Chiral symmetry breaking

In particle physics, chiral symmetry breaking is the spontaneous symmetry breaking of a chiral symmetry – usually by a gauge theory such as quantum chromodynamics, the quantum field theory of the strong interaction. Yoichiro Nambu was awarded the 2008 Nobel prize in physics for describing this phenomenon ("for the discovery of the mechanism of spontaneous broken symmetry in subatomic physics").

Overview

Quantum chromodynamics

Experimentally, it is observed that the masses of the octet of pseudoscalar mesons (such as the pion) are much lighter than the next heavier states such as the octet of vector mesons, such as rho meson.

This is a consequence of spontaneous symmetry breaking of chiral symmetry in a fermion sector of QCD with 3 flavors of light quarks, u, d and s. Such a theory, for idealized massless quarks, has global $SU (3) \times SU (3)$ chiral flavor symmetry. Under SSB, this is spontaneously broken to the diagonal flavor SU(3) subgroup, generating eight Nambu–Goldstone bosons, which are the pseudoscalar mesons transforming as an octet representation of this flavor SU(3).

Beyond this idealization of massless quarks, the actual small quark masses also break the chiral symmetry explicitly as well (providing non-vanishing pieces to the divergence of chiral currents). The masses of the pseudoscalar meson octet are specified by an expansion in the quark masses which goes by the name of chiral perturbation theory. The internal consistency of this argument is further checked by lattice QCD computations, which allow one to vary the quark mass and confirm that the variation of the pseudoscalar masses with the quark masses is as dictated by chiral perturbation theory, effectively as the square-root of the quark masses.

For the three heavy quarks: the charm quark, bottom quark, and top quark, their masses, and hence the explicit breaking these amount to, are much larger than the QCD spontaneous chiral symmetry breaking scale. Thus, they cannot be treated as a small perturbation around the explicit symmetry limit.

Mass generation

Chiral symmetry breaking is most apparent in the mass generation of nucleons from more elementary light quarks, accounting for approximately 99% of their combined mass as a baryon. It thus accounts for most of the mass of all visible matter.^[1] For example, in the proton, of mass m_p ≈ 938 MeV, the valence quarks, two up quarks with m_u ≈ 2.3 MeV and one down quark with m_d ≈ 4.8 MeV, only contribute about 9.4 MeV to the proton's mass. The source of the bulk of the proton's mass is quantum chromodynamics binding energy, which arises out of QCD chiral symmetry breaking.^[2]

Fermion condensate

The spontaneous symmetry breaking may be described in analogy to magnetization.

A vacuum condensate of bilinear expressions involving the quarks in the QCD vacuum is known as the fermion condensate.

It can be calculated as

\langle {\bar {q}}_{R}^{a}q_{L}^{b}\rangle =v\delta ^{{ab}}~,

formed through nonperturbative action of QCD gluons, with v ≈ −(250 MeV)³. This cannot be preserved under an isolated L or R rotation. The pion decay constant, $f π$ ≈ 93 MeV, may be viewed as a measure of the strength of the chiral symmetry breaking.^[3]

Two-quark model

For two light quarks, the up quark and the down quark, the QCD Lagrangian provides insight. The symmetry of the QCD Lagrangian, called chiral symmetry describes invariance with respect to a symmetry group $U(2)_{L}\times U(2)_{R}$ . This symmetry group amounts to

SU(2)_{L}\times SU(2)_{R}\times U(1)_{V}\times U(1)_{A}~.

The quark condensate induced by nonperturbative strong interactions spontaneously breaks the $SU(2)_{L}\times SU(2)_{R}$ down to the diagonal vector subgroup SU(2)_V, known as isospin. The resulting effective theory of baryon bound states of QCD (which describes protons and neutrons), then, has mass terms for these, disallowed by the original linear realization of the chiral symmetry, but allowed by the spontaneously broken nonlinear realization thus achieved as a result of the strong interactions.^[4]

The Nambu-Goldstone bosons corresponding to the three broken generators are the three pions, charged and neutral.

Pseudo-Goldstone bosons

Pseudo-Goldstone bosons arise in a quantum field theory with both spontaneous and explicit symmetry breaking. These two types of symmetry breaking typically occur separately, and at different energy scales, and are not thought to be predicated on each other.

In the absence of explicit breaking, spontaneous symmetry breaking would engender massless Nambu–Goldstone bosons for the exact spontaneously broken chiral symmetries. The chiral symmetries discussed, however, are only approximate symmetries, given their small explicit breaking.

