-
2
-
-
0035846688
-
-
F. Bouquet, Y. Wang, R.A. Fisher, D.G. Hinks, J.D. Jorgensen, A. Junod, and N.E. Phillips, Europhys. Lett. 56, 856 (2001).
-
(2001)
Europhys. Lett.
, vol.56
, pp. 856
-
-
Bouquet, F.1
Wang, Y.2
Fisher, R.A.3
Hinks, D.G.4
Jorgensen, J.D.5
Junod, A.6
Phillips, N.E.7
-
3
-
-
0037171180
-
-
H. Schmidt, J.F. Zasadzinski, K.E. Gray, and D.G. Hinks, Phys. Rev. Lett. 88, 127002 (2002).
-
(2002)
Phys. Rev. Lett.
, vol.88
, pp. 127002
-
-
Schmidt, H.1
Zasadzinski, J.F.2
Gray, K.E.3
Hinks, D.G.4
-
5
-
-
0000837328
-
-
M. Angst, R. Puzniak, A. Wisniewski, J. Jun, S.M. Kazakov, J. Karpinski, J. Roos, and H. Keller, Phys. Rev. Lett. 88, 167004 (2002).
-
(2002)
Phys. Rev. Lett.
, vol.88
, pp. 167004
-
-
Angst, M.1
Puzniak, R.2
Wisniewski, A.3
Jun, J.4
Kazakov, S.M.5
Karpinski, J.6
Roos, J.7
Keller, H.8
-
6
-
-
0036563981
-
-
A.V. Sologubenko, J. Jun, S.M. Kazakov, J. Karpinski, and H.R. Ott, Phys. Rev. B 65, 180505(R)(2002).
-
(2002)
Phys. Rev. B
, vol.65
, pp. 180505
-
-
Sologubenko, A.V.1
Jun, J.2
Kazakov, S.M.3
Karpinski, J.4
Ott, H.R.5
-
8
-
-
4243685874
-
-
M. Zehetmayer, M. Eisterer, J. Jun, S.M. Kazakov, J. Karpinski, A. Wisniewski, and H.W. Weber, Phys. Rev. B 66, 052505 (2002).
-
(2002)
Phys. Rev. B
, vol.66
, pp. 52505
-
-
Zehetmayer, M.1
Eisterer, M.2
Jun, J.3
Kazakov, S.M.4
Karpinski, J.5
Wisniewski, A.6
Weber, H.W.7
-
9
-
-
85038956461
-
-
cond-mat/0203337, Phys. Rev. B (to be published 1 February 2003)
-
U. Welp et al., cond-mat/0203337, Phys. Rev. B (to be published 1 February 2003).
-
-
-
Welp, U.1
-
10
-
-
0029782809
-
-
A. Schilling, R.A. Fisher, N.E. Phillips, U. Welp, D. Dasgupta, W.K. Kwok, and G.W. Crabtree, Nature (London) 382, 791 (1996).
-
(1996)
Nature (London)
, vol.382
, pp. 791
-
-
Schilling, A.1
Fisher, R.A.2
Phillips, N.E.3
Welp, U.4
Dasgupta, D.5
Kwok, W.K.6
Crabtree, G.W.7
-
17
-
-
0035942756
-
-
We follow convention and treat melting and order-disorder transition separately, although there is evidence that they form one line of phase transitions, which just changes character from thermally driven to disorder driven. See N. Avraham et al., Nature (London) 411, 451 (2001).
-
(2001)
Nature (London)
, vol.411
, pp. 451
-
-
Avraham, N.1
-
18
-
-
85039025967
-
-
G. Ravikumar, V.C. Sahni, A.K. Grover, S. Ramakrishnan, P.L. Gammel, D.J. Bishop, E. Bucher, M.J. Higgins, and S. Bhattacharya, Phys. Rev. B 63, 024505 (2001).
-
(2001)
Phys. Rev. B
, vol.63
, pp. 24505
-
-
Ravikumar, G.1
Sahni, V.C.2
Grover, A.K.3
Ramakrishnan, S.4
Gammel, P.L.5
Bishop, D.J.6
Bucher, E.7
Higgins, M.J.8
Bhattacharya, S.9
-
20
-
-
0035133722
-
-
X.S. Ling, S.R. Park, B.A. McClain, S.M. Choi, D.C. Dender, and J.W. Lynn, Phys. Rev. Lett. 86, 712 (2001).
