-
2
-
-
12944257434
-
-
P. Jung, Phys. Rep. 234, 175 (1994)
-
(1994)
Phys. Rep.
, vol.234
, pp. 175
-
-
Jung, P.1
-
3
-
-
0039065101
-
-
L. Gammaitoni, P. Hänggi, P. Jung, and F. Marchesoni, Rev. Mod. Phys. 70, 223 (1998).
-
(1998)
Rev. Mod. Phys.
, vol.70
, pp. 223
-
-
Gammaitoni, L.1
Hänggi, P.2
Jung, P.3
Marchesoni, F.4
-
9
-
-
0000371732
-
-
Springer, Berlin
-
P. Hänggi and R. Bartussek, in Nonlinear Physics of Complex Systems, Lectures Notes in Physics, Vol. 476 (Springer, Berlin, 1996) pp. 294-308.
-
(1996)
Nonlinear Physics of Complex Systems, Lectures Notes in Physics, Vol. 476
, pp. 294-308
-
-
Hänggi, P.1
Bartussek, R.2
-
10
-
-
0028085872
-
-
J. Rousselet, L. Salome, A. Ajdari, and J. Prost, Nature (London) 370, 446 (1994).
-
(1994)
Nature (London)
, vol.370
, pp. 446
-
-
Rousselet, J.1
Salome, L.2
Ajdari, A.3
Prost, J.4
-
11
-
-
0033595268
-
-
C.S. Lee, B. Janko, I. Derényi, and A.L. Barabasi, Nature (London) 400, 337 (1999).
-
(1999)
Nature (London)
, vol.400
, pp. 337
-
-
Lee, C.S.1
Janko, B.2
Derényi, I.3
Barabasi, A.L.4
-
13
-
-
0030288152
-
-
and references therein
-
See L.M. Floría and J.J. Mazo, Adv. Phys. 45, 505 (1996), and references therein.
-
(1996)
Adv. Phys.
, vol.45
, pp. 505
-
-
Floría, L.M.1
Mazo, J.J.2
-
15
-
-
0030263090
-
-
S. Watanabe, H.S.J. van der Zant, S.H. Strogatz, and T.P. Orlando, Physica D 97, 429 (1996).
-
(1996)
Physica D
, vol.97
, pp. 429
-
-
Watanabe, S.1
van der Zant, H.S.J.2
Strogatz, S.H.3
Orlando, T.P.4
-
16
-
-
4243715037
-
-
D.J. Resnick, J.C. Garland, J.T. Boyd, S. Shoemaker, and R.S. Newrock, Phys. Rev. Lett. 47, 1542 (1981).
-
(1981)
Phys. Rev. Lett.
, vol.47
, pp. 1542
-
-
Resnick, D.J.1
Garland, J.C.2
Boyd, J.T.3
Shoemaker, S.4
Newrock, R.S.5
-
17
-
-
0033558653
-
-
F. Falo, P.J. Martínez, J.J. Mazo, and S. Cilla, Europhys. Lett. 45, 700 (1999).
-
(1999)
Europhys. Lett.
, vol.45
, pp. 700
-
-
Falo, F.1
Martínez, P.J.2
Mazo, J.J.3
Cilla, S.4
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18
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85036299017
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To derive the circuit equations we need to apply both Kirchhoff’s current law (KCL) at the nodes and Kirchhoff’s voltage law (KVL) for each loop. In circuits with Josephson junctions, KVL is superseded by the more stringent requirement of flux quantization. Flux quantization gives a constraint on the flux of a loop while KVL only constrains the derivative of the flux, i.e. the voltage. Satisfying flux quantization automatically satisfies KVL
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To derive the circuit equations we need to apply both Kirchhoff’s current law (KCL) at the nodes and Kirchhoff’s voltage law (KVL) for each loop. In circuits with Josephson junctions, KVL is superseded by the more stringent requirement of flux quantization. Flux quantization gives a constraint on the flux of a loop while KVL only constrains the derivative of the flux, i.e. the voltage. Satisfying flux quantization automatically satisfies KVL.
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19
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85036394292
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We have used the Josephson-voltage relation (Formula presented) and set the damping (Formula presented) to (Formula presented). The damping is usually referred to as the Stewart-McCumber parameter (Formula presented)
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We have used the Josephson-voltage relation (Formula presented) and set the damping (Formula presented) to (Formula presented). The damping is usually referred to as the Stewart-McCumber parameter (Formula presented).
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20
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85036271389
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the case of an open array, where open boundary conditions must be imposed, (Formula presented) (Formula presented) and (Formula presented) otherwise
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In the case of an open array, where open boundary conditions must be imposed, (Formula presented) (Formula presented) and (Formula presented) otherwise.
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21
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85036143009
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There are several ways of calculating the periodicity in M of the sine-Gordon equation (regular array). Probably the most straightforward is to find a transformation that moves the M dependence from the boundary conditions to the sine term. In the case of the regular discrete sine-Gordon equation the new phases are just (Formula presented). Then M appears only in (Formula presented) and the periodicity of the equations in M is just (Formula presented). Though this approach can also be used in an inhomogeneous ring, it is not trivial to guess the correct transformation
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There are several ways of calculating the periodicity in M of the sine-Gordon equation (regular array). Probably the most straightforward is to find a transformation that moves the M dependence from the boundary conditions to the sine term. In the case of the regular discrete sine-Gordon equation the new phases are just (Formula presented). Then M appears only in (Formula presented) and the periodicity of the equations in M is just (Formula presented). Though this approach can also be used in an inhomogeneous ring, it is not trivial to guess the correct transformation.
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22
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85036406543
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Due to the convex (i.e., inductive) character of the inter-junction coupling all the junctions show the same dc (Formula presented) curve
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Due to the convex (i.e., inductive) character of the inter-junction coupling all the junctions show the same dc (Formula presented) curve.
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24
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85036359358
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FASTHENRY, see http://rle-vlsi.mit.edu. See also E. Trías, Ph.D. thesis, Massachusetts Institute of Technology, 2000
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FASTHENRY, see http://rle-vlsi.mit.edu. See also E. Trías, Ph.D. thesis, Massachusetts Institute of Technology, 2000.
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25
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85036245498
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This corresponds to a perturbative expansion from the so-called anti-integrable limit (Formula presented), which can be rigorously justified [C. Baesens (private communication)]
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This corresponds to a perturbative expansion from the so-called anti-integrable limit (Formula presented), which can be rigorously justified [C. Baesens (private communication)].
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27
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84907889046
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for underdamped effects in a ratchet potential
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See, for example, P. Jung, J.G. Kissner, and P. Hänggi, Phys. Rev. Lett. 76, 3436 (1996), for underdamped effects in a ratchet potential.
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(1996)
Phys. Rev. Lett.
, vol.76
, pp. 3436
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Jung, P.1
Kissner, J.G.2
Hänggi, P.3
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