Beta function (physics): Difference between revisions

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In [[theoretical physics]], specifically [[quantum field theory]], a '''beta function''', ''β(g)'', encodes the dependence of a [[Coupling constant|coupling parameter]], ''g'', on the [[energy scale]], ''μ'', of a given physical process described by [[quantum field theory]].
It is defined by the '''Gell-Mann–Low equation''' or '''renormalization flow equation,''' given by
It is defined as
:: <math>\beta(g) = \mu \frac{\partial g}{\partial \mu} = \frac{\partial g}{\partial \ln(\mu)} ~,</math>
and, because of the underlying [[renormalization group]], it has no explicit dependence on ''μ'', so it only depends on ''μ'' implicitly through ''g''.
This dependence on the energy scale thus specified is known as the [[Coupling constant#Running coupling|running]] of the coupling parameter, a fundamental
feature of scale-dependence in quantum field theory, and its explicit computation is achievable through a variety of mathematical techniques. The concept of Betabeta function was Introducedfirst introduced by [[Ernst Stueckelberg]] and [[André Petermann]] in 1953.,<ref>{{cite journal |author1-link=Ernst Stueckelberg |last1=Stueckelberg |first1=E.C.G. |author2-link=André Petermann |first2=A. |last2=Petermann |year=1953 |url=https://www.e-periodica.ch/cntmng?pid=hpa-001:1953:26::894 |title=La renormalisation des constants dans la théorie de quanta |journal=Helv. Phys. Acta |volume=26 |pages=499–520 |language=FR}}</ref> and independently postulated by [[Murray Gell-Mann]] and [[Francis E. Low]] in 1954.<ref>{{Cite journal |last=Fraser |first=James D. |date=2021-10-01 |title=The twin origins of renormalization group concepts |url=https://www.sciencedirect.com/science/article/pii/S0039368121001126 |journal=Studies in History and Philosophy of Science Part A |volume=89 |pages=114–128 |doi=10.1016/j.shpsa.2021.08.002 |issn=0039-3681}}</ref>
 
==Scale invariance==