The explicit symmetry breaking occurs at a smaller energy scale. The properties of these pseudo-Goldstone bosons can normally be calculated using chiral perturbation theory, expanding around the exactly symmetric theory in terms of the explicit symmetry-breaking parameters. In particular, the computed mass must be small,^[5] $m π \approx \sqrt vm q / f π$ .

Three-quark model

For three light quarks, the up quark, down quark, and strange quark, the flavor-chiral symmetries extending those discussed above also decompose, to Gell-Mann's^[6]

SU(3)_{L}\times SU(3)_{R}\times U(1)_{V}\times U(1)_{A}

.

The chiral symmetry generators spontaneously broken comprise the coset space $(SU(3)_{L}\times SU(3)_{R})/SU(3)_{V}$ . This space is not a group, and consists of the eight axial generators, corresponding to the eight light pseudoscalar mesons, the nondiagonal part of $SU(3)_{L}\times SU(3)_{R}$ .

The remaining eight unbroken vector subgroup generators constitute the manifest standard "Eightfold Way" flavor symmetries, SU(3)_V.

References

↑ Ta-Pei Cheng and Ling-Fong Li, Gauge Theory of Elementary Particle Physics, (Oxford 1984) ISBN 978-0198519614; Wilczek, F. (1999). "Mass Without Mass I: Most of Matter". Physics Today. 52 (11): 11–11. Bibcode:1999PhT....52k..11W. doi:10.1063/1.882879.
↑ The idealized chiral limit of the nucleon mass is about 880 MeV, cf. Procura, M.; Musch, B.; Wollenweber, T.; Hemmert, T.; Weise, W. (2006). "Nucleon mass: From lattice QCD to the chiral limit". Physical Review D. 73 (11). arXiv:hep-lat/0603001. Bibcode:2006PhRvD..73k4510P. doi:10.1103/PhysRevD.73.114510. .
↑ Peskin, Michael; Schroeder, Daniel (1995). An Introduction to Quantum Field Theory. Westview Press. p. 670. ISBN 0-201-50397-2.
↑ J Donoghue, E Golowich and B Holstein, Dynamics of the Standard Model, (Cambridge University Press, 1994) ISBN 9780521476522.
↑ Gell-Mann, M.; Oakes, R.; Renner, B. (1968). "Behavior of Current Divergences under SU_{3}×SU_{3}". Physical Review. 175 (5): 2195. Bibcode:1968PhRv..175.2195G. doi:10.1103/PhysRev.175.2195. . The generic formula for the mass of pseudogoldstone bosons in the presence of an explicit breaking perturbation is often called Dashen's formula, here $m_{\pi }^{2}f_{\pi }^{2}=-\langle 0|[Q_{5},[Q_{5},H]]|0\rangle$ .
↑ See Current algebra.

Gell-Mann, M.; Lévy, M. (1960), "The axial vector current in beta decay", Il Nuovo Cimento, 16: 705–726, Bibcode:1960NCim...16..705G, doi:10.1007/BF02859738 online copy

This article is issued from Wikipedia. The text is licensed under Creative Commons - Attribution - Sharealike. Additional terms may apply for the media files.

[1] Ta-Pei Cheng and Ling-Fong Li, Gauge Theory of Elementary Particle Physics, (Oxford 1984) ISBN 978-0198519614; Wilczek, F. (1999). "Mass Without Mass I: Most of Matter". Physics Today. 52 (11): 11–11. Bibcode:1999PhT....52k..11W. doi:10.1063/1.882879.

[2] The idealized chiral limit of the nucleon mass is about 880 MeV, cf. Procura, M.; Musch, B.; Wollenweber, T.; Hemmert, T.; Weise, W. (2006). "Nucleon mass: From lattice QCD to the chiral limit". Physical Review D. 73 (11). arXiv:hep-lat/0603001. Bibcode:2006PhRvD..73k4510P. doi:10.1103/PhysRevD.73.114510. .

[3] Peskin, Michael; Schroeder, Daniel (1995). An Introduction to Quantum Field Theory. Westview Press. p. 670. ISBN 0-201-50397-2.

[4] J Donoghue, E Golowich and B Holstein, Dynamics of the Standard Model, (Cambridge University Press, 1994) ISBN 9780521476522.

[5] Gell-Mann, M.; Oakes, R.; Renner, B. (1968). "Behavior of Current Divergences under SU_{3}×SU_{3}". Physical Review. 175 (5): 2195. Bibcode:1968PhRv..175.2195G. doi:10.1103/PhysRev.175.2195. . The generic formula for the mass of pseudogoldstone bosons in the presence of an explicit breaking perturbation is often called Dashen's formula, here $m_{\pi }^{2}f_{\pi }^{2}=-\langle 0|[Q_{5},[Q_{5},H]]|0\rangle$ .

[6] See Current algebra.