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1325:{\displaystyle =\,i\,{\bar {\psi }}_{La}\partial \!\!\!/\psi _{L}^{a}+\,i\,{\bar {\psi }}_{Ra}\partial \!\!\!/\psi _{R}^{a}+{\frac {\lambda }{N}}\,\left({\bar {\psi }}_{La}\psi _{R}^{b}\right)\left({\bar {\psi }}_{Rb}\psi _{L}^{a}\right).}
663:{\displaystyle {\mathcal {L}}=\,i\,{\bar {\psi }}_{L}\partial \!\!\!/\psi _{L}+\,i\,{\bar {\psi }}_{R}\partial \!\!\!/\psi _{R}+\lambda \,\left({\bar {\psi }}_{L}\psi _{R}\right)\left({\bar {\psi }}_{R}\psi _{L}\right).}
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acting upon the left-handed flavors and right-handed flavors respectively is the chiral symmetry (in other words, there is no natural correspondence between the left-handed and the right-handed flavors),
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and is defined in a spacetime with an even number of dimensions. It is still important and is used primarily as an effective although not rigorous low energy substitute for quantum chromodynamics.
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The model is quite technical, although based essentially on symmetry principles. It is an example of the importance of
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Chiral symmetry forbids a bare mass term, but there may be chiral condensates. The global symmetry here is SU(
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The Rise of the
Standard Model: A History of Particle Physics from 1964 to 1979
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from fermion interactions inspired many theories of the breaking of
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flavors and the flavor indices represented by the Latin letters
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1427:Since the Nambu–Jona-Lasinio model is
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60: –
59:
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54:Find sources:
48:
44:
38:
37:
32:This article
30:
26:
21:
20:
2212:
2141:Quantum foam
2081:Stueckelberg
2065:
2035:Chern–Simons
1972:Supergravity
1711:Supergravity
1696:Gauge theory
1594:
1590:
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1558:
1545:
1518:
1514:
1504:
1477:
1473:
1463:
1437:UV completed
1426:
1422:chiral limit
1411:
1399:pseudoscalar
1396:
1391:
1388:axial charge
1370:
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1346:
1338:
1336:
801:
797:
793:
789:
787:
772:
676:
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456:
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151:Cooper pairs
130:
126:
120:
105:
96:
86:
79:
72:
65:
53:
41:Please help
36:verification
33:
2023:Topological
1937:Wess–Zumino
1850:Sine-Gordon
1840:Gross–Neveu
1749:Born–Infeld
1716:Thermal QFT
1357:× U(1)
1353:× U(1)
779:confinement
229:technicolor
199:strangeness
99:August 2009
2234:Categories
1804:Yang–Mills
1597:: 192–193.
1455:References
705:×U(1)
227:, such as
221:condensate
159:BCS theory
69:newspapers
2213:See also:
1932:Super QCD
1886:Liouville
1874:Conformal
1845:Schwinger
1369:×SU(
1361:where SU(
1345:×SU(
1301:ψ
1285:¯
1282:ψ
1254:ψ
1238:¯
1235:ψ
1217:λ
1198:ψ
1186:∂
1171:¯
1168:ψ
1142:ψ
1130:∂
1115:¯
1112:ψ
1059:ψ
1049:γ
1036:¯
1033:ψ
1010:ψ
1000:γ
987:¯
984:ψ
972:−
958:ψ
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919:ψ
906:¯
903:ψ
875:λ
861:ψ
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737:λ
717:λ
684:λ
644:ψ
631:¯
628:ψ
605:ψ
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589:ψ
576:λ
564:ψ
552:∂
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516:ψ
504:∂
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367:−
359:ψ
353:¯
350:ψ
334:ψ
328:¯
325:ψ
303:λ
295:ψ
284:∂
278:¯
275:ψ
155:electrons
2009:Type IIB
2004:Type IIA
1989:4D N = 8
1984:4D N = 1
1953:6D (2,0)
1917:4D N = 1
1896:Polyakov
1855:Thirring
1664:Theories
1553:(1997).
1443:See also
777:(but no
231:and the
173:Overview
135:nucleons
2111:History
2094:Related
1891:Minimal
1742:Regular
1523:Bibcode
1482:Bibcode
1420:in the
1386:is the
195:isospin
157:in the
83:scholar
2051:Chiral
1999:Type I
1814:Yukawa
1735:Models
1565:
1405:. See
240:flavor
139:mesons
125:, the
85:
78:
71:
64:
56:
2190:links
2163:links
2151:links
2071:NMSSM
2056:Fermi
1799:Soler
1769:Proca
1587:(PDF)
1403:pions
788:With
153:from
145:with
90:JSTOR
76:books
2061:MSSM
1958:ABJM
1865:Toda
1614:and
1563:ISBN
1378:U(1)
205:and
197:and
137:and
62:news
2014:11D
1531:doi
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1490:doi
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246:is
161:of
121:In
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