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N. F. Mott, Rev. Mod. Phys. 40, 677 (1968); Metal-Insulator Transitions (Taylor & Francis, London, 1990); F. Gebhard, The Mott Metal-Insulator Transition (Springer, Berlin, 1997).
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Mott, N.F.1
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Springer, Berlin
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N. F. Mott, Rev. Mod. Phys. 40, 677 (1968); Metal-Insulator Transitions (Taylor & Francis, London, 1990); F. Gebhard, The Mott Metal-Insulator Transition (Springer, Berlin, 1997).
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The Mott Metal-insulator Transition
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Gebhard, F.1
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3
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0035878361
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See, e.g., R. Bulla, T. A. Costi, and D. Vollhardt, Phys. Rev. B 64, 045103 (2001); J. Schlipf et al., Phys. Rev. Lett. 82, 4890 (1999).
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Phys. Rev. B
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Bulla, R.1
Costi, T.A.2
Vollhardt, D.3
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4
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4243444335
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See, e.g., R. Bulla, T. A. Costi, and D. Vollhardt, Phys. Rev. B 64, 045103 (2001); J. Schlipf et al., Phys. Rev. Lett. 82, 4890 (1999).
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Phys. Rev. Lett.
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Schlipf, J.1
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35949011563
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W. Metzner and D. Vollhardt, Phys. Rev. Lett. 62, 324 (1989); A. Georges and G. Kotliar, Phys. Rev. B 45, 6479 (1992); M. Jarrell, Phys. Rev. Lett. 69, 168 (1992).
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Metzner, W.1
Vollhardt, D.2
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Phys. Rev. B
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Georges, A.1
Kotliar, G.2
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7
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4043083512
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W. Metzner and D. Vollhardt, Phys. Rev. Lett. 62, 324 (1989); A. Georges and G. Kotliar, Phys. Rev. B 45, 6479 (1992); M. Jarrell, Phys. Rev. Lett. 69, 168 (1992).
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Jarrell, M.1
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K. Held et al., Phys. Rev. Lett. 86, 5345 (2001); G. Keller et al., cond-mat/0402133.
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11
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4644277288
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note
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T = 0.6/1000 K. The boundary of the crossover regime is not sharply defined. For the line shown in Fig. 1, we used the criterion that dη/dx is becoming small, i.e., 25% of its maximal value at the same T.
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13
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4243643061
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0, which includes lattice contributions via a normal compressibility K, has a negative curvature with respect to volume V above the DMFT critical point [P. Majumdar and H. R. Krishnamurthy, Phys. Rev. Lett. 73, 1525 (1994)]. This gives rise to a thermodynamic instability as in the liquid gas transition or the Kondo volume collapse scenario for Ce [ J. W. Allen and R. M. Martin, Phys. Rev. Lett. 49, 1106 (1982)].
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(1994)
Phys. Rev. Lett.
, vol.73
, pp. 1525
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Majumdar, P.1
Krishnamurthy, H.R.2
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14
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3342917360
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0, which includes lattice contributions via a normal compressibility K, has a negative curvature with respect to volume V above the DMFT critical point [P. Majumdar and H. R. Krishnamurthy, Phys. Rev. Lett. 73, 1525 (1994)]. This gives rise to a thermodynamic instability as in the liquid gas transition or the Kondo volume collapse scenario for Ce [ J. W. Allen and R. M. Martin, Phys. Rev. Lett. 49, 1106 (1982)].
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(1982)
Phys. Rev. Lett.
, vol.49
, pp. 1106
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Allen, J.W.1
Martin, R.M.2
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16
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0141531069
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The critical resistivity behavior around the critical point has been determined recently by P. Limelette et al., Science 302, 89 (2003).
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(2003)
Science
, vol.302
, pp. 89
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Limelette, P.1
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4644361973
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note
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A small contribution to the 500 eV spectrum from Cr 3d emission has been removed by using information obtained from resonant photoemission spectra at the V 2p edge, for which the Cr emission is entirely suppressed, and from PI phase spectra for a much smaller value of x.
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22
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4644346781
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note
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A temperature cycle sometimes produces a small (≈0.1 eV) shift of the chemical potential, indicating some change of the surface states.
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