2005
DOI: 10.1142/s0217979205028797
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Inverse Melting of Vortex Lattice in Layered Superconductors

Abstract: Using molecular dynamic simulations for the melting transition of a flux line lattice(FLL) with point disordered pinnings, thermal fluctuations and magnetic interactions between pancake vortices, we study the disorder-driven melting transition from a disentangled and ordered Bragg glass (BG) to an entangled amorphous vortex glass (VG) or a vortex liquid (VL) in the pinning strength-temperature phase diagram. A portion of the BG region is found to be sandwiched in between the VG phase at lower temperatures and … Show more

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Cited by 3 publications
(3 citation statements)
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“…Another example is given by the phenomenon of reentrant phase transitions [146][147][148][149], where the macroscopic 'ordered' phase has higher entropy than the microscopic 'disordered' one because of the unfreezing of certain DOF. Irreversible microscopic dynamics, such as diffusive motion, does not conserve the number of accessible microstates of the system conditioned by the macroscopic constraints and, thus, lead to an increase of entropy [144,145].…”
Section: Electromagnetic Fields In the Brainmentioning
confidence: 99%
“…Another example is given by the phenomenon of reentrant phase transitions [146][147][148][149], where the macroscopic 'ordered' phase has higher entropy than the microscopic 'disordered' one because of the unfreezing of certain DOF. Irreversible microscopic dynamics, such as diffusive motion, does not conserve the number of accessible microstates of the system conditioned by the macroscopic constraints and, thus, lead to an increase of entropy [144,145].…”
Section: Electromagnetic Fields In the Brainmentioning
confidence: 99%
“…In agreement with the third law of thermodynamics, for example, this takes place at T = 0, where there is only one accessible microstate and the system is maximally ordered on the microscopic level. Another example is given by the phenomenon of re-entrant phase transitions [149][150][151][152], where the macroscopic 'ordered' phase has a higher entropy than the microscopic 'disordered' one because of the unfreezing of certain DOF.…”
Section: Ficationmentioning
confidence: 99%
“…In agreement with the third law of thermodynamics, for example, this takes place at , where there is only one accessible microstate and the system is maximally ordered on the microscopic level. Another example is given by the phenomenon of re-entrant phase transitions [ 149 , 150 , 151 , 152 ], where the macroscopic ‘ordered’ phase has a higher entropy than the microscopic ‘disordered’ one because of the unfreezing of certain DOF. Irreversible microscopic dynamics, such as diffusive motion, does not conserve the number of accessible microstates of the system conditioned by the macroscopic constraints and thus leads to an increase in entropy [ 147 , 148 ].…”
Section: Schrödinger’s ‘Order From Order’ and Jordan’s Quantum Amplif...mentioning
confidence: 99%