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Phys. Rev. B 75, 115103 (2007) [25 pages]

Fermi liquid instabilities in the spin channel

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Congjun Wu1, Kai Sun2, Eduardo Fradkin2, and Shou-Cheng Zhang3
1Kavli Institute for Theoretical Physics, University of California, Santa Barbara, California 93106-4030, USA
2Department of Physics, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801-3080, USA
3Department of Physics, McCullough Building, Stanford University, Stanford, California 94305-4045, USA

Received 12 October 2006; published 5 March 2007

We study the Fermi-surface instabilities of the Pomeranchuk type Sov. Phys. JETP 8 361 (1959) in the spin-triplet channel with high orbital partial waves [Fla(l>0)]. The ordered phases are classified into two classes, dubbed the α and β phases by analogy to the superfluid 3He A and B phases. The Fermi surfaces in the α phases exhibit spontaneous anisotropic distortions, while those in the β phases remain circular or spherical with topologically nontrivial spin configurations in momentum space. In the α phase, the Goldstone modes in the density channel exhibit anisotropic overdamping. The Goldstone modes in the spin channel have a nearly isotropic underdamped dispersion relation at small propagating wave vectors. Due to the coupling to the Goldstone modes, the spin-wave spectrum develops resonance peaks in both the α and β phases, which can be detected in inelastic neutron-scattering experiments. In the p-wave channel β phase, a chiral ground-state inhomogeneity is spontaneously generated due to a Lifshitz-like instability in the originally nonchiral systems. Possible experiments to detect these phases are discussed.

© 2007 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.75.115103
DOI:
10.1103/PhysRevB.75.115103
PACS:
71.10.Ay, 71.10.Ca, 05.30.Fk