-
1
-
-
10244244991
-
-
10.1021/cr040697x
-
P. Batail, Chem. Rev. 104, 4887 (2004). 10.1021/cr040697x
-
(2004)
Chem. Rev.
, vol.104
, pp. 4887
-
-
Batail, P.1
-
3
-
-
0035867123
-
-
10.1016/S0379-6779(00)00683-4
-
Y. Takano, K. Hiraki, H. M. Yamamoto, T. Nakamura, and T. Takahashi, Synth. Met. 120, 1081 (2001). 10.1016/S0379-6779(00)00683-4
-
(2001)
Synth. Met.
, vol.120
, pp. 1081
-
-
Takano, Y.1
Hiraki, K.2
Yamamoto, H.M.3
Nakamura, T.4
Takahashi, T.5
-
4
-
-
0036350853
-
-
10.1143/JPSJ.71.1832
-
N. Tajima, A. Ebina-Tajima, M. Tamura, Y. Nishio, and K. Kajita, J. Phys. Soc. Jpn. 71, 1832 (2002). 10.1143/JPSJ.71.1832
-
(2002)
J. Phys. Soc. Jpn.
, vol.71
, pp. 1832
-
-
Tajima, N.1
Ebina-Tajima, A.2
Tamura, M.3
Nishio, Y.4
Kajita, K.5
-
5
-
-
79051471432
-
-
10.1209/0295-5075/80/47002
-
N. Tajima, S. Sugawara, M. Tamura, R. Kato, Y. Nishio, and K. Kajita, EPL 80, 47002 (2007). 10.1209/0295-5075/80/47002
-
(2007)
EPL
, vol.80
, pp. 47002
-
-
Tajima, N.1
Sugawara, S.2
Tamura, M.3
Kato, R.4
Nishio, Y.5
Kajita, K.6
-
6
-
-
24644475825
-
-
10.1143/JPSJ.74.511
-
N. Tajima, J. Fujisawa, N. Naka, T. Ishihara, R. Kato, Y. Nishio, and K. Kajita, J. Phys. Soc. Jpn. 74, 511 (2005). 10.1143/JPSJ.74.511
-
(2005)
J. Phys. Soc. Jpn.
, vol.74
, pp. 511
-
-
Tajima, N.1
Fujisawa, J.2
Naka, N.3
Ishihara, T.4
Kato, R.5
Nishio, Y.6
Kajita, K.7
-
7
-
-
41549132125
-
-
10.1103/PhysRevB.77.125131
-
S. Iwai, K. Yamamoto, F. Hiramatsu, H. Nakaya, Y. Kawakami, and K. Yakushi, Phys. Rev. B 77, 125131 (2008). 10.1103/PhysRevB.77.125131
-
(2008)
Phys. Rev. B
, vol.77
, pp. 125131
-
-
Iwai, S.1
Yamamoto, K.2
Hiramatsu, F.3
Nakaya, H.4
Kawakami, Y.5
Yakushi, K.6
-
8
-
-
54349098480
-
-
10.1143/JPSJ.77.074709
-
K. Yamamoto, S. Iwai, S. Boyko, A. Kashiwazaki, F. Hiramatsu, C. Okabe, N. Nishi, and K. Yakushi, J. Phys. Soc. Jpn. 77, 074709 (2008). 10.1143/JPSJ.77.074709
-
(2008)
J. Phys. Soc. Jpn.
, vol.77
, pp. 074709
-
-
Yamamoto, K.1
Iwai, S.2
Boyko, S.3
Kashiwazaki, A.4
Hiramatsu, F.5
Okabe, C.6
Nishi, N.7
Yakushi, K.8
-
9
-
-
0021479774
-
-
10.1080/00268948408078687
-
K. Bender, I. Henning, D. Schweitzer, K. Dietz, H. Endres, and H. J. Keller, Mol. Cryst. Liq. Cryst. 108, 359 (1984). 10.1080/00268948408078687
-
(1984)
Mol. Cryst. Liq. Cryst.
, vol.108
, pp. 359
-
-
Bender, K.1
Henning, I.2
Schweitzer, D.3
Dietz, K.4
Endres, H.5
Keller, H.J.6
-
10
-
-
0000917407
-
-
10.1246/cl.1984.957
-
T. Mori, A. Kobayashi, Y. Sasaki, H. Kobayashi, G. Saito, and H. Ionokuchi, Chem. Lett. 13, 957 (1984). 10.1246/cl.1984.957
-
(1984)
Chem. Lett.
