Massless boson that must be present in a quantum system with spontaneously broken symmetry
"Goldstone theorem" redirects here. For the theorem on Feynman diagrams, see linked-cluster theorem.
In particle and condensed matter physics, Goldstone bosons or Nambu–Goldstone bosons (NGBs) are bosons that appear necessarily in models exhibiting spontaneous breakdown of continuous symmetries. They were discovered by Yoichiro Nambu in particle physics within the context of the BCS superconductivity mechanism,[1] and subsequently elucidated by Jeffrey Goldstone,[2] and systematically generalized in the context of quantum field theory.[3] In condensed matter physics such bosons are quasiparticles and are known as Anderson–Bogoliubov modes.[4][5][6]
These spinless bosons correspond to the spontaneously broken internal symmetry generators, and are characterized by the quantum numbers of these.
They transform nonlinearly (shift) under the action of these generators, and can thus be excited out of the asymmetric vacuum by these generators. Thus, they can be thought of as the excitations of the field in the broken symmetry directions in group space—and are massless if the spontaneously broken symmetry is not also broken explicitly.
If, instead, the symmetry is not exact, i.e. if it is explicitly broken as well as spontaneously broken, then the Nambu–Goldstone bosons are not massless, though they typically remain relatively light; they are then called pseudo-Goldstone bosons or pseudo–Nambu–Goldstone bosons (abbreviated PNGBs).
^Nambu, Y (1960). "Quasiparticles and Gauge Invariance in the Theory of Superconductivity". Physical Review. 117 (3): 648–663. Bibcode:1960PhRv..117..648N. doi:10.1103/PhysRev.117.648.
^Goldstone, J (1961). "Field Theories with Superconductor Solutions". Nuovo Cimento. 19 (1): 154–164. Bibcode:1961NCim...19..154G. doi:10.1007/BF02812722. S2CID 120409034.
^Anderson, P. W. (1958-05-15). "Coherent Excited States in the Theory of Superconductivity: Gauge Invariance and the Meissner Effect". Physical Review. 110 (4). American Physical Society (APS): 827–835. Bibcode:1958PhRv..110..827A. doi:10.1103/physrev.110.827. ISSN 0031-899X.
^Anderson, P. W. (1958-12-15). "Random-Phase Approximation in the Theory of Superconductivity". Physical Review. 112 (6). American Physical Society (APS): 1900–1916. Bibcode:1958PhRv..112.1900A. doi:10.1103/physrev.112.1900. ISSN 0031-899X.
^Bogoljubov, N. N.; Tolmachov, V. V.; Širkov, D. V. (1958). "A New Method in the Theory of Superconductivity". Fortschritte der Physik. 6 (11–12). Wiley: 605–682. Bibcode:1958ForPh...6..605B. doi:10.1002/prop.19580061102. ISSN 0015-8208.
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