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1
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85037914968
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Min-Eum Sa, Seoul M.Y. Choi J.S. Chung, D. Kim
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For a list of references, see, e.g., Proceedings of the 2nd CTP Workshop on Statistical Physics: KT Transition and Superconducting Arrays, edited by D. Kim, J.S. Chung, and M.Y. Choi (Min-Eum Sa, Seoul, 1993);
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Proceedings of the 2nd CTP Workshop on Statistical Physics: KT Transition and Superconducting Arrays
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2
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0007130527
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Physica B 222, 253(1996);
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Physica B
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7
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S.P. Benz, M.S. Rzchowski, M. Tinkham, and C.J. Lobb, Phys. Rev. Lett. 64, 693 (1990).
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Phys. Rev. Lett.
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Benz, S.P.1
Rzchowski, M.S.2
Tinkham, M.3
Lobb, C.J.4
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10
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0008707781
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J.U. Free, S.P. Benz, M.S. Rzchowski, M. Tinkham, C.J. Lobb, and M. Octavio, Phys. Rev. B 41, 7267 (1990).
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Free, J.U.1
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Lobb, C.J.5
Octavio, M.6
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11
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0000525355
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M. Octavio, J.U. Free, S.P. Benz, R.S. Newrock, D.B. Mast, and C.J. Lobb, Phys. Rev. B 44, 4601 (1991).
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Phys. Rev. B
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Octavio, M.1
Free, J.U.2
Benz, S.P.3
Newrock, R.S.4
Mast, D.B.5
Lobb, C.J.6
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12
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5544263353
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P.H.E. Tiesinga, T.J. Hagenaars, J.E. van Himbergen, and J.V. José, J. Phys.: Condens. Matter 9, 1813 (1997).
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Tiesinga, P.H.E.1
Hagenaars, T.J.2
van Himbergen, J.E.3
José, J.V.4
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19
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85037909199
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The notation RSJ and TDGL in the present context refers to the dynamical equations; RSJ refers to Eq. (3) and TDGL to Eq. (4).
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The notation RSJ and TDGL in the present context refers to the dynamical equations; RSJ refers to Eq. (3) and TDGL to Eq. (4).
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24
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17044393275
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K.-H. Wagenblast and R. Fazio, JETP Lett. 68, 312 (1998).
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Fazio, R.1
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25
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0000475395
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P.H.E. Tiesinga, T.J. Hagenaars, J.E. van Himbergen, and J.V. José, Phys. Rev. Lett. 78, 519 (1997).
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Phys. Rev. Lett.
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Tiesinga, P.H.E.1
Hagenaars, T.J.2
van Himbergen, J.E.3
José, J.V.4
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26
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85037897154
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Some authors prefer to let the TDGL model with external currents exclusively denote the case of an open boundary. This corresponds to the case when the normal current is short circuit to the ground. The TDGL model with FTBC used here instead corresponds to the case when the normal current flow is through the array (see Ref. 26
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Some authors prefer to let the TDGL model with external currents exclusively denote the case of an open boundary. This corresponds to the case when the normal current is short circuit to the ground. The TDGL model with FTBC used here instead corresponds to the case when the normal current flow is through the array (see Ref. 26).
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30
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0001034046
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I.-J. Hwang and D. Stroud, Phys. Rev. B 57, 6036 (1998).
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Stroud, D.1
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32
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26344475497
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The FTBC introduced and explored in Ref. 15 has some antecedents in earlier works, e.g., H. Eikman and J.E. van Himbergen, Phys. Rev. B 41, 8927 (1990);
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Phys. Rev. B
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Eikman, H.1
van Himbergen, J.E.2
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37
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1642310884
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K. Ravindran, L.B. Gómez, R.R. Li, S.T. Herbert, P. Lukens, Y. Jun, S. Elhamri, R.S. Newrock, and D.B. Mast, Phys. Rev. B 53, 5141 (1996).
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Phys. Rev. B
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Ravindran, K.1
Gómez, L.B.2
Li, R.R.3
Herbert, S.T.4
Lukens, P.5
Jun, Y.6
Elhamri, S.7
Newrock, R.S.8
Mast, D.B.9
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38
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0142209749
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S.P. Benz, M.S. Rzchowski, M. Tinkham, and C.J. Lobb, Phys. Rev. B 42, 6165 (1990).
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(1990)
Phys. Rev. B
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Benz, S.P.1
Rzchowski, M.S.2
Tinkham, M.3
Lobb, C.J.4
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40
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85037875323
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Similarly to Eq. (2), the external current in Ref. 9 has been included as an effective bond angle term in the gauge-invariant phase difference.
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Similarly to Eq. (2), the external current in Ref. 9 has been included as an effective bond angle term in the gauge-invariant phase difference.
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41
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85037896745
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P.H.E. Tiesinga, Ph.D. thesis, Utrecht University, 1996.
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P.H.E. Tiesinga, Ph.D. thesis, Utrecht University, 1996.
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