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5
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0001350877
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The solid curve in Fig. 2 of this reference is well-approximated by a curve with the 3D-LLL scaling
-
M. J. W. Dodgson et al.: Phys. Rev. B 57 (1997) 14498. The solid curve in Fig. 2 of this reference is well-approximated by a curve with the 3D-LLL scaling.
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Dodgson, M.J.W.1
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R. Ikeda: Physica C 316 (1999) 189; Phys. Rev. Lett. 82 (1999) 3378.
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Ikeda, R.1
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R. Ikeda: Physica C 316 (1999) 189; Phys. Rev. Lett. 82 (1999) 3378.
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Phys. Rev. Lett.
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8
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26544478070
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W. Goeb et al.: Phys. Rev. B 62 (2000) 9780; G. D'Anna et al.: Phys. Rev. Lett. 81 (1998) 2530.
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Phys. Rev. B
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Goeb, W.1
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9
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0032555828
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W. Goeb et al.: Phys. Rev. B 62 (2000) 9780; G. D'Anna et al.: Phys. Rev. Lett. 81 (1998) 2530.
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Phys. Rev. Lett.
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D'Anna, G.1
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14
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0031999753
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V. M. Viriokur et al.: Physica C 295 (1998) 209; D. Ertas and D. R. Nelson: Physica C 272 (1996) 79.
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Physica C
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Vinokur, V.M.1
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V. M. Viriokur et al.: Physica C 295 (1998) 209; D. Ertas and D. R. Nelson: Physica C 272 (1996) 79.
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Ertas, D.1
Nelson, D.R.2
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16
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0033325568
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and private communication. The resistivity curves in the vortex slush region, clearly detected in this experiment, vanish algebraically just like in the ordinary VG-scaling. This is consistent with the theory in ref. 1 but, possibly, not with that of ref. 14 in which an argument of nonperturbative TAFF type was used to describe a vanishing of resistivity in the slush region
-
T. Nishizaki et al.: J. Low Temp. Phys. 117 (1999) 1375 and private communication. The resistivity curves in the vortex slush region, clearly detected in this experiment, vanish algebraically just like in the ordinary VG-scaling. This is consistent with the theory in ref. 1 but, possibly, not with that of ref. 14 in which an argument of nonperturbative TAFF type was used to describe a vanishing of resistivity in the slush region.
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J. Low Temp. Phys.
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Nishizaki, T.1
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4043158787
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W. Jiang et al.: Phys. Rev. Lett. 72 (1994) 550; D. S. Reed et al.: Phys. Rev. B 51 (1995) 16448.
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Jiang, W.1
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W. Jiang et al.: Phys. Rev. Lett. 72 (1994) 550; D. S. Reed et al.: Phys. Rev. B 51 (1995) 16448.
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Reed, D.S.1
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24
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0039099661
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note
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G), this is an artifact characteristic of the ordinary (phenomenological) GL model. Actually, in the ordinary dirty limit (defined at the electronic level), g̃3 is found to be positive even at low T limit where the ordinary GL model is inapplicable. In this paper, this complexity will not be discussed any more, and g̃3 is assumed to be always positive.
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25
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4243879901
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l by reflecting an enhanced thermal fluctuation, as seen in a report [A. Samoilov et al.: Phys. Rev. Lett. 76 (1996) 2728].
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Samoilov, A.1
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28
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0039691892
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note
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G itself increases by adding this disorder.
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29
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0040283612
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private communication
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W. K. Kwok: private communication.
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Kwok, W.K.1
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0002165194
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G. Blatter et al.: Phys. Rev. B 54 (1996) 72; S. Ooi et al.: Phys. Rev. Lett. 82 (1999) 4308.
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G. Blatter et al.: Phys. Rev. B 54 (1996) 72; S. Ooi et al.: Phys. Rev. Lett. 82 (1999) 4308.
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Ooi, S.1
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0033338531
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Note that the LLL fluctuation strength in 2D limit is given, except the dependences on universal constants, by B/(ΔCd).
-
A drastic decrease of heat capacity jump ΔC with increasing oxygen deficiency in YBCO is seen [e.g., M. Ido et al., J. Low Temp. Phys. 117 (1999) 329]. Note that the LLL fluctuation strength in 2D limit is given, except the dependences on universal constants, by B/(ΔCd).
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J. Low Temp. Phys.
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Ido, M.1
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33
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0039691891
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note
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-1/2), and hence the vortex slush regime becomes wider.
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35
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0026939918
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G. Blatter, V. B. Geshkenbein and A. I. Larkin: Phys. Rev. Lett. 68 (1992) 875; R. Ikeda: Physica C 201 (1992) 386.
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cond-mat/0008092
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Y. Paltiel et al.: cond-mat/0008092.
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Paltiel, Y.1
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