Non-linear sigma model: Difference between revisions

Revision as of 17:33, 10 July 2020

Latest revision as of 07:03, 4 July 2025

(15 intermediate revisions by 10 users not shown)

Line 1:

{{Short description|Class of quantum field theory models}}

In [[quantum field theory]], a '''nonlinear ''σ'' model''' describes a [[scalar field]] {{mvar|Σ}} whichthat takes on values in a nonlinear manifold called the '''target manifold''' &nbsp;''T''. The non-linear ''σ''-model was introduced by {{harvtxt|Gell-Mann|Lévy|1960|loc=section §6}}, who named it after a field corresponding to a spinless[[spin (physics)|sp]] [[meson]] called ''σ'' in their model.<ref>{{Citation | last2=Lévy | first1=M. | last1=Gell-Mann | first2=M. | s2cid=122945049 | title=The axial vector current in beta decay | publisher=Italian Physical Society | doi=10.1007/BF02859738 | year=1960 | journal=Il Nuovo Cimento | issn=1827-6121 | volume=16 | issue=4 | pages=705–726| bibcode=1960NCim...16..705G }}</ref> This article deals primarily with the quantization of the non-linear sigma model; please refer to the base article on the [[sigma model]] for general definitions and classical (non-quantum) formulations and results.

==Description==

Line 5 ⟶ 6:

The target manifold ''T'' is equipped with a [[Riemannian metric]]&nbsp;''g''. {{mvar|Σ}} is a differentiable map from [[Minkowski space]] ''M'' (or some other space) to&nbsp;''T''.

The [[Lagrangian density]] in contemporary chiral form<ref>{{Cite journal | last1 = Gürsey | first1 = F. | s2cid = 122270607 | title = On the symmetries of strong and weak interactions | doi = 10.1007/BF02860276 | journal = Il Nuovo Cimento | volume = 16 | issue = 2 | pages = 230–240 | year = 1960 | pmid = | pmc = | bibcode = 1960NCim...16..230G }}</ref> is given by

:<math>\mathcal{L}={1\over 2}g(\partial^\mu\Sigma,\partial_\mu\Sigma)-V(\Sigma)</math>

where we have used a +&nbsp;−&nbsp;−&nbsp;− [[metric signature]] and the [[partial derivative]] {{math| ''∂Σ''}} is given by a section of the [[jet bundle]] of ''T''&times;''M'' and {{mvar|V}} is the potential.

Line 13 ⟶ 14:

In more than two dimensions, nonlinear ''σ'' models contain a dimensionful coupling constant and are thus not perturbatively renormalizable.

Nevertheless, they exhibit a non-trivial ultraviolet fixed point of the renormalization group both in the lattice formulation<ref>{{cite book | last = Zinn-Justin | first= Jean | title= Quantum Field Theory and Critical Phenomena | publisher = Oxford University Press | date = 2002 }}</ref><ref>{{ cite book | last= Cardy | first= John L. | title = Scaling and the Renormalization Group in Statistical Physics | publisher = Cambridge University Press | date = 1997 }}</ref> and in the double expansion originally proposed by [[Kenneth G. Wilson]].<ref>{{cite journal|last=Brezin|first=Eduard|year=1976|title=Renormalization of the nonlinear sigma model in 2 + epsilon dimensions|url=|journal=Physical Review Letters|volume=36|issue=13|pages=691–693|bibcode=1976PhRvL..36..691B|doi=10.1103/PhysRevLett.36.691|pmid=|access-date=|author2=Zinn-Justin, Jean}}</ref>

In both approaches, the non-trivial renormalization-group fixed point found for the [[n-vector model|''O(n)''-symmetric model]] is seen to simply describe, in dimensions greater than two, the critical point separating the ordered from the disordered phase. In addition, the improved lattice or quantum field theory predictions can then be compared to laboratory experiments on [[critical phenomena]], since the ''O(n)'' model describes physical [[Heisenberg ferromagnet]]s and related systems. The above results point therefore to a failure of naive perturbation theory in describing correctly the physical behavior of the ''O(n)''-symmetric model above two dimensions, and to the need for more sophisticated non-perturbative methods such as the lattice formulation.

