Landau Theory of the Finite Temperature Mott Transition
In the context of the dynamical mean-field theory of the Hubbard model, we identify microscopically an order parameter for the finite temperature Mott end point. We derive a Landau functional of the order parameter. We then use the order parameter theory to elucidate the singular behavior of various...
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2000
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005 | 20230518203145.0 | ||
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024 | 7 | |2 scopus |a 2-s2.0-0000549473 | |
040 | |a Scopus |b spa |c AR-BaUEN |d AR-BaUEN | ||
030 | |a PRLTA | ||
100 | 1 | |a Kotliar, G. | |
245 | 1 | 0 | |a Landau Theory of the Finite Temperature Mott Transition |
260 | |c 2000 | ||
270 | 1 | 0 | |m Kotliar, G.; Serin Physics Laboratory, Rutgers University, 136 Frelinghuysen Road, Piscataway, NJ 08854, United States |
506 | |2 openaire |e Política editorial | ||
504 | |a Mott, N.F., (1974) Metal-Insulator Transitions, , Taylor & Francis, London | ||
504 | |a Imada, M., Fujimori, A., Tokura, Y., (1998) Rev. Mod. Phys., 70, p. 1039 | ||
504 | |a Georges, A., Kotliar, G., Krauth, W., Rozenberg, M.J., (1996) Rev. Mod. Phys., 68, p. 13 | ||
504 | |a Brinkman, W.F., Rice, T.M., (1970) Phys. Rev. B, 2, p. 4302 | ||
504 | |a Kotliar, G., Ruckenstein, A.E., (1986) Phys. Rev. Lett., 57, p. 1362 | ||
504 | |a Fresard, R., Wolfle, P., (1986) Int. J. Mod. Phys. B, 6, p. 685 | ||
504 | |a (1986) Int. J. Mod. Phys. B, 6, p. 3087 | ||
504 | |a Castellani, C., Di Castro, C., Feinberg, D., Ranninger, J., (1979) Phys. Rev. Lett., 43, p. 1957 | ||
504 | |a Schlipf, J., Jarrell, M., Van Dongen, P.G.J., Blümer, N., Kehrein, S., Pruschke, T., Vollhardt, D., (1999) Phys. Rev. Lett., 82, p. 4890 | ||
504 | |a Rozenberg, M.J., Chitra, R., Kotliar, G., (1999) Phys. Rev. Lett., 83, p. 3498 | ||
504 | |a Krauth, W., cond-mat/9908221; Kotliar, G., (1999) Eur. J. Phys. B, 11, pp. 27-39 | ||
504 | |a This is true only at finite temperatures, which ensures that the limit of integration β is finite. At zero temperature the spectrum of fluctuations is continuous and the transition at a point denoted Uc2 has a very different character and was described in Ref. [9]; To accurately locate the critical point with IPT, we found it best to solve the DMFT equations on the imaginary axis. We note that, closest to the (Uc, Tc) point, up to 10 000 iterations were required to find converged solutions; Matsuura, A.Y., (1996) Phys. Rev. B, 53, p. 7584 | ||
504 | |a Pruschke, T., Cox, D., Jarrell, M., (1993) Phys. Rev. B, 47, p. 3553 | ||
504 | |a Georges, A., Krauth, W., (1993) Phys. Rev. B, 48, p. 7167 | ||
504 | |a Rozenberg, M., (1995) Phys. Rev. Lett., 75, p. 105 | ||
504 | |a Miyasaka, S., Takagi, H., unpublished | ||
520 | 3 | |a In the context of the dynamical mean-field theory of the Hubbard model, we identify microscopically an order parameter for the finite temperature Mott end point. We derive a Landau functional of the order parameter. We then use the order parameter theory to elucidate the singular behavior of various physical quantities which are experimentally accessible. |l eng | |
593 | |a Serin Physics Laboratory, Rutgers University, 136 Frelinghuysen Road, Piscataway, NJ 08854, United States | ||
593 | |a Departamento de Física, FCEN, Universidad de Buenos Aires, (1428) Buenos Aires, Argentina | ||
700 | 1 | |a Lange, E. | |
700 | 1 | |a Rozenberg, M.J. | |
773 | 0 | |d 2000 |g v. 84 |h pp. 5180-5183 |k n. 22 |p Phys Rev Lett |x 00319007 |w (AR-BaUEN)CENRE-386 |t Physical Review Letters | |
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856 | 4 | 0 | |u https://hdl.handle.net/20.500.12110/paper_00319007_v84_n22_p5180_Kotliar |y Handle |
856 | 4 | 0 | |u https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_00319007_v84_n22_p5180_Kotliar |y Registro en la Biblioteca Digital |
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