期刊
PHYSICAL REVIEW B
卷 80, 期 2, 页码 -出版社
AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.80.024512
关键词
band model of magnetism; charge density waves; doping; electrical conductivity; Fermi surface; fluctuations in superconductors; ground states; high-temperature superconductors; Hubbard model; iron compounds; Zeeman effect
资金
- NSF [DMR-0531159]
- U. S. Department of Energy, Office of Science [DE-FG0208ER46544]
The key feature of the Fe-based superconductors is their quasi-two-dimensional multiband Fermi surface. By relating the problem to a negative U Hubbard model and its superconducting ground state, we show that the defining instability of such a Fermi surface is the valley density-wave (VDW), a combined spin/charge density-wave at the wave vector connecting the electron and hole valleys. As the valley parameters change by doping or pressure, the fictitious superconductor experiences Zeeman splitting, eventually going into a nonuniform Fulde-Ferrell-Larkin-Ovchinikov (FFLO) state, an itinerant and often incommensurate VDW of the real world, characterized by the metallic conductivity from the ungapped remnants of the Fermi surface. When Zeeman splitting exceeds the Chandrasekhar-Clogston limit, the FFLO state disappears and the VDW is destabilized. Near this point, the VDW fluctuations and interband pair repulsion are essential ingredients of high-T-c superconductivity in Fe pnictides.
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