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10
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0033346173
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G. W. Crabtree, et al., JETP 117, 1313 (1999).
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(1999)
JETP
, vol.117
, pp. 1313
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Crabtree, G.W.1
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11
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85038270792
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G. W. Crabtree, et al., Physica C 341-348, 996 (2000).
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(2000)
Physica C
, vol.341-348
, pp. 996
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Crabtree, G.W.1
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13
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33646668527
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V. Ambegaokar, B. I. Halperin, D. R. Nelson, and E. D. Siggia, Phys. Rev. B 21, 1806 (1980).
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(1980)
Phys. Rev. B
, vol.21
, pp. 1806
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Ambegaokar, V.1
Halperin, B.I.2
Nelson, D.R.3
Siggia, E.D.4
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19
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0001337725
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See, e.g., edited by C. Domb and J. Lebowitz, Academic, London
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See, e.g., D. R. Nelson, in Phase Transitions and Critical Phenomena, edited by C. Domb and J. Lebowitz (Academic, London, 1983), Vol. 7, pp. 76-79.
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(1983)
Phase Transitions and Critical Phenomena
, vol.7
, pp. 76-79
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Nelson, D.R.1
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23
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85038317410
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No-slip boundary conditions for the displacement yield a stress of the form given in Eq. (2.12), but with the plus sign inside the square bracket replaced by a minus sign. In this case the stress is largest (in magnitude) at the inner and outer rims of the disk and vanishes in the interior. Plastic slip will occur first at the rims, and then propagate towards the interior of the disk as the current is increased. No-slip boundary conditions are relevant for the experimental geometry proposed in Ref. 8 of a Corbino disk with Bose glass contacts
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No-slip boundary conditions for the displacement yield a stress of the form given in Eq. (2.12), but with the plus sign inside the square bracket replaced by a minus sign. In this case the stress is largest (in magnitude) at the inner and outer rims of the disk and vanishes in the interior. Plastic slip will occur first at the rims, and then propagate towards the interior of the disk as the current is increased. No-slip boundary conditions are relevant for the experimental geometry proposed in Ref. 8 of a Corbino disk with Bose glass contacts.
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27
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85038277533
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The same symbol y is used here for the fugacity and below for the separation of a neutral pair of dislocations along the climb direction. There should be no confusion as the meaning of y will be clear from the context
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The same symbol y is used here for the fugacity and below for the separation of a neutral pair of dislocations along the climb direction. There should be no confusion as the meaning of y will be clear from the context.
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28
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85038266480
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We have neglected the force arising from Peierls barriers to glide motion due to the periodicity of the lattice. In the Langevin equation for the separation of the dislocation pair in the glide direction considered below, this force only couples to gradients of the external stress
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We have neglected the force arising from Peierls barriers to glide motion due to the periodicity of the lattice. In the Langevin equation for the separation of the dislocation pair in the glide direction considered below, this force only couples to gradients of the external stress.
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30
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85038317107
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Taking into account the angular part of the dislocation interaction only changes the numerical coefficient of the (formula presented) term in the expression for the saddle point
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Taking into account the angular part of the dislocation interaction only changes the numerical coefficient of the (formula presented) term in the expression for the saddle point.
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32
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4243065217
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V. Ambegaokar, B. I. Halperin, D. R. Nelson, and E. D. Siggia, Phys. Rev. Lett. 40, 783 (1978).
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(1978)
Phys. Rev. Lett.
, vol.40
, pp. 783
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Ambegaokar, V.1
Halperin, B.I.2
Nelson, D.R.3
Siggia, E.D.4
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