Fluctuating spin density waves in metals
Abstract
Recent work has used a U(1) gauge theory to describe the physics of Fermi pockets in the presence of fluctuating spin density wave order. We generalize this theory to an arbitrary band structure and ordering wave vector. The transition to the large Fermi-surface state, without pockets induced by local spin density wave order, is described by embedding the U(1) gauge theory in a SU(2) gauge theory. The phase diagram of the SU(2) gauge theory shows that the onset of spin density wave order in the Fermi liquid occurs either directly, in the framework discussed by Hertz, or via intermediate non-Fermi-liquid phases with Fermi surfaces of fractionalized excitations. We discuss application of our results to the phase diagram of the cuprates.
- Publication:
-
Physical Review B
- Pub Date:
- October 2009
- DOI:
- 10.1103/PhysRevB.80.155129
- arXiv:
- arXiv:0907.3732
- Bibcode:
- 2009PhRvB..80o5129S
- Keywords:
-
- 71.10.Hf;
- 75.10.Jm;
- 74.25.Dw;
- Non-Fermi-liquid ground states electron phase diagrams and phase transitions in model systems;
- Quantized spin models;
- Superconductivity phase diagrams;
- Condensed Matter - Strongly Correlated Electrons;
- Condensed Matter - Superconductivity;
- High Energy Physics - Theory
- E-Print:
- 15 pages, 2 figures