-
1
-
-
0032474839
-
-
N. D. Mathur, F. M. Grosche, S. R. Julian, I. R. Walker, D. M. Freye, R. K. W. Haselwimmer, and G. G. Lonzarich: Nature 394 (1998) 39.
-
(1998)
Nature
, vol.394
, pp. 39
-
-
Mathur, N.D.1
Grosche, F.M.2
Julian, S.R.3
Walker, I.R.4
Freye, D.M.5
Haselwimmer, R.K.W.6
Lonzarich, G.G.7
-
4
-
-
0345802609
-
-
H. Q. Yuan, F. M. Grosche, M. Deppe, C. Geibel, G. Sparn, and F. Steglich: Science 302 (2003) 2104.
-
(2003)
Science
, vol.302
, pp. 2104
-
-
Yuan, H.Q.1
Grosche, F.M.2
Deppe, M.3
Geibel, C.4
Sparn, G.5
Steglich, F.6
-
5
-
-
33244464968
-
-
H. Q. Yuan, F. M. Grosche, M. Deppe, G. Sparn, C. Geibel, and F. Steglich: Phys. Rev. Lett. 96 (2006) 047008.
-
(2006)
Phys. Rev. Lett
, vol.96
, pp. 047008
-
-
Yuan, H.Q.1
Grosche, F.M.2
Deppe, M.3
Sparn, G.4
Geibel, C.5
Steglich, F.6
-
6
-
-
42749098893
-
-
G.-q. Zheng, N. Yamaguchi, H. Kan, Y. Kitaoka, J. L. Sarrao, P. G. Pagliuso, N. O. Moreno, and J. D. Thompson: Phys. Rev. B 70 (2004) 014511.
-
(2004)
Phys. Rev. B
, vol.70
, pp. 014511
-
-
Zheng, G.-Q.1
Yamaguchi, N.2
Kan, H.3
Kitaoka, Y.4
Sarrao, J.L.5
Pagliuso, P.G.6
Moreno, N.O.7
Thompson, J.D.8
-
7
-
-
33645802407
-
-
S. Kawasaki, M. Yashima, Y. Mugino, H. Mukuda, Y. Kitaoka, H. Shishido, and Y. Ōnuki: Phys. Rev. Lett. 96 (2006) 147001.
-
(2006)
Phys. Rev. Lett
, vol.96
, pp. 147001
-
-
Kawasaki, S.1
Yashima, M.2
Mugino, Y.3
Mukuda, H.4
Kitaoka, Y.5
Shishido, H.6
Ōnuki, Y.7
-
8
-
-
0038476582
-
-
T. Muramatsu, T. C. Kobayashi, K. Shimizu, K. Amaya, D. Aoki, Y. Haga, and Y. Onuki: Physica C 388-389 (2003) 539.
-
(2003)
Physica C
, vol.388-389
, pp. 539
-
-
Muramatsu, T.1
Kobayashi, T.C.2
Shimizu, K.3
Amaya, K.4
Aoki, D.5
Haga, Y.6
Onuki, Y.7
-
9
-
-
18144422440
-
-
S. Kawasaki, G.-q. Zheng, H. Kan, Y. Kitaoka, H. Shishido, and Y. Ōnuki: Phys. Rev. Lett. 94 (2005) 037007.
-
(2005)
Phys. Rev. Lett
, vol.94
, pp. 037007
-
-
Kawasaki, S.1
Zheng, G.-Q.2
Kan, H.3
Kitaoka, Y.4
Shishido, H.5
Ōnuki, Y.6
-
11
-
-
33845522473
-
-
H. Q. Yuan, M. Nicklas, Z. Hossain, C. Geibel, and F. Steglich: Phys. Rev. B 74 (2006) 212403.
-
(2006)
Phys. Rev. B
, vol.74
, pp. 212403
-
-
Yuan, H.Q.1
Nicklas, M.2
Hossain, Z.3
Geibel, C.4
Steglich, F.5
-
12
-
-
0003756811
-
-
For example, see, Cambridge University Press, Cambridge, U.K
-
For example, see A. C. Hewson: The Kondo Problem to Heavy Fermions (Cambridge University Press, Cambridge, U.K., 1993);
-
(1993)
The Kondo Problem to Heavy Fermions
-
-
Hewson, A.C.1
-
18
-
-
39749156985
-
-
T. Sugibayashi and D. S. Hirashima: Proc. 5th Int. Symp. ASR-WYP-2005: Advances in the Physics and Chemistry of Actinide Compounds. J. Phys. Soc. Jpn. 75 (2006) Suppl., p. 244.
