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0000016599
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Fiz. Tverd. Tela (Leningrad) 2, 2031 (1960) [, ]. SPSSA7
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V. L. Ginsburg, Fiz. Tverd. Tela (Leningrad) 2, 2031 (1960) [Sov. Phys. Solid State 2, 1824 (1960)].SPSSA7
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Ginsburg, V.L.1
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8
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0000047249
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K. Ema, J. Watanabe, A. Takagi, and H. Yao, Phys. Rev. E 52, 1216 (1995).PLEEE8
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Ema, K.1
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9
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5644227323
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K. Ema, H. Yao, A. Fukuda, Y. Takanishi, and H. Takezoe, Phys. Rev. E 54, 4450 (1996).PLEEE8
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Ema, K.1
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Takezoe, H.5
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12
-
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0345976596
-
-
It was found that racemate of MHPOBC exhibits a non-Landau tricritical [formula presented] transition. See PLEEE8
-
It was found that racemate of MHPOBC exhibits a non-Landau tricritical Sm-A–Sm-C transition. See K. Ema, A. Takagi, and H. Yao, Phys. Rev. E 53, R3036 (1996); PLEEE8
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Phys. Rev. E
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Ema, K.1
Takagi, A.2
Yao, H.3
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14
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0021555675
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edited by C. Domb, J. L. Lebowitz, Academic, New York
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I. D. Lawrie and S. Sarbach, in Phase Transitions and Critical Phenomena, edited by C. Domb and J. L. Lebowitz (Academic, New York, 1984), Vol. 9.
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Lawrie, I.D.1
Sarbach, S.2
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22
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0001664523
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and references cited therin. ZPCMDN
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B. M. Ocko, R. J. Birgeneau, and J. D. Litster, Z. Phys. B 62, 487 (1986), and references cited therin.ZPCMDN
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Ocko, B.M.1
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23
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5844299723
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and references therein. PRLTAO
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J. Thoen, H. Marynissen, and W. Van Dael, Phys. Rev. Lett. 52, 204 (1984), and references therein.PRLTAO
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Thoen, J.1
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Van Dael, W.3
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28
-
-
85036221924
-
-
We note that the racemic mixture is an exceptional case. This is because Fisher renormalization depends on [formula presented] being large, and [formula presented] for racemates
-
We note that the racemic mixture is an exceptional case. This is because Fisher renormalization depends on d(ln Tc)/dX being large, and d(ln Tc)/dX=0 for racemates.
-
-
-
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29
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0024706163
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A. D. L. Chandani, Y. Ouchi, H. Takezoe, A. Fukuda, K. Terashima, K. Furukawa, and A. Kishi, Jpn. J. Appl. Phys., Part 2 28, L1261 (1989); JAPLD8
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Chandani, A.D.L.1
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Kishi, A.7
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30
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0026224154
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Y. Takanishi, K. Hiraoka, V. K. Agrawal, H. Takezoe, A. Fukuda, and M. Matsushita, Jpn. J. Appl. Phys. Part 1 30, 2023 (1991)
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Takanishi, Y.1
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31
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0026240936
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K. Hiraoka, Y. Takanishi, K. Skarp, H. Takezoe, and A. Fukuda, Jpn. J. Appl. J. Phys. Part 2 30, L1819 (1991).JAPLD8
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32
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77949951925
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N. Okabe, Y. Suzuki, I. Kawamura, T. Isozaki, H. Takezoe, and A. Fukuda, Jpn. J. Appl. Phys., Part 2 31, L793 (1992).JAPLD8
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Okabe, N.1
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Fukuda, A.6
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33
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0026219310
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T. Isozaki, Y. Suzuki, I. Kawamura, K. Mori, N. Yamamoto, Y. Yamada, H. Orihara, and Y. Ishibashi, Jpn. J. Appl. Phys., Part 2 30, L1573 (1991); JAPLD8
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Ishibashi, Y.8
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34
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84947154720
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T. Isozaki, K. Hiraoka, Y. Takanishi, H. Takezoe, A. Fukuda, Y. Suzuki, and I. Kawamura, Liq. Cryst. 12, 59 (1992).LICRE6
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Fukuda, A.5
Suzuki, Y.6
Kawamura, I.7
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35
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0000708104
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K. Itoh, M. Kabe, K. Miyachi, Y. Takanishi, K. Ishikawa, H. Takezoe, and A. Fukuda, J. Mater. Chem. 7, 407 (1997).JMACEP
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Itoh, K.1
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Fukuda, A.7
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36
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0008984112
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K. Ema, M. Ogawa, A. Takagi, and H. Yao, Phys. Rev. E 54, R25 (1996).PLEEE8
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Ema, K.1
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37
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0027577951
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K. Ema, T. Uematsu, A. Sugata, and H. Yao, Jpn. J. Appl. Phys., Part 1 32, 1846 (1993).JAPNDE
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Ema, K.1
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Yao, H.4
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38
-
-
85036226134
-
-
Because of an insufficient calibration of the thermometer used just after the completion of the improved calorimeter, it was found that the temperature scale should be shifted by about 0.4 K in the results of Ref. 8
-
Because of an insufficient calibration of the thermometer used just after the completion of the improved calorimeter, it was found that the temperature scale should be shifted by about 0.4 K in the results of Ref. 8.
