-
4
-
-
0000910817
-
-
S. Taniguchi, T. Nishikawa, Y. Yasui, Y. Kobayashi, M. Sato, T. Nishioka, M. Kontani, and K. Sano: J. Phys. Soc. Jpn. 64 (1995) 2758.
-
(1995)
J. Phys. Soc. Jpn
, vol.64
, pp. 2758
-
-
Taniguchi, S.1
Nishikawa, T.2
Yasui, Y.3
Kobayashi, Y.4
Sato, M.5
Nishioka, T.6
Kontani, M.7
Sano, K.8
-
5
-
-
4243717268
-
-
H. Kageyama, K. Yoshimura, R. Stern, N. V. Mushnikov, K. Onizuka, M. Kato, K. Kosuge, C. P. Slichter, T. Goto, and Y. Ueda: Phys. Rev. Lett. 82 (1999) 3168.
-
(1999)
Phys. Rev. Lett
, vol.82
, pp. 3168
-
-
Kageyama, H.1
Yoshimura, K.2
Stern, R.3
Mushnikov, N.V.4
Onizuka, K.5
Kato, M.6
Kosuge, K.7
Slichter, C.P.8
Goto, T.9
Ueda, Y.10
-
7
-
-
27144482967
-
-
A. Läuchli, J. C. Domenge, C. Lhuillier, P. Sindzingre, and M. Troyer: Phys. Rev. Lett. 95 (2005) 137206.
-
(2005)
Phys. Rev. Lett
, vol.95
, pp. 137206
-
-
Läuchli, A.1
Domenge, J.C.2
Lhuillier, C.3
Sindzingre, P.4
Troyer, M.5
-
11
-
-
27144467475
-
-
R. G. Melko, A. Paramekanti, A. A. Burkov, A. Vishwanath, D. N. Sheng, and L. Balents: Phys. Rev. Lett. 95 (2005) 127207.
-
(2005)
Phys. Rev. Lett
, vol.95
, pp. 127207
-
-
Melko, R.G.1
Paramekanti, A.2
Burkov, A.A.3
Vishwanath, A.4
Sheng, D.N.5
Balents, L.6
-
15
-
-
27744452435
-
-
F. Sawano, I. Terasaki, H. Mori, T. Mori, M. Watanabe, N. Ikeda, Y. Nogami, and Y. Noda: Nature 437 (2005) 522.
-
(2005)
Nature
, vol.437
, pp. 522
-
-
Sawano, F.1
Terasaki, I.2
Mori, H.3
Mori, T.4
Watanabe, M.5
Ikeda, N.6
Nogami, Y.7
Noda, Y.8
-
17
-
-
33947259995
-
-
Y. Takahide, T. Konoike, K. Enomoto, M. Nishimura, T. Terashima, S. Uji, and H. M. Yamamoto: Phys. Rev. Lett. 98 (2007) 116602.
-
(2007)
Phys. Rev. Lett
, vol.98
, pp. 116602
-
-
Takahide, Y.1
Konoike, T.2
Enomoto, K.3
Nishimura, M.4
Terashima, T.5
Uji, S.6
Yamamoto, H.M.7
-
18
-
-
10344242414
-
-
For a review, see
-
For a review, see, H. Seo, C. Hotta, and H. Fukuyama: Chem. Rev. 104 (2004) 5005.
-
(2004)
Chem. Rev
, vol.104
, pp. 5005
-
-
Seo, H.1
Hotta, C.2
Fukuyama, H.3
-
26
-
-
84868881573
-
-
c = 12-13. The large error bar is due to the fitting errors originating from the several choices of functional form we adopted.
-
c = 12-13. The large error bar is due to the fitting errors originating from the several choices of functional form we adopted.
-
-
-
-
28
-
-
84868885209
-
-
CDW ∼ 3 and 2 for the projected and purely mean-field wave functions, respectively, reflecting the degree of correlation included. Therefore, we shall again stress that the CDW phase is artifactual and here we discuss it just for references.
-
CDW ∼ 3 and 2 for the projected and purely mean-field wave functions, respectively, reflecting the degree of correlation included. Therefore, we shall again stress that the CDW phase is artifactual and here we discuss it just for references.
-
-
-
-
30
-
-
35348829741
-
-
E. Wawrzyńska, R. Coldea, E. M. Wheeler, I. I. Mazin, M. D. Johannes, T. Sörgel, M. Jansen, R. M. Ibberson, and P. G. Radaelli: Phys. Rev. Lett. 99 (2007) 157204;
-
(2007)
Phys. Rev. Lett
, vol.99
, pp. 157204
-
-
Wawrzyńska, E.1
Coldea, R.2
Wheeler, E.M.3
Mazin, I.I.4
Johannes, M.D.5
Sörgel, T.6
Jansen, M.7
Ibberson, R.M.8
Radaelli, P.G.9
-
31
-
-
41549097344
-
-
E. Wawrzyńska, R. Coldea, E. M. Wheeler, T. Sörgel, M. Jansen, R. M. Ibberson, P. G. Radaelli, and M. M. Koza: Phys. Rev. B 77 (2008) 094439.
-
(2008)
Phys. Rev. B
, vol.77
, pp. 094439
-
-
Wawrzyńska, E.1
Coldea, R.2
Wheeler, E.M.3
Sörgel, T.4
Jansen, M.5
Ibberson, R.M.6
Radaelli, P.G.7
Koza, M.M.8
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