-
T. Sugibayashi and D. S. Hirashima: Proc. 5th Int. Symp. ASR-WYP-2005: Advances in the Physics and Chemistry of Actinide Compounds. J. Phys. Soc. Jpn. 75 (2006) Suppl., p. 244.
-
-
-
-
23
-
-
0030528685
-
-
and references therein
-
A. Georges, G. Kotliar, W. Kreuth, and M. J. Rozenberg: Rev. Mod. Phys. 68 (1996) 13, and references therein.
-
(1996)
Rev. Mod. Phys
, vol.68
, pp. 13
-
-
Georges, A.1
Kotliar, G.2
Kreuth, W.3
Rozenberg, M.J.4
-
27
-
-
84868932290
-
-
lm(p)}) is the most difficult in the DMFT + Lanczos method (see Appendix B).
-
lm(p)}) is the most difficult in the DMFT + Lanczos method (see Appendix B).
-
-
-
-
29
-
-
65549125364
-
-
In the region where a converged solution could not be obtained, it is possible that the phase separation occurs where the condition n tot, 1.75 cannot be satisfied
-
tot = 1.75 cannot be satisfied.
-
-
-
-
32
-
-
46849087961
-
-
T. Sugibayashi, Y. Saiga, and D. S. Hirashima: Proc. Int. Conf. New Quantum Phenomena in Skutterudite and Related Systems (Skutterudite 2007), J. Phys. Soc. Jpn. 77 (2008) Suppl. A, p. 278.
-
T. Sugibayashi, Y. Saiga, and D. S. Hirashima: Proc. Int. Conf. New Quantum Phenomena in Skutterudite and Related Systems (Skutterudite 2007), J. Phys. Soc. Jpn. 77 (2008) Suppl. A, p. 278.
-
-
-
-
34
-
-
65549086973
-
-
This scaling comes from, the requirement that the kinetic energy and the interaction one remain in the same order of magnitude
-
This scaling comes from, the requirement that the kinetic energy and the interaction one remain in the same order of magnitude.
-
-
-
-
35
-
-
16344363992
-
-
For the Hamiltonian (1) with vk→v and εfk→0, the three quantities Gff(iω n, Gcf(iωn, and G fc(iωn) are related to G cc(iωn) as follows: G ff(iωn, 1/iωn+μ- ε(0)f-Σff(iωn, v, Σcf(iωn, v +Σcf(iω n), iωn+μ-ε(0) f-Σff(iωn)]2 G cc(iωn, Gcf(iω n)=v+Σcf(iω n)/iωn+μ-ε(0) f-Σff(iωn) Gcc
-
2]. See, for example, H. O. Jeschke and G. Kotliar: Phys. Rev. B 71 (2005) 085103.
-
-
-
-
36
-
-
0008543873
-
-
In the present study, we chose the two-channel single-impurity model given by eq, B·39, because the lattice action in the presence of the cavity (S(o, contains two kinds of electrons, c and f. However, for the Hamiltonian (1) with, vk → v and ε fk 0, which is considered in the main text, a drastic simplification occurs that the coupling between the central site and the rest of the system affects only cc-component of (g 0)-1 due to Bcf, Bfc, Bff, 0. It is then possible to take another type of single-impurity model where the bath, consists only of c electrons. See, for example, Q. Si and G. Kotliar: Phys. Rev. Lett. 70 (1993) 3143;
-
ff = 0. It is then possible to take another type of single-impurity model where the bath, consists only of c electrons. See, for example, Q. Si and G. Kotliar: Phys. Rev. Lett. 70 (1993) 3143;
-
-
-
-
37
-
-
0038429560
-
-
Q. Si and G. Kotliar: Phys. Rev. B 48 (1993) 13881. We have checked that the results in the present study are in good agreement with those with use of the single-impurity model where the bath consists only of c electrons
-
Q. Si and G. Kotliar: Phys. Rev. B 48 (1993) 13881. We have checked that the results in the present study are in good agreement with those with use of the single-impurity model where the bath consists only of c electrons.
-
-
-
|