-
-
-
-
41
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0000313073
-
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C. Bagnuls, C. Bervillier, D. I. Meiron, and B. G. Nickel, Phys. Rev. B 35, 3585 (1987).PRBMDO
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Bagnuls, C.1
Bervillier, C.2
Meiron, D.I.3
Nickel, B.G.4
-
42
-
-
0001139945
-
-
The theory in Ref. 33 has been applied for the [formula presented] transition in PLEEE8
-
The theory in Ref. 33 has been applied for the N–Sm-A transition in C. W. Garland, G. Nounesis, M. J. Young, and R. J. Birgeneau, Phys. Rev. E 47, 1918 (1993).PLEEE8
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Phys. Rev. E
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Garland, C.W.1
Nounesis, G.2
Young, M.J.3
Birgeneau, R.J.4
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44
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21844497176
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H. Haga, A. Onodera, Y. Shiozaki, K. Ema, and H. Sakata, J. Phys. Soc. Jpn. 64, 822 (1995).JUPSAU
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Haga, H.1
Onodera, A.2
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Ema, K.4
Sakata, H.5
-
45
-
-
3843125208
-
-
[formula presented] is expected in the ε-expansion calculation to leading order ε. See , PRLTAO
-
D1+=D1- is expected in the ε-expansion calculation to leading order ε. See A. Aharony and G. Ahlers, Phys. Rev. Lett. 44, 782 (1980).PRLTAO
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Phys. Rev. Lett.
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Aharony, A.1
Ahlers, G.2
-
46
-
-
85036407153
-
-
The values of [formula presented] obtained in the ε expansion up to higher order and in the field theory are only slightly larger than unity for 3D [formula presented] universality class: 1.17 and 1.6, respectively. See V. Privman, P. C. Hohenberg, and A. Aharony, in Phase Transitions and Critical Phenomena, edited by C. Domb and J. L. Lebowitz (Academic, New York, 1991), Vol. 14
-
The values of D1+/D1- obtained in the ε expansion up to higher order and in the field theory are only slightly larger than unity for 3D XY universality class: 1.17 and 1.6, respectively. See V. Privman, P. C. Hohenberg, and A. Aharony, in Phase Transitions and Critical Phenomena, edited by C. Domb and J. L. Lebowitz (Academic, New York, 1991), Vol. 14.
-
-
-
-
52
-
-
85036177468
-
-
[formula presented] However, we found that the dependence of σ on τ yields only small effect and can be neglected practically in fitting the experimental data., To be precise, τ should be replaced by στ rather than [formula presented] where σ is determined in a consistent manner at each temperature. If [formula presented] then [formula presented] for all τ. For nonzero [formula presented] σ takes a value between [formula presented]
-
To be precise, τ should be replaced by στ rather than -2τ, where σ is determined in a consistent manner at each temperature. If v=0 then σ=-2 for all τ. For nonzero v, σ takes a value between -3 and -2. However, we found that the dependence of σ on τ yields only small effect and can be neglected practically in fitting the experimental data.
-
-
-
-
53
-
-
11544275571
-
-
Also see, for instance, I. D. Lawrie, J. Phys. A 12, 919 (1979).JPHAC5
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J. Phys. A
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, pp. 919
-
-
Lawrie, I.D.1
-
54
-
-
85036423944
-
-
We also tried fits by numerically differentiating [formula presented] by τ. The result was essentially the same
-
We also tried fits by numerically differentiating F(M) by τ. The result was essentially the same.
-
-
-
|