-
(2001)
Phys. Rev. Lett.
, vol.86
, pp. 712
-
-
Ling, X.S.1
Park, S.R.2
McClain, B.A.3
Choi, S.M.4
Dender, D.C.5
Lynn, J.W.6
-
21
-
-
0037156894
-
-
E.M. Forgan, S.J. Levett, P.G. Kealey, R. Cubitt, C.D. Dewhurst, and D. Fort, Phys. Rev. Lett. 88, 167003 (2002).
-
(2002)
Phys. Rev. Lett.
, vol.88
, pp. 167003
-
-
Forgan, E.M.1
Levett, S.J.2
Kealey, P.G.3
Cubitt, R.4
Dewhurst, C.D.5
Fort, D.6
-
22
-
-
85038936845
-
-
M.R. Eskildsen (private communication)
-
M.R. Eskildsen (private communication).
-
-
-
-
23
-
-
0036497117
-
-
M. Angst, S.M. Kazakov, J. Karpinski, A. Wisniewski, R. Puzniak, and M. Baran, Phys. Rev. B 65, 094518 (2002).
-
(2002)
Phys. Rev. B
, vol.65
, pp. 94518
-
-
Angst, M.1
Kazakov, S.M.2
Karpinski, J.3
Wisniewski, A.4
Puzniak, R.5
Baran, M.6
-
24
-
-
0036115610
-
-
V.V. Eremenko, V.A. Sirenko, Y.A. Shabakayeva, R. Schleser, and P.L. Gammel, Low Temp. Phys. 28, 6 (2002).
-
(2002)
Low Temp. Phys.
, vol.28
, pp. 6
-
-
Eremenko, V.V.1
Sirenko, V.A.2
Shabakayeva, Y.A.3
Schleser, R.4
Gammel, P.L.5
-
26
-
-
85038926432
-
-
The form of the MHL clearly indicates that a full reversal of the critical state (Ref. 24) is achieved
-
The form of the MHL clearly indicates that a full reversal of the critical state (Ref. 24) is achieved.
-
-
-
-
28
-
-
85038963073
-
-
A criterion (Formula presented) was used for defining (Formula presented)
-
A criterion (Formula presented) was used for defining (Formula presented)
-
-
-
-
30
-
-
85038901887
-
-
R. Puzniak et al. (unpublished)
-
R. Puzniak et al. (unpublished).
-
-
-
-
31
-
-
85038917435
-
-
The signal-to-noise ratio is decreased in lower fields, since (Formula presented)
-
The signal-to-noise ratio is decreased in lower fields, since (Formula presented)
-
-
-
-
32
-
-
85038926769
-
-
cond-mat/0206407 (unpublished)
-
M. Angst, R. Puzniak, A. Wisniewski, J. Roos, H. Keller, and J. Karpinski, cond-mat/0206407 (unpublished).
-
-
-
Angst, M.1
Puzniak, R.2
Wisniewski, A.3
Roos, J.4
Keller, H.5
Karpinski, J.6
-
35
-
-
0000147171
-
-
Combined ac susceptibility and dc magnetization measurements found the PE maximum to be located in fields equal to or even higher than the magnetization step signifying melting. See, e.g., J. Shi et al., Phys. Rev. B 60, R12 593 (1999);
-
(1999)
Phys. Rev. B
, vol.60
-
-
Shi, J.1
-
37
-
-
4644264872
-
-
T. Nishizaki, T. Naito, S. Okayasu, A. Iwase, and N. Kobayashi, Phys. Rev. B 61, 3649 (2000).
-
(2000)
Phys. Rev. B
, vol.61
, pp. 3649
-
-
Nishizaki, T.1
Naito, T.2
Okayasu, S.3
Iwase, A.4
Kobayashi, N.5
-
38
-
-
0037179325
-
-
M. Pissas, S. Lee, A. Yamamoto, and S. Tajima, Phys. Rev. Lett. 89, 097002 (2002).
-
(2002)
Phys. Rev. Lett.
, vol.89
, pp. 97002
-
-
Pissas, M.1
Lee, S.2
Yamamoto, A.3
Tajima, S.4
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