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| 001 | 48851 | ||
| 005 | 20200423204254.0 | ||
| 017 | _ | _ | |a This version is available at the following Publisher URL: http://prl.aps.org |
| 024 | 7 | _ | |a 10.1103/PhysRevLett.95.116402 |2 DOI |
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| 024 | 7 | _ | |a 2128/1423 |2 Handle |
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| 041 | _ | _ | |a eng |
| 082 | _ | _ | |a 550 |
| 084 | _ | _ | |2 WoS |a Physics, Multidisciplinary |
| 100 | 1 | _ | |a Liebsch, A. |b 0 |u FZJ |0 P:(DE-Juel1)VDB941 |
| 245 | _ | _ | |a Novel Mott transitions in a nonisotropic two-band Hubbard model |
| 260 | _ | _ | |a College Park, Md. |b APS |c 2005 |
| 300 | _ | _ | |a 116402 |
| 336 | 7 | _ | |a Journal Article |0 PUB:(DE-HGF)16 |2 PUB:(DE-HGF) |
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| 440 | _ | 0 | |a Physical Review Letters |x 0031-9007 |0 4925 |v 95 |
| 500 | _ | _ | |a Record converted from VDB: 12.11.2012 |
| 520 | _ | _ | |a The Mott transition in a two-band Hubbard model involving subbands of different widths is studied as a function of temperature using dynamical mean field theory combined with exact diagonalization. The phase diagram is shown to exhibit two successive first-order transitions if the full Hund's rule coupling is included. In the absence of spin-flip and pair-exchange terms the lower transition remains first-order while the upper becomes continuous. |
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| 773 | _ | _ | |a 10.1103/PhysRevLett.95.116402 |g Vol. 95, p. 116402 |p 116402 |q 95<116402 |0 PERI:(DE-600)1472655-5 |t Physical review letters |v 95 |y 2005 |x 0031-9007 |
| 856 | 7 | _ | |u http://dx.doi.org/10.1103/PhysRevLett.95.116402 |u http://hdl.handle.net/2128/1423 |
| 856 | 4 | _ | |u https://juser.fz-juelich.de/record/48851/files/76684.pdf |y OpenAccess |
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| 915 | _ | _ | |0 StatID:(DE-HGF)0010 |a JCR/ISI refereed |
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| 920 | 1 | _ | |k IFF-TH-I |l Theorie I |d 31.12.2006 |g IFF |0 I:(DE-Juel1)VDB30 |x 0 |
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