Axial anomaly and magnetism of nuclear and quark matter

By D. Son, M. Stephanov. 2007

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We consider the response of the QCD ground state at finite baryon density to a strong magnetic field B. We point out the dominant role played by the coupling of neutral Goldstone bosons, such as {pi}{sup 0}, to the magnetic field via the axial triangle anomaly. We show that, in vacuum, above a value of B{approx}m{sub {pi}}{sup 2}/e, a metastable object appears - the {pi}{sup 0} domain wall. Because of the axial anomaly, the wall carries a baryon number surface density proportional to B. As a result, for B > or approx. 10{sup 19} G a stack of parallel {pi}{sup 0} domain walls is energetically more favorable than nuclear matter at the same density. Similarly, at higher densities, somewhat weaker magnetic fields of order B > or approx. 10{sup 17}-10{sup 18} G transform the color-superconducting ground state of QCD into new phases containing stacks of axial isoscalar ({eta} or {eta}{sup '}) domain walls. We also show that a quark-matter state known as ''Goldstone current state,'' in which a gradient of a Goldstone field is spontaneously generated, is ferromagnetic due to the axial anomaly. We estimate the size of the fields created by such a state in a typical neutron starmore » to be of order 10{sup 14}-10{sup 15} G.« less

Subfields: Astronomy and Astrophysics, Atomic and Molecular Physics, and Optics, Condensed Matter Physics

View Paper: https://www.semanticscholar.org/paper/f0c60b89d5570b90bc1170f51ce26e3a8a3bd777

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