-
3
-
-
0012234520
-
-
J. Smit: Physica 21 (1955) 877;
-
(1955)
Physica
, vol.21
, pp. 877
-
-
Smit, J.1
-
4
-
-
85039019022
-
-
J. Smit: Physica 21 (1958) 39.
-
(1958)
Physica
, vol.21
, pp. 39
-
-
Smit, J.1
-
7
-
-
0000833740
-
-
P. Matl, N. P. Ong, Y. F. Yan, Y. Q. Li, D. Studebaker T. Baum and G. Doubinina: Phys. Rev. B 57 (1998) 10248.
-
(1998)
Phys. Rev. B
, vol.57
, pp. 10248
-
-
Matl, P.1
Ong, N.P.2
Yan, Y.F.3
Li, Y.Q.4
Studebaker, D.5
Baum, T.6
Doubinina, G.7
-
8
-
-
0000809415
-
-
S. H. Chun, M. B. Salamon, Y. Lyanda-Geller, P. M. Goldbart and P. D. Han: Phys. Rev. Lett. 84 (2000) 757.
-
(2000)
Phys. Rev. Lett.
, vol.84
, pp. 757
-
-
Chun, S.H.1
Salamon, M.B.2
Lyanda-Geller, Y.3
Goldbart, P.M.4
Han, P.D.5
-
9
-
-
0001690247
-
-
J. Ye, Y. B. Kim, A. J. Millis, B. I. Shraiman, P. Majumdar and Z. Tešanović: Phys. Rev. Lett. 83 (1999) 3737.
-
(1999)
Phys. Rev. Lett.
, vol.83
, pp. 3737
-
-
Ye, J.1
Kim, Y.B.2
Millis, A.J.3
Shraiman, B.I.4
Majumdar, P.5
Teš anović, Z.6
-
11
-
-
0035970804
-
-
Y. Taguchi, Y. Oohara, H. Yoshizawa and N. Nagaosa, Y. Tokura: Science 291 (2001) 2573;
-
(2001)
Science
, vol.291
, pp. 2573
-
-
Taguchi, Y.1
Oohara, Y.2
Yoshizawa, H.3
Nagaosa, N.4
Tokura, Y.5
-
12
-
-
0043269832
-
-
Y. Taguchi, T. Sasaki, S. Awaji, Y. Iwasa, T. Tayama, T. Sakakibara, S. Iguchi, T. Ito and Y. Tokura: Phys. Rev. Lett. 90 (2003) 257202.
-
(2003)
Phys. Rev. Lett.
, vol.90
, pp. 257202
-
-
Taguchi, Y.1
Sasaki, T.2
Awaji, S.3
Iwasa, Y.4
Tayama, T.5
Sakakibara, T.6
Iguchi, S.7
Ito, T.8
Tokura, Y.9
-
13
-
-
0035617660
-
-
T. Kageyama, S. Iikubo, S. Yoshii, Y. Kondo, M. Sato and Y. Iye: J. Phys. Soc. Jpn. 70 (2001) 3006.
-
(2001)
J. Phys. Soc. Jpn.
, vol.70
, pp. 3006
-
-
Kageyama, T.1
Iikubo, S.2
Yoshii, S.3
Kondo, Y.4
Sato, M.5
Iye, Y.6
-
21
-
-
0042769320
-
-
T. Jungwirth, J. Sinova, K. Y. Wang, K. W. Edmonds, R. P. Campion, B. L. Gallagher, C. T. Foxon, Q. Niu and A. H. MacDonald: Appl. Phys. Lett. 83 (2003) 320.
-
(2003)
Appl. Phys. Lett.
, vol.83
, pp. 320
-
-
Jungwirth, T.1
Sinova, J.2
Wang, K.Y.3
Edmonds, K.W.4
Campion, R.P.5
Gallagher, B.L.6
Foxon, C.T.7
Niu, Q.8
MacDonald, A.H.9
-
23
-
-
0141865713
-
-
Z. Fang, N. Nagaosa, K. S. Takahashi, A. Asamitsu, R. Mathieu, T. Ogasawara, H. Yamada, M. Kawasaki and Y. Tokura: Science 302 (2003) 92.
-
(2003)
Science
, vol.302
, pp. 92
-
-
Fang, Z.1
Nagaosa, N.2
Takahashi, K.S.3
Asamitsu, A.4
Mathieu, R.5
Ogasawara, T.6
Yamada, H.7
Kawasaki, M.8
Tokura, Y.9
-
24
-
-
1442282238
-
-
Y. Yao, L. Kleinman, A. H. MacDonald, S. Sinova, D. Wang, E. Wang and Q. Niu: Phys. Rev. Lett. 92 (2004) 037204.
-
(2004)
Phys. Rev. Lett.
, vol.92
, pp. 037204
-
-
Yao, Y.1
Kleinman, L.2
MacDonald, A.H.3
Sinova, S.4
Wang, D.5
Wang, E.6
Niu, Q.7
-
29
-
-
0030230401
-
-
J. M. Shilton,V. I. Talyanskii, M. Pepper, D. A. Ritchie, J. E. F. Frost, C. J. B. Ford, C. G. Smith and G. A. C. Jones: J. Phys.: Condens. Matter 8 (1996) L531.
-
(1996)
J. Phys.: Condens. Matter
, vol.8
-
-
Shilton, J.M.1
Talyanskii, V.I.2
Pepper, M.3
Ritchie, D.A.4
Frost, J.E.F.5
Ford, C.J.B.6
Smith, C.G.7
Jones, G.A.C.8
-
30
-
-
0000117520
-
-
V. I. Talyanskii, J. M. Shilton, M. Pepper,C. G. Smith, C. J. B. Ford, E. H. Linfield, D. A. Ritchie and G. A. C. Jones: Phys. Rev. B 56 (1997) 15180.
-
(1997)
Phys. Rev. B
, vol.56
, pp. 15180
-
-
Talyanskii, V.I.1
Shilton, J.M.2
Pepper, M.3
Smith, C.G.4
Ford, C.J.B.5
Linfield, E.H.6
Ritchie, D.A.7
Jones, G.A.C.8
-
31
-
-
24644514738
-
-
note
-
a] becomes a non-generic matrix in general.
-
-
-
-
32
-
-
0001514970
-
-
D. C. Dender, P. R. Hammar, D. H. Reich, C. Broholm and G. Aeppli: Phys. Rev. Lett. 79 (1997) 1750.
-
(1997)
Phys. Rev. Lett.
, vol.79
, pp. 1750
-
-
Dender, D.C.1
Hammar, P.R.2
Reich, D.H.3
Broholm, C.4
Aeppli, G.5
-
34
-
-
4243468159
-
-
I. Affleck and M. Oshikawa: Phys. Rev. B 60 (1999) 1038. In these papers, not only the staggered component of g-tensor but also the alternating DM vector are found to be relevant to induce a finite spin gap.
-
(1999)
Phys. Rev. B
, vol.60
, pp. 1038
-
-
Affleck, I.1
Oshikawa, M.2
-
35
-
-
0033261765
-
-
M. Oshikawa, K. Ueda, H. Aoki, A. Ochiai and M. Kohgi: J. Phys. Soc. Jpn. 68 (1999) 3181.
-
(1999)
J. Phys. Soc. Jpn.
, vol.68
, pp. 3181
-
-
Oshikawa, M.1
Ueda, K.2
Aoki, H.3
Ochiai, A.4
Kohgi, M.5
-
36
-
-
24644467581
-
-
note
-
If the system is invariant under the π-rotational symmetry which exchanges the nearest neighboring bonds, the direction of E must be deviated from this π-rotational axis.
-
-
-
-
37
-
-
24644477981
-
-
note
-
Here we also rotate by π around the z-direction in the spin space on odd sites: (equation presented) We take this sign convention only in §2.
-
-
-
-
43
-
-
0000609380
-
-
For example, R. Shankar: Acta Phys. Pol. B 26 (1995) 1835. From this paper, we change its notations as follows; (equation presented)
-
(1995)
Acta Phys. Pol. B
, vol.26
, pp. 1835
-
-
Shankar, R.1
-
45
-
-
24644515733
-
-
note
-
z ≠ 0.
-
-
-
-
48
-
-
24644464965
-
-
note
-
2.
-
-
-
-
49
-
-
24644432348
-
-
note
-
Here the wavefunction does not have the projected weight on the third excited state with n = 3 [thin line in Fig. 5(a)] during the cycle.
-
-
-
-
50
-
-
24644446804
-
-
note
-
+ is quantized to be 1.
-
-
-
-
67
-
-
24644482540
-
-
note
-
In spin-gapped systems, the effects of the boundary range only within its magnetic correlation length from both ends.
-
-
-
-
68
-
-
24644523501
-
-
note
-
In the final line of eq. (A·7), we drop those terms which can be summarized into a form of the total derivative.
-
-
-
-
70
-
-
80052648759
-
-
+(0) denotes the phase operator at the midpoint of two contacts. This backscattering potential turns out to be relevant in the presence of repulsive electron-electron interactions and tunneling probability of spins between two contacts becomes vanishing. As a consequence of this vanishing tunneling probability of spins (TPS), number of spins transported between these two contacts is also quantized in their work. Even though our work treats a pumping in macro-scale systems and is different from their work which is about meso (nano)-scale systems, there is an interesting correspondence between these two works. Namely, in both stories, quantizations of spin transports result from the vanishing TPS between two "contacts". Two contacts in their configurations correspond to the two sample boundaries in this paper and TPS between these two "contacts", namely tunneling probability between the state of eq. (26) and that of eq. (27) decreases exponetially in thermodynamic limit, which is also a necessity of the quantized spin transfers in this paper (see §3).
-
(2003)
Phys. Rev. B
, vol.68
, pp. 035321
-
-
Sharma, P.1
Chamon, C.2
|