Finite-momentum condensate of magnetic excitons in a bilayer quantum Hall system


Autoria(s): Doretto, R. L.; Smith, C. Morais; Caldeira, A. O.
Contribuinte(s)

Universidade Estadual Paulista (UNESP)

Data(s)

30/09/2013

20/05/2014

30/09/2013

20/05/2014

26/07/2012

Resumo

Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)

Processo FAPESP: 10/00479-6

Processo FAPESP: 07/57630-5

We study the bilayer quantum Hall system at total filling factor nu(T) = 1 within a bosonization formalism which allows us to approximately treat the magnetic exciton as a boson. We show that in the region where the distance between the two layers is comparable to the magnetic length, the ground state of the system can be seen as a finite-momentum condensate of magnetic excitons provided that the excitation spectrum is gapped. We analyze the stability of such a phase within the Bogoliubov approximation first assuming that only one momentum Q is macroscopically occupied and later we consider the same situation for two modes +/- Q. We find strong evidences that a first-order quantum phase transition at small interlayer separation takes place from a zero-momentum condensate phase, which corresponds to Halperin 111 state, to a finite-momentum condensate of magnetic excitons.

Formato

17

Identificador

http://dx.doi.org/10.1103/PhysRevB.86.035326

Physical Review B. College Pk: Amer Physical Soc, v. 86, n. 3, p. 17, 2012.

1098-