Spin-Density-Wave Phase Transitions in Quasi-One-Dimensional Dimerized Quarter-Filled Organic Conductors
arXiv:cond-mat/9906383 · doi:10.1143/JPSJ.68.2790
Abstract
We have studied spin density wave (SDW) phase transitions in dimerized quarter-filled Hubbard chains weakly coupled via interchain one-particle hopping, . It is shown that there exists a critical value of , , between the incoherent metal regime () and the Fermi liquid regime () in the metallic phase above the SDW transition temperature. By using the 2-loop perturbative renormalization-group approach together with the random-phase-approximation, we propose a SDW phase diagram covering both of the regimes. The SDW phase transition from the incoherent metal phase for is caused by growth of the intrachain electron-electron umklapp scattering toward low temperatures, which is regarded as preformation of the Mott gap. We discuss relevance of the present result to the SDW phase transitions in the quasi-one-dimensional dimerized quarter-filled organic conductors, (TMTTF)X and (TMTSF)X.
19 pages, 13 eps figures, uses jpsj.sty, corrected typo in the text and figures, no changes to the paper, to appear in J. Phys. Soc. Jpn. 68, No.8 (1999)
References in corpus (4)
- Antiferromagnetic Phases of One-Dimensional Quarter-Filled Organic Conductors
- On-chain electrodynamics of metallic (TMTSF)_2 X salts: Observation of Tomonaga-Luttinger liquid response
- Confinement of Interchain Hopping by Umklapp Scattering in Two-Coupled Chains
- Effects of Spin Fluctuations in Quasi-One-Dimensional Organic Superconductors
Cited by in corpus (3)
- Charge Ordering in the One-Dimensional Extended Hubbard Model: Implication to the TMTTF Family of Organic Conductors
- Two-loop renormalization-group theory for the quasi-one-dimensional Hubbard model at half filling
- Quantum phase transitions and collapse of the Mott gap in the dimensional half-filled Hubbard model