-order]] diagrams.

Latest revision as of 15:49, 6 April 2017

In the context of perturbation theory, a tree-level Feynman diagram is a topology contributing to the probability amplitude for a scattering process which contains no closed loops. If the S-matrix elements for a process with given initial and final states receive contributions from tree-level diagrams (i.e. the tree-level diagrams are also the lowest order in perturbation theory in which this process is first described), such graphs also constitute the leading-order diagrams.