Line 24 ⟶ 25:

==Renormalization==

This model proved to be relevant in string theory where the two-dimensional manifold is named '''[[worldsheet]]'''. Appreciation of its generalized renormalizability was provided by [[Daniel Friedan]].<ref name="Frie80">

{{cite journal|last=Friedan|first=D.|authorlinkauthor-link=Daniel Friedan|title=Nonlinear models in 2+ε dimensions | journal = Physical Review Letters| volume = 45 | issue = 13| pages = 1057–1060 | year = 1980 |doi= 10.1103/PhysRevLett.45.1057 | bibcode=1980PhRvL..45.1057F|url=https://digital.library.unt.edu/ark:/67531/metadc841801/}}</ref> He showed that the theory admits a renormalization group equation, at the leading order of perturbation theory, in the form

:<math>\lambda\frac{\partial g_{ab}}{\partial\lambda}=\beta_{ab}(T^{-1}g)=R_{ab}+O(T^2)~,</math>

{{math|''R_ab''}} being the [[Ricci tensor]] of the target manifold.

Line 30 ⟶ 31:

This represents a [[Ricci flow]], obeying [[Einstein field equations]] for the target manifold as a fixed point. The existence of such a fixed point is relevant, as it grants, at this order of perturbation theory, that [[conformal field theory|conformal invariance]] is not lost due to quantum corrections, so that the [[quantum field theory]] of this model is sensible (renormalizable).

Further adding nonlinear interactions representing flavor-chiral anomalies results in the [[Wess–Zumino–Witten model]],<ref>{{cite journal |first=E. |last=Witten |s2cid=122018499 |title=Non-abelian bosonization in two dimensions |journal=[[Communications in Mathematical Physics]] |volume= 92| issue= 4 |year=1984 | pages= 455–472 | doi= 10.1007/BF01215276|bibcode = 1984CMaPh..92..455W |url=http://projecteuclid.org/euclid.cmp/1103940923 }}</ref> which

augments the geometry of the flow to include [[Torsion tensor|torsion]], preserving renormalizability and leading to an [[infrared fixed point]] as well, on account of [[teleparallelism]] ("geometrostasis").<ref>{{Cite journal | last1 = Braaten | first1 = E. | last2 = Curtright | first2 = T. L. | last3 = Zachos | first3 = C. K. | doi = 10.1016/0550-3213(85)90053-7 | title = Torsion and geometrostasis in nonlinear sigma models | journal = Nuclear Physics B | volume = 260 | issue = 3–4 | pages = 630 | year = 1985 | pmid = | pmc = |bibcode = 1985NuPhB.260..630B }}</ref>

{{further|Ricci flow}}

Line 50 ⟶ 51:

* [[Little Higgs]]

* [[Skyrmion]], a soliton in non-linear sigma models

* [[Polyakov action]]

* [[WZW model]]

* [[Fubini–Study metric]], a metric often used with non-linear sigma models

Line 59 ⟶ 61:

==External links==

* Ketov,{{cite S.journal V|doi=10. [http:4249//www.scholarpedia.org/article/Nonlinear_Sigma_model ''8508|title=Nonlinear Sigma model''] on |year=2009|last1=Ketov|first1=Sergei|journal=Scholarpedia|volume=4|issue=1|page=8508|bibcode=2009SchpJ...4.8508K|doi-access=free}}

* {{cite journal |doi=10.1023/A:1021009008129|year=2002|last1=Kulshreshtha|first1=U.|last2=Kulshreshtha|first2=D. S.|s2cid=115710780|title=Front-Form Hamiltonian, Path Integral, and BRST Formulations of the Nonlinear Sigma Model|journal=International Journal of Theoretical Physics|volume=41|issue=10|pages=1941–1956}}

* U. Kulshreshtha, D.S. Kulshreshtha and H.J.W. Mueller-Kirsten, ``Gauge invariant O(N) [[nonlinear sigma model]](s) and gauge invariant Klein-Gordon theory: Wess-Zumino terms and Hamiltonian and BRST formulations``, Helv.Phys.Acta 66 752-794 (1993); U. Kulshreshtha and D.S. Kulshreshtha, ``Front-form Hamiltonian, path integral and BRST formulations of the [[nonlinear sigma model]]``, Int. J. Theor. Phys. 41, 1941-1956 (2002), DOI: 10.1023/A:1021009008129.

{{Quantum field theories}}

Line 67 ⟶ 69:

[[Category:Quantum field theory]]

[[Category:Mathematical physics]]

[[Category:Murray Gell-Mann]]