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See for example, A. C. Hewson: The Kondo Problem to Heary Fermions (Cambridge University Press, Cambridge, 1993) and references cited therein.
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Hewson, A.C.1
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10
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A. Oguri: Phys. Rev. B 56 (1997) 13422: Phys. Rev. B 58 (1998) 1690 (errata).
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Phys. Rev. B
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Oguri, A.1
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15
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33744559866
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errata
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A. Oguri: Phys. Rev. B 56 (1997) 13422: Phys. Rev. B 58 (1998) 1690 (errata).
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Phys. Rev. B
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17
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0038544380
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ed. H. Takayama, M. Tsukada, H. Shiba, F. Yonezawa, M. Imada and Y. Okabe The Physical Society of Japan, Tokyo
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Y. Shimizu and O. Sakai: Computational Physics as a New Frontier in Condensed Matter Research, ed. H. Takayama, M. Tsukada, H. Shiba, F. Yonezawa, M. Imada and Y. Okabe (The Physical Society of Japan, Tokyo, 1995) p. 42.
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D. Goldhaber-Gordon, H. Shtrikman, D. Mahalu, D. Abusch-Magder, U. Meirav and M. A. Kastner: Nature 391 (1998) 156.
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Shtrikman, H.2
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Abusch-Magder, D.4
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Kastner, M.A.6
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D. Goldhaber-Gordon, J. Göres, M. A. Kastner, H. Shtrikman, D. Mahalu and U. Meirav: Phys. Rev. Lett. 81 (1998) 5225.
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Göres, J.2
Kastner, M.A.3
Shtrikman, H.4
Mahalu, D.5
Meirav, U.6
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29
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85034151564
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note
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Non-ergodic phenomena was not observed in the present calculation.
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31
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0039252759
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Quantum phenomena in advanced materials at high magnetic fields
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March 9-12, National Research Institute for Metals, Tsukuba ed. G. Kido, Izumida, S. Suzuki and O. Sakai: in preparation
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O. Sakai, W. Izumida and S. Suzuki: Quantum Phenomena in Advanced Materials at High Magnetic Fields (Proceedings of the 4th International Symposium on Advanced Physical Fields, March 9-12, 1999, National Research Institute for Metals, Tsukuba) ed. G. Kido, p. 143: Izumida, S. Suzuki and O. Sakai: in preparation.
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(1999)
Proceedings of the 4th International Symposium on Advanced Physical Fields
, pp. 143
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Sakai, O.1
Izumida, W.2
Suzuki, S.3
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32
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85034127459
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note
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We used the expression (3.1) in the present NRG calculation. The expression (2.17) is reduced to eq. (3.1) in an obvious way in the NRG method. While it is not obvious in the course of the QMC calculation. But the final result should have equal magnitude with the value given by eq. (3.1).
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33
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85034126006
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note
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K0 decreases rapidly, but the temperature dependence of the Coulomb peak is governed mainly by Δμ.
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34
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85034149550
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note
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K = 0.04. For the relation of this definition to the usual one, see the ref. 25.
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