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{{short description|Theorem in quantum field theory}}
{{DISPLAYTITLE:''C''-theorem}}
In
*<math>C(g^{}_i,\mu)</math> decreases monotonically under the [[renormalization group]] (RG) flow. ▼
*At fixed points of the [[RG flow]], which are specified by a set of fixed-point couplings <math>g^*_i</math>, the function <math>C(g^*_i,\mu)=C_*</math> is a constant, independent of energy scale.
The theorem formalizes the notion that theories at high energies have more [[Degrees of freedom (physics and chemistry)|degrees of freedom]] than theories at low energies and that information is lost as we flow from the former to the latter.
==Two-dimensional case==
[[Alexander Zamolodchikov]] proved in 1986 that two-dimensional quantum field theory always has such a ''C''-function. Moreover, at fixed points of the RG flow, which correspond to [[two-dimensional conformal field theory|conformal field theories]], Zamolodchikov's ''C''-function is equal to the [[central charge]] of the corresponding conformal field theory,<ref>
[[John Cardy]] in 1988 considered the possibility to generalise ''C''-theorem to higher-dimensional quantum field theory. He conjectured that in four spacetime dimensions, the quantity behaving monotonically under renormalization group flows, and thus playing the role analogous to the central charge {{mvar|c}} in two dimensions, is a certain anomaly coefficient which came to be denoted as {{mvar|a}}.<ref>{{cite journal | last1 = Cardy | first1 = John | year = 1988 | title = Is there a c-theorem in four dimensions? | journal = Physics Letters B | volume = 215 | issue = 4| pages = 749–752 | doi=10.1016/0370-2693(88)90054-8|bibcode =1988PhLB..215..749C }}</ref>
For this reason, the analog of the ''C''-theorem in four dimensions is called the '''''A''-theorem'''.
In perturbation theory, that is for renormalization flows which do not deviate much from free theories, the ''A''-theorem in four dimensions was proved by [[Hugh Osborn]] using the local renormalization group equation.<ref>{{cite journal | last1 = Osborn | first1 = Hugh | year = 1989 | title = Derivation of a Four-Dimensional c Theorem | journal = Physics Letters B | volume = 222 | issue = 1| pages = 97 | doi=10.1016/0370-2693(89)90729-6|bibcode =1989PhLB..222...97O }}</ref><ref>{{cite journal | last1 = Ian | first1 = Jack| last2 = Osborn | first2 = Hugh | year = 1990 | title = Analogs for the c Theorem for Four-Dimensional Renormalizable Field Theories | url = https://cds.cern.ch/record/205908| journal = Nuclear Physics B | volume = 343 | issue = 3| pages = 647–688 | doi=10.1016/0550-3213(90)90584-Z|bibcode =1990NuPhB.343..647J }}</ref> However, the problem of finding a proof valid beyond perturbation theory remained open for many years.
▲==Four-dimensional case - ''A''-theorem==
In 2011, [[Zohar Komargodski]] and Adam Schwimmer of the [[Weizmann Institute of Science]] proposed a nonperturbative proof for the ''A''-theorem, which has gained acceptance.<ref>{{Cite journal | last1 = Reich | first1 = E. S. | doi = 10.1038/nature.2011.9352 | title = Proof found for unifying quantum principle | journal = Nature | year = 2011 |
==See also==
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[[Category:Conformal field theory]]
[[Category:Renormalization group]]
[[Category:Mathematical physics]]
[[Category:Theorems in
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