, vol.13
, pp. 957
-
-
Mori, T.1
Kobayashi, A.2
Sasaki, Y.3
Kobayashi, H.4
Saito, G.5
Ionokuchi, H.6
-
13
-
-
0034417997
-
-
10.1143/JPSJ.69.805
-
H. Seo, J. Phys. Soc. Jpn. 69, 805 (2000). 10.1143/JPSJ.69.805
-
(2000)
J. Phys. Soc. Jpn.
, vol.69
, pp. 805
-
-
Seo, H.1
-
14
-
-
33646791681
-
-
10.1051/jp4:2004114096
-
S. Moroto, K.-I. Hiraki, Y. Takano, Y. Kubo, T. Takahashi, and T. Nakamura, J. Phys. IV 114, 399 (2004). 10.1051/jp4:2004114096
-
(2004)
J. Phys. IV
, vol.114
, pp. 399
-
-
Moroto, S.1
Hiraki, K.-I.2
Takano, Y.3
Kubo, Y.4
Takahashi, T.5
Nakamura, T.6
-
15
-
-
0043207385
-
-
10.1103/PhysRevB.67.224105
-
R. Wojciechowski, K. Yamamoto, K. Yakushi, M. Inokuchi, and A. Kawamoto, Phys. Rev. B 67, 224105 (2003). 10.1103/PhysRevB.67.224105
-
(2003)
Phys. Rev. B
, vol.67
, pp. 224105
-
-
Wojciechowski, R.1
Yamamoto, K.2
Yakushi, K.3
Inokuchi, M.4
Kawamoto, A.5
-
16
-
-
36148964439
-
-
10.1143/JPSJ.76.113702
-
T. Kakiuchi, Y. Wakabayashi, H. Sawa, T. Takahashi, and T. Nakamura, J. Phys. Soc. Jpn. 76, 113702 (2007). 10.1143/JPSJ.76.113702
-
(2007)
J. Phys. Soc. Jpn.
, vol.76
, pp. 113702
-
-
Kakiuchi, T.1
Wakabayashi, Y.2
Sawa, H.3
Takahashi, T.4
Nakamura, T.5
-
17
-
-
0022904320
-
-
10.1016/0379-6779(86)90173-6
-
Y. Nogami, S. Kagoshima, T. Sugano, and G. Saito, Synth. Met. 16, 367 (1986). 10.1016/0379-6779(86)90173-6
-
(1986)
Synth. Met.
, vol.16
, pp. 367
-
-
Nogami, Y.1
Kagoshima, S.2
Sugano, T.3
Saito, G.4
-
18
-
-
0026943738
-
-
10.1016/0038-1098(92)90464-K
-
C. P. Heidmann, A. Bansteiner, F. Grob-Alltag, B. S. Chandrasekhar, and E. Hess, Solid State Commun. 84, 711 (1992). 10.1016/0038-1098(92)90464-K
-
(1992)
Solid State Commun.
, vol.84
, pp. 711
-
-
Heidmann, C.P.1
Bansteiner, A.2
Grob-Alltag, F.3
Chandrasekhar, B.S.4
Hess, E.5
-
19
-
-
0026190284
-
-
10.1016/0038-1098(91)90647-E
-
N. A. Fortune, K. Murata, M. Ishibashi, M. Tokumoto, N. Kinoshita, and H. Anzai, Solid State Commun. 79, 265 (1991). 10.1016/0038-1098(91)90647-E
-
(1991)
Solid State Commun.
, vol.79
, pp. 265
-
-
Fortune, N.A.1
Murata, K.2
Ishibashi, M.3
Tokumoto, M.4
Kinoshita, N.5
Anzai, H.6
-
20
-
-
0027660333
-
-
10.1016/0379-6779(93)91180-A
-
J. Moldenhauer, Ch. Horn, K. I. Pokhodnia, D. Schweitzer, I. Heinen, and H. J. Keller, Synth. Met. 60, 31 (1993). 10.1016/0379-6779(93)91180-A
-
(1993)
Synth. Met.
