Dangerously irrelevant operator: Difference between revisions

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In [[statistical mechanics]] and [[quantum field theory]], a '''dangerously irrelevant operator''' (or '''dangerous irrelevant operator''') is an [[operator (mathematics)|operator]] which is irrelevant at a renormalization group fixed point, yet affects the [[infrared]] (IR) physics significantly (e.g. because the [[vacuum expectation value]] (VEV) of some field depends sensitively upon the coefficient of this operator). This term was introduced by Daniel Amit and Luca Peliti in 1982.<ref name=":1">{{Cite journal|last=Amit|first=Daniel J|last2=Peliti|first2=Luca|date=1982|title=On dangerous irrelevant operators|url=https://linkinghub.elsevier.com/retrieve/pii/0003491682901592|journal=Annals of Physics|language=en|volume=140|issue=2|pages=207–231|doi=10.1016/0003-4916(82)90159-2|via=}}</ref>

== Critical phenomena ==

In the theory of critical phenomena, free energy of a system near the critical point depends analytically on the coefficients of generic (not dangerous) irrelevant operators, while the dependence on the coefficients of dangeorously irrelevant operators is non-analytic (<ref name=":0">{{Cite book|last=Cardy|first=John|title=Scaling and Renormalization in Statistical Physics|publisher=Cambridge University Press|year=1996|isbn=|___location=|pages=}}</ref> , p.49).

The presence of dangerously irrelevant operators leads to the violation of the hyperscaling relation <math>\alpha=2-d\nu</math> between the critical exponents <math>\alpha</math> and <math>\nu</math> in <math>d</math> dimensions. The simplest example (<ref name=":0" /> , p.93) is the critical point of the Ising ferromagnet in <math>d\ge4</math> dimensions, which is a gaussian theory (free massless scalar <math>\phi</math>), but the leading irrelevant perturbation <math>\phi^4</math> is dangerously irrelevant. Another example occurs for the Ising model with random-field disorder, where the fixed point occurs at zero temperature, and the temperature perturbation is dangerously irrelevant (<ref name=":0" /> , p.164).

==Quantum field theory==

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[[supersymmetry|Supersymmetric]] models with [[moduli space|a modulus]] can often have dangerously irrelevant parameters.

== Other meaningsuses of the term ==

SometimesConsider onea callsrenormalization group (RG) flow triggered at short distances by a relevant perturbation of an ultra-violet (UV) fixed point, and flowing at long distances to an infra-red (IR) fixed point. It may be possible (e.g. in perturbation theory) to monitor how dimensions of UV operators change along the RG flow. In such a situation, one sometimes<ref>{{Cite journal|last=Gukov|first=Sergei|date=2016-01-05|title=Counting RG flows|url=https://doi.org/10.1007/JHEP01(2016)020|journal=Journal of High Energy Physics|language=en|volume=2016|issue=1|pages=20|arxiv=1503.01474|doi=10.1007/JHEP01(2016)020|issn=1029-8479|via=}}</ref> calls dangerously irrelevant ana UV operator whose scaling dimension, while irrelevant at short distances: <math>\Delta_{\rm UV}>d</math> , receives a negative correction along a renormslizationrenormalization group flow, so that the operator becomes relevant at long distances: <math>\Delta_{\rm IR}<d</math>. This usage of the term is non-standarddifferent andfrom shouldthe beone avoidedoriginally introduced in <ref name=":1" />.

==References==

{{Cite journal | last1 = Amit | first1 = D. | last2 = Peliti | first2 = L. | title = On dangerous irrelevant operators | journal = Annals of Physics | volume = 140 | issue = 2 | pages = 207–231 | year = 1982 | doi = 10.1016/0003-4916(82)90159-2|bibcode = 1982AnPhy.140..207A | arxiv = cond-mat/0108323 }}

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{{DEFAULTSORT:Dangerously Irrelevant Operator}}

[[Category:Renormalization group]]

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