TY - JOUR
T1 - Color magnetism in non-Abelian vortex matter
AU - Kobayashi, Michikazu
AU - Nakano, Eiji
AU - Nitta, Muneto
PY - 2014/6/1
Y1 - 2014/6/1
N2 - We propose color magnetism as a generalization of the ordinary Heisenberg (anti-)ferro magnets on a triangular lattice. Vortex matter consisting of an Abrikosov lattice of non-Abelian vortices with color magnetic fluxes shows a color ferro or anti-ferro magnetism, depending on the interaction among the vortex sites. A prime example is a non-Abelian vortex lattice in rotating dense quark matter, showing a color ferromagnetism. We show that the low-energy effective theory for the vortex lattice system in the color ferromagnetic phase is described by a 3+1 dimensional CP N -1 nonlinear sigma model with spatially anisotropic couplings. We identify gapless excitations independent from Tkachenko modes as color magnons, that is, Nambu-Goldstone modes propagating in the vortex lattice with an anisotropic linear dispersion relation ωp 2 = cxy 2c(p x 2 + py 2) + cz 2 p z 2. We calculate the transition temperature between the ordered and disordered phases, and apply it to dense quark matter. We also identify the order parameter spaces for color anti-ferromagnets.
AB - We propose color magnetism as a generalization of the ordinary Heisenberg (anti-)ferro magnets on a triangular lattice. Vortex matter consisting of an Abrikosov lattice of non-Abelian vortices with color magnetic fluxes shows a color ferro or anti-ferro magnetism, depending on the interaction among the vortex sites. A prime example is a non-Abelian vortex lattice in rotating dense quark matter, showing a color ferromagnetism. We show that the low-energy effective theory for the vortex lattice system in the color ferromagnetic phase is described by a 3+1 dimensional CP N -1 nonlinear sigma model with spatially anisotropic couplings. We identify gapless excitations independent from Tkachenko modes as color magnons, that is, Nambu-Goldstone modes propagating in the vortex lattice with an anisotropic linear dispersion relation ωp 2 = cxy 2c(p x 2 + py 2) + cz 2 p z 2. We calculate the transition temperature between the ordered and disordered phases, and apply it to dense quark matter. We also identify the order parameter spaces for color anti-ferromagnets.
KW - Sigma Models
KW - Solitons Monopoles and Instantons
KW - Spontaneous Symmetry Breaking
KW - Topological States of Matter
UR - http://www.scopus.com/inward/record.url?scp=84904350465&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=84904350465&partnerID=8YFLogxK
U2 - 10.1007/JHEP06(2014)130
DO - 10.1007/JHEP06(2014)130
M3 - Article
AN - SCOPUS:84904350465
SN - 1126-6708
VL - 2014
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 6
M1 - 130
ER -