, vol.60
, pp. 31
-
-
Moldenhauer, J.1
Horn, Ch.2
Pokhodnia, K.I.3
Schweitzer, D.4
Heinen, I.5
Keller, H.J.6
-
21
-
-
24344474080
-
-
10.1021/jp050247o
-
T. Yamamoto, M. Uruichi, K. Yamamoto, K. Yakushi, A. Kawamoto, and H. Taniguchi, J. Phys. Chem. B 109, 15226 (2005). 10.1021/jp050247o
-
(2005)
J. Phys. Chem. B
, vol.109
, pp. 15226
-
-
Yamamoto, T.1
Uruichi, M.2
Yamamoto, K.3
Yakushi, K.4
Kawamoto, A.5
Taniguchi, H.6
-
22
-
-
0034380063
-
-
10.1143/JPSJ.69.543
-
N. Tajima, M. Tamura, Y. Nishio, K. Kajita, and Y. Iye, J. Phys. Soc. Jpn. 69, 543 (2000). 10.1143/JPSJ.69.543
-
(2000)
J. Phys. Soc. Jpn.
, vol.69
, pp. 543
-
-
Tajima, N.1
Tamura, M.2
Nishio, Y.3
Kajita, K.4
Iye, Y.5
-
23
-
-
0344386965
-
-
10.1051/jphys:01990005109086900
-
V. Železný, J. Petzelt, R. Swietlik, B. P. Corshunov, A. A. Volkov, G. V. Kozlov, D. Schweitzer, and H. J. Keller, J. Phys. (France) 51, 869 (1990). 10.1051/jphys:01990005109086900
-
(1990)
J. Phys. (France)
, vol.51
, pp. 869
-
-
Železný, V.1
Petzelt, J.2
Swietlik, R.3
Corshunov, B.P.4
Volkov, A.A.5
Kozlov, G.V.6
Schweitzer, D.7
Keller, H.J.8
-
24
-
-
0004705024
-
-
10.1051/jp1:1994162
-
M. Dressel, G. Gruner, J. P. Pouget, A. Breining, and D. Schweitzer, J. Phys. IV 4, 579 (1994). 10.1051/jp1:1994162
-
(1994)
J. Phys. IV
, vol.4
, pp. 579
-
-
Dressel, M.1
Gruner, G.2
Pouget, J.P.3
Breining, A.4
Schweitzer, D.5
-
25
-
-
21144457459
-
-
10.1143/JPSJ.73.116
-
M. Watanabe, Y. Noda, Y. Nogami, and H. Mori, J. Phys. Soc. Jpn. 73, 116 (2004). 10.1143/JPSJ.73.116
-
(2004)
J. Phys. Soc. Jpn.
, vol.73
, pp. 116
-
-
Watanabe, M.1
Noda, Y.2
Nogami, Y.3
Mori, H.4
-
26
-
-
0034529179
-
-
10.1246/bcsj.73.2643
-
K. Yakushi, Bull. Chem. Soc. Jpn. 73, 2643 (2000). 10.1246/bcsj.73.2643
-
(2000)
Bull. Chem. Soc. Jpn.
, vol.73
, pp. 2643
-
-
Yakushi, K.1
-
27
-
-
67649226742
-
-
10.1143/JPSJ.78.044701
-
Y. Yue, C. Nakano, K. Yamamoto, M. Uruichi, R. Wojciechowski, M. Inokuchi, and K. Yakushi, J. Phys. Soc. Jpn. 78, 044701 (2009). 10.1143/JPSJ.78.044701
-
(2009)
J. Phys. Soc. Jpn.
, vol.78
, pp. 044701
-
-
Yue, Y.1
Nakano, C.2
Yamamoto, K.3
Uruichi, M.4
Wojciechowski, R.5
Inokuchi, M.6
Yakushi, K.7
-
28
-
-
0035566262
-
-
10.1143/JPSJ.70.3728
-
M. Maksimuk, K. Yakushi, H. Taniguchi, K. Kanoda, and A. Kawamoto, J. Phys. Soc. Jpn. 70, 3728 (2001). 10.1143/JPSJ.70.3728
-
(2001)
J. Phys. Soc. Jpn.
, vol.70
, pp. 3728
-
-
Maksimuk, M.1
Yakushi, K.2
Taniguchi, H.3
Kanoda, K.4
Kawamoto, A.5
-
29
-
-
77957556720
-
-
-1.
-
- 1.
