Comment on arXiv:0811.1575 entitled "Quantum phase transitions in the Hubbard model on triangular lattice" by T. Yoshioka, A. Koga and N. Kawakami
| dc.creator | Watanabe, Shinji | |
| dc.creator | Mizusaki, Takahiro | |
| dc.creator | Imada, Masatoshi | |
| dc.date | 2008-11-22 | |
| dc.date.accessioned | 2026-07-07T10:20:32Z | |
| dc.date.available | 2026-07-07T10:20:32Z | |
| dc.description | We show that the phase boundary between the paramagnetic metal and the nonmagnetic Mott insulator for the Hubbard model on a triangular lattice obtained by Yoshioka et al. in arXiv:0811.1575 does not correctly represent that of the thermodynamic limit but is an artifact of the 6 by 6 lattice they rely on. After the system size extrapolation, the phase boundary is located at U/t=5.2 as proposed by Morita et al., J. Phys. Soc. Jpn. 71 (2008) 2109 and in contrast to Yoshioka et al. Here, U is the onsite Coulomb repulsion and t is the nearest-neighbor transfer. | |
| dc.description | 3 pages, 6 figures | |
| dc.identifier | https://arxiv.org/abs/0811.3718 | |
| dc.identifier | http://arxiv.org/abs/0811.3718 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/174880 | |
| dc.subject | Strongly Correlated Electrons | |
| dc.title | Comment on arXiv:0811.1575 entitled "Quantum phase transitions in the Hubbard model on triangular lattice" by T. Yoshioka, A. Koga and N. Kawakami | |
| dc.type | text |