2002
DOI: 10.1103/physrevb.66.153318
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Reentrant melting of soliton lattice phase in a bilayer quantum Hall system

Abstract: At large parallel magnetic field B , the ground state of bilayer quantum Hall system forms uniform soliton lattice phase. The soliton lattice will melt due to the proliferation of unbound dislocations at certain finite temperature leading to the Kosterlitz-Thouless (KT) melting. We calculate the KT phase boundary by numerically solving the newly developed set of Bethe ansatz equations, which fully take into account the thermal fluctuations of soliton walls. We predict that within certain ranges of B , the soli… Show more

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Cited by 7 publications
(3 citation statements)
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“…[105]. It is also related to previous work on quantum Hall bilayer systems [106,107,108,109,110], with the important difference that the boundary conditions in the present case are dx ∂ x φ = 0, while in Refs. [107,65,105] (amongst numerous others), there is no such restriction on φ.…”
Section: Actionsupporting
confidence: 52%
“…[105]. It is also related to previous work on quantum Hall bilayer systems [106,107,108,109,110], with the important difference that the boundary conditions in the present case are dx ∂ x φ = 0, while in Refs. [107,65,105] (amongst numerous others), there is no such restriction on φ.…”
Section: Actionsupporting
confidence: 52%
“…More accurate pictures of this commensurate-incommensurate ͑C-IC͒ phase transition have suggested the existence of a domain structure of pseudospins in the IC phase, which is called a soliton-lattice ͑SL͒ phase. 2,[9][10][11][12][13][14][15] In the SL phase, domains of the commensurate phase are separated by a pseudospin soliton, in which the pseudospin slips by 2 around a magnetic flux penetrating between the two layers. An important feature of the SL is that its translational symmetry is broken by the introduction of periodic kinks of pseudospins.…”
mentioning
confidence: 99%
“…Since the SL spontaneously breaks the translational symmetry of the two-dimensional system, the KT transition is expected to appear. 9,13,15 When the temperature is higher than a critical temperature, the SL is expected to melt into a randomly distributed array because of unbound dislocations. While the melting of the lattice is suggested to be detected by an abrupt increase in R xx , 13,15 the temperature dependence of R xx ͓inset of Fig.…”
mentioning
confidence: 99%