-
-
-
-
30
-
-
77957570667
-
-
Strictly speaking, the linear relationship cannot be applied straightforwardly to the estimation of site charge of charge-rich sites because a dipole-dipole interaction occurs between the phonon modes of charge-rich sites. However, the perturbation of the frequency by this dipole-dipole interaction is very small. This situation is similar to the case of the ν2 mode, in which the frequency is perturbed not only by site charge but also by weak electron-molecular-vibration interaction.
-
Strictly speaking, the linear relationship cannot be applied straightforwardly to the estimation of site charge of charge-rich sites because a dipole-dipole interaction occurs between the phonon modes of charge-rich sites. However, the perturbation of the frequency by this dipole-dipole interaction is very small. This situation is similar to the case of the ν 2 mode, in which the frequency is perturbed not only by site charge but also by weak electron-molecular-vibration interaction.
-
-
-
-
31
-
-
77957555013
-
-
10.1016/j.physb.2010.01.082
-
Y. Yue, K. Yamamoto, C. Nakano, M. Uruichi, K. Yakushi, M. Inokuchi, T. Hiejima, and A. Kawamoto, Physica B 405, S232 (2010). 10.1016/j.physb.2010.01. 082
-
(2010)
Physica B
, vol.405
, pp. 232
-
-
Yue, Y.1
Yamamoto, K.2
Nakano, C.3
Uruichi, M.4
Yakushi, K.5
Inokuchi, M.6
Hiejima, T.7
Kawamoto, A.8
-
32
-
-
55449118957
-
-
10.1103/PhysRevB.78.165119
-
T. Kawai and A. Kawamoto, Phys. Rev. B 78, 165119 (2008). 10.1103/PhysRevB.78.165119
-
(2008)
Phys. Rev. B
, vol.78
, pp. 165119
-
-
Kawai, T.1
Kawamoto, A.2
-
34
-
-
77957603084
-
-
The linewidth of the ν23 mode involves the effect of the hidden ν22 mode. It is therefore inappropriate to compare the linewidths of the ν23 of different compounds since the separation between ν22 and ν23 differs slightly between α- (ET ) 2 I3 and α- (ET ) 2 NH4 Hg (SCN ) 4.
-
The linewidth of the ν 2 3 mode involves the effect of the hidden ν 2 2 mode. It is therefore inappropriate to compare the linewidths of the ν 2 3 of different compounds since the separation between ν 2 2 and ν 2 3 differs slightly between α - (ET) 2 I 3 and α - (ET) 2 NH 4 Hg (SCN) 4.
-
-
-
-
35
-
-
84949218859
-
-
10.1002/9780470143605.ch6
-
R. Kubo, Adv. Chem. Phys. 15, 101 (1969). 10.1002/9780470143605.ch6
-
(1969)
Adv. Chem. Phys.
, vol.15
, pp. 101
-
-
Kubo, R.1
-
37
-
-
77957569077
-
-
-1 ), we neglected the effect of the slit function
-
- 1), we neglected the effect of the slit function.
-
-
-
-
38
-
-
77957566976
-
-
To obtain the second moment of the spectrum, a much wider spectral range should be integrated.
-
To obtain the second moment of the spectrum, a much wider spectral range should be integrated.
-
-
-
-
39
-
-
77957582941
-
-
note
-
) 2]. As the site charge should be in the range of 0 < x < 1, the variance was restricted to the range of 3 Δ c < ∼ 0.4.
-
-
-
-
42
-
-
1042299877
-
-
note
-
Similar results were reported by Merino They calculated the dynamical charge susceptibility and charge correlation function using a square lattice model. The collective mode which corresponds to a checkerboard CO is very softened, when the Coulomb interaction is close to a critical value. J. Merino, A. Greco, R. H. McKenzie, and M. Calandra, Phys. Rev. B 68, 245121 (2003). 10.1103/PhysRevB.68.245121
-
(2003)
Phys. Rev. B
, vol.68
, pp. 245121
-
-
Merino, J.1
Greco, A.2
McKenzie, R.H.3
Calandra, M.4
-
43
-
-
77957600440
-
-
note
-
- 1) of the vibronic ν 3 mode.
