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3
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0027905399
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H. Amitsuka et al., Physica B 186-188 (1993) 337.
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(1993)
Physica B
, vol.186-188
, pp. 337
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Amitsuka, H.1
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7
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0027905068
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D.L. Cox, Physica B 186-188 (1993) 312.
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(1993)
Physica B
, vol.186-188
, pp. 312
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Cox, D.L.1
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8
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0001217626
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-
This suggestion has been disputed because of recent non-linear susceptibility results; see A.P. Ramirez et al., Phys. Rev. Lett. 73 (1994) 3018.
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(1994)
Phys. Rev. Lett.
, vol.73
, pp. 3018
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Ramirez, A.P.1
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9
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0029247458
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F. Aliev et al., Physica B 206&207 (1995) 454.
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(1995)
Physica B
, vol.206-207
, pp. 454
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Aliev, F.1
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14
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4243335232
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K. Ueda, H. Tsunetsugu and M. Sigrist, Phys. Rev. Lett. 68 (1992) 1030; C.C. Yu and S.R. White, Phys. Rev. Lett. 71 (1993) 3866.
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(1993)
Phys. Rev. Lett.
, vol.71
, pp. 3866
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Yu, C.C.1
White, S.R.2
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16
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4043133154
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communication private
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M. Jarrell, H. Akhlaghpour and Th. Pruschke, Phys. Rev. Lett. 70 (1993) 1670; M. Jarrell (1994) communication private.
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(1994)
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Jarrell, M.1
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17
-
-
30244478519
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private communications
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However, in infinite dimensions, metallic behavior is not obtained when the phase shift at the Fermi energy is maintained precisely at π/2, even if the conduction band is not at half filling (T. Pruschke and M. Jarrell (1994) private communications).
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(1994)
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Pruschke, T.1
Jarrell, M.2
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20
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11744358228
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A.W.W. Ludwig and I. Affleck, Phys. Rev. Lett. 57 (1991) 3160; Nucl. Phys. B 428 (1994) 545.
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(1994)
Nucl. Phys. B
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, pp. 545
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-
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24
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0003756811
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Eqs. (5.84) and (5.103), Cambridge University Press, Cambridge
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This is inferred from Eqs. (5.84) and (5.103) in: The Kondo Problem to Heavy Fermions, ed. A. Hewson (Cambridge University Press, Cambridge, 1993) p. 121.
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(1993)
The Kondo Problem to Heavy Fermions
, pp. 121
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Hewson, A.1
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26
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0004168227
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ed. V.J. Emery World Scientific, Singapore
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See, for example, D. Vollhardt, in: Correlated Electron Systems, ed. V.J. Emery (World Scientific, Singapore, 1993); Th. Pruschke et al., Adv. Phys. 42 (1995) 2; A. Georges et al., Rev. Mod. Phys. (Jan. 1996).
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(1993)
Correlated Electron Systems
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Vollhardt, D.1
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27
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30244450736
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See, for example, D. Vollhardt, in: Correlated Electron Systems, ed. V.J. Emery (World Scientific, Singapore, 1993); Th. Pruschke et al., Adv. Phys. 42 (1995) 2; A. Georges et al., Rev. Mod. Phys. (Jan. 1996).
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(1995)
Adv. Phys.
, vol.42
, pp. 2
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Pruschke, Th.1
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28
-
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84867034206
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Jan.
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See, for example, D. Vollhardt, in: Correlated Electron Systems, ed. V.J. Emery (World Scientific, Singapore, 1993); Th. Pruschke et al., Adv. Phys. 42 (1995) 2; A. Georges et al., Rev. Mod. Phys. (Jan. 1996).
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(1996)
Rev. Mod. Phys.
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Georges, A.1
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29
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0000318530
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(a) A. Georges, G. Kotliar and Q. Si, Int. J. Mod. Phys. B 6 (1992) 705 - this reference also gave a preliminary discussion of the infinite dimensional two-channel lattice;
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(1992)
Int. J. Mod. Phys. B
, vol.6
, pp. 705
-
-
Georges, A.1
Kotliar, G.2
Si, Q.3
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32
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0003964324
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Eq. (7.1.3), Plenum, New York
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See, for example, Eq. (7.1.3) in: Many Particle Physics, ed. G.D. Mahan (Plenum, New York, 1990) p. 604.
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(1990)
Many Particle Physics
, pp. 604
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Mahan, G.D.1
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36
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30244507621
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note
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unitarity. Since this significantly exceeds the unitarity limit and the renormalized density of states is zero at ω, T = 0, it is still reasonable to identify the one-channel model at half filling and zero potential scattering as a soft gap insulator.
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39
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30244464660
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to be published
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However, in 1D, numerical calculations suggest no metal-insulator transition in applied field due to nonlocal spin flip scattering excluded in infinite dimensions; see H.M. Carruzzo and C.C. Yu, to be published in Phys. Rev. B.
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Phys. Rev. B
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Carruzzo, H.M.1
Yu, C.C.2
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