-
1
-
-
0000273064
-
-
L.? I. Glazman and M.E. Raikh, JETP Lett.JTPLA2 47, 452 (1988);
-
(1988)
JETP Lett.
, vol.47
, pp. 452
-
-
-
2
-
-
33744553393
-
-
T.K. Ng and P.A. Lee, Phys. Rev. Lett. 61, 1768 (1988).10.1103/PhysRevLett.61.1768
-
(1988)
Phys. Rev. Lett.
, vol.61
, pp. 1768
-
-
-
4
-
-
0032563237
-
-
S.M. Cronenwett et al, Science 281, 540 (1998); 10.1126/science.281.5376.540
-
(1998)
Science
, vol.281
, pp. 540
-
-
Cronenwett, S.M.1
-
5
-
-
0032614514
-
-
F. Simmel et al, Phys. Rev. Lett. 83, 804 (1999); 10.1103/PhysRevLett.83.804
-
(1999)
Phys. Rev. Lett.
, vol.83
, pp. 804
-
-
Simmel, F.1
-
6
-
-
0033717586
-
-
J. Schmid et al, Phys. Rev. Lett. 84, 5824 (2000); 10.1103/PhysRevLett.84.5824
-
(2000)
Phys. Rev. Lett.
, vol.84
, pp. 5824
-
-
Schmid, J.1
-
7
-
-
0034703339
-
-
W.G. van der Wiel et al, Science 289, 2105 (2000).10.1126/science.289.5487.2105
-
(2000)
Science
, vol.289
, pp. 2105
-
-
-
8
-
-
0034676421
-
-
J. Nygård et al, Nature (London) 408, 342 (2000).10.1038/35042545
-
(2000)
Nature (London)
, vol.408
, pp. 342
-
-
Nygård, J.1
-
9
-
-
0037091281
-
-
M.R. Buitelaar et al, Phys. Rev. Lett. 88, 156801 (2002).10.1103/PhysRevLett.88.156801
-
(2002)
Phys. Rev. Lett.
, vol.88
, pp. 156801
-
-
Buitelaar, M.R.1
-
10
-
-
0037071635
-
-
J. Park et al, Nature (London) 417, 722 (2002); 10.1038/nature00791
-
(2002)
Nature (London)
, vol.417
, pp. 722
-
-
Park, J.1
-
11
-
-
0037071820
-
-
W. Liang et al, Nature (London) 417, 725 (2002).10.1038/nature00790
-
(2002)
Nature (London)
, vol.417
, pp. 725
-
-
Liang, W.1
-
12
-
-
0037122295
-
-
M.R. Buitelaar et al, Phys. Rev. Lett. 89, 256801 (2002).10.1103/PhysRevLett.89.256801
-
(2002)
Phys. Rev. Lett.
, vol.89
, pp. 256801
-
-
Buitelaar, M.R.1
-
13
-
-
0037091649
-
-
N. Sergueev et al, Phys. Rev. B 65, 165303 (2002).10.1103/PhysRevB.65.165303
-
(2002)
Phys. Rev. B
, vol.65
, pp. 165303
-
-
Sergueev, N.1
-
14
-
-
0037207350
-
-
P. Zhang et al, Phys. Rev. Lett. 89, 286803 (2002).10.1103/PhysRevLett.89.286803
-
(2002)
Phys. Rev. Lett.
, vol.89
, pp. 286803
-
-
Zhang, P.1
-
15
-
-
4243380809
-
-
B.R. Bułka et al, Phys. Rev. B 67, 024404 (2003).10.1103/PhysRevB.67.024404
-
(2003)
Phys. Rev. B
, vol.67
, pp. 24404
-
-
-
16
-
-
0037625899
-
-
R. Lopez et al, Phys. Rev. Lett. 90, 116602 (2003).10.1103/PhysRevLett.90.116602
-
(2003)
Phys. Rev. Lett.
, vol.90
, pp. 116602
-
-
Lopez, R.1
-
17
-
-
0142157607
-
-
J. Martinek et al, Phys. Rev. Lett. 91, 127203 (2003).10.1103/PhysRevLett.91.127203
-
(2003)
Phys. Rev. Lett.
, vol.91
, pp. 127203
-
-
Martinek, J.1
-
22
-
-
0034251301
-
-
T.A. Costi, Phys. Rev. Lett. 85, 1504 (2000); 10.1103/PhysRevLett.85.1504
-
(2000)
Phys. Rev. Lett.
, vol.85
, pp. 1504
-
-
Costi, T.A.1
-
23
-
-
0035894356
-
-
T.A. CostiPhys. Rev. B 64, 241310 (2001).10.1103/PhysRevB.64.241310
-
(2001)
Phys. Rev. B
, vol.64
, pp. 241310
-
-
Costi, T.A.1
-
24
-
-
85038266706
-
-
The remarkable full recovery of the Kondo effect should be contrasted to the competition between Kondo physics and magnetic RKKY interactions in heavy-fermion systems
-
The remarkable full recovery of the Kondo effect should be contrasted to the competition between Kondo physics and magnetic RKKY interactions in heavy-fermion systems
-
-
-
-
25
-
-
0034450719
-
-
A.H. Castro Neto and B.A. Jones, Phys. Rev. B 62, 14?975 (2000), and references therein.10.1103/PhysRevB.62.14975
-
(2000)
Phys. Rev. B
, vol.62
, pp. 14-975
-
-
-
26
-
-
36049055020
-
-
D.C. Langreth, Phys. Rev. 150, 516 (1966).10.1103/PhysRev.150.516
-
(1966)
Phys. Rev.
, vol.150
, pp. 516
-
-
Langreth, D.C.1
-
28
-
-
0141883429
-
-
E.?Yu. Tsymbal and D.G. Pettifor, J. Phys. Condens. Matter 9, L411 (1997).10.1088/0953-8984/9/30/002
-
(1997)
J. Phys. Condens. Matter
, vol.9
-
-
-
29
-
-
85038340332
-
-
We expect that a finite (Formula presented)-electron interaction, (Formula presented), will lead only to a slight renormalization of (Formula presented). Recently, an Anderson impurity embedded in a correlated host (without magnetic order) was studied
-
We expect that a finite (Formula presented)-electron interaction, (Formula presented), will lead only to a slight renormalization of (Formula presented). Recently, an Anderson impurity embedded in a correlated host (without magnetic order) was studied
-
-
-
-
33
-
-
85038347039
-
-
A lowest-order perturbation calculation shows that for (Formula presented) the spin splitting of the bottom of the band (Formula presented) (for (Formula presented) bands we consider no spin splitting for the band top) generates an effective local magnetic field (Formula presented). To account for this in our model of Eq.� 2, one could renormalize (Formula presented) (or else use a shifted compensation field (Formula presented) below)
-
A lowest-order perturbation calculation shows that for (Formula presented) the spin splitting of the bottom of the band (Formula presented) (for (Formula presented) bands we consider no spin splitting for the band top) generates an effective local magnetic field (Formula presented). To account for this in our model of Eq.� 2, one could renormalize (Formula presented) (or else use a shifted compensation field (Formula presented) below).
-
-
-
-
35
-
-
85038324298
-
-
A poor man’s scaling analysis
-
A poor man’s scaling analysis
-
-
-
-
36
-
-
0035883562
-
-
A similar splitting was predicted [D. Boese, et al, Phys. Rev. B 64, 125309 (2001); 10.1103/PhysRevB.64.125309
-
(2001)
Phys. Rev. B
, vol.64
, pp. 125309
-
-
Boese, D.1
-
37
-
-
85038337695
-
-
cond-mat/0104297
-
W. Hofstetter, cond-mat/0104297] for a two-level QD system which, in a special situation, can be mapped on our model.
-
-
-
Hofstetter, W.1
-
38
-
-
85038327772
-
-
Our NRG confirms Eq.� 4 for arbitrary (Formula presented) and (Formula presented)
-
Our NRG confirms Eq.� 4 for arbitrary (Formula presented) and (Formula presented).
-
-
-
-
39
-
-
85038321990
-
-
cond-mat/0305107
-
M.S. Choi et al, cond-mat/0305107.
-
-
-
Choi, M.S.1
|