-
-
-
-
44
-
-
0001370990
-
-
10.1103/PhysRevB.58.9460
-
G. Visentini, M. Masino, C. Bellitto, and A. Girlando, Phys. Rev. B 58, 9460 (1998). 10.1103/PhysRevB.58.9460
-
(1998)
Phys. Rev. B
, vol.58
, pp. 9460
-
-
Visentini, G.1
Masino, M.2
Bellitto, C.3
Girlando, A.4
-
45
-
-
0000861914
-
-
10.1016/0584-8539(89)80039-X;
-
M. E. Kozlov, K. I. Pokhondnia, and A. A. Yuruchenio, Spectrochim. Acta, Part A 45, 437 (1989) 10.1016/0584-8539(89)80039-X
-
(1989)
Spectrochim. Acta, Part A
, vol.45
, pp. 437
-
-
Kozlov, M.E.1
Pokhondnia, K.I.2
Yuruchenio, A.A.3
-
46
-
-
0001541684
-
-
10.1016/0584-8539(94)00236-5
-
J. E. Eldridge, C. C. Homes, J. M. Williams, A. M. Kini, and H. Hau Wang, Spectrochim. Acta, Part A 51, 947 (1995). 10.1016/0584-8539(94)00236-5
-
(1995)
Spectrochim. Acta, Part A
, vol.51
, pp. 947
-
-
Eldridge, J.E.1
Homes, C.C.2
Williams, J.M.3
Kini, A.M.4
Hau Wang, H.5
-
47
-
-
77957557620
-
-
As to the lattice modes, this compound involves 33 optical phonons which are classified into 3 Ag +12 Au translational modes and 15 Ag +3 Au librational modes, when the space group is P 1̄. The Ag mode is Raman active and the Au mode is infrared active. In the CO state, however, the selection rule is broken, and all of the lattice modes are detectable in both infrared and Raman spectra.
-
As to the lattice modes, this compound involves 33 optical phonons which are classified into 3 A g + 12 A u translational modes and 15 A g + 3 A u librational modes, when the space group is P 1 ̄. The A g mode is Raman active and the A u mode is infrared active. In the CO state, however, the selection rule is broken, and all of the lattice modes are detectable in both infrared and Raman spectra.
-
-
-
-
48
-
-
0033515289
-
-
10.1016/S0921-4526(98)01372-6
-
R. G. Della Valle, A. Brillante, G. Visentini, and A. Girlando, Physica B 265, 195 (1999). 10.1016/S0921-4526(98)01372-6
-
(1999)
Physica B
, vol.265
, pp. 195
-
-
Della Valle, R.G.1
Brillante, A.2
Visentini, G.3
Girlando, A.4
-
49
-
-
0000089530
-
-
10.1007/BF02198145
-
K. I. Pokhodnia, A. Graja, M. Weger, and D. Schweitzer, Z. Phys. B: Condens. Matter 90, 127 (1993). 10.1007/BF02198145
-
(1993)
Z. Phys. B: Condens. Matter
, vol.90
, pp. 127
-
-
Pokhodnia, K.I.1
Graja, A.2
Weger, M.3
Schweitzer, D.4
-
51
-
-
77955408399
-
-
10.1103/PhysRevB.81.155111
-
N. Nakaya, K. Itoh, Y. Takahashi, H. Itoh, S. Iwai, S. Saito, K. Yamamoto, and K. Yakushi, Phys. Rev. B 81, 155111 (2010). 10.1103/PhysRevB.81. 155111
-
(2010)
Phys. Rev. B
, vol.81
, pp. 155111
-
-
Nakaya, N.1
Itoh, K.2
Takahashi, Y.3
Itoh, H.4
Iwai, S.5
Saito, S.6
Yamamoto, K.7
Yakushi, K.8
-
53
-
-
77957575062
-
-
The infrared light was focused on the rectangular area of 50μm×200μm. The spectrum was taken in the cooling process.
-
The infrared light was focused on the rectangular area of 50 μ m × 200 μ m. The spectrum was taken in the cooling process.
-
-
-
-
54
-
-
77957586184
-
-
The Raman spectrum was measured with the polarization of E||b on the (001) crystal face using α- ( C 13 -ET ) 2 I3, as the spectrum of metallic phase is very different from that of CO phase in this condition.
-
The Raman spectrum was measured with the polarization of E || b on the (001) crystal face using α - (C 13 -ET) 2 I 3, as the spectrum of metallic phase is very different from that of CO phase in this condition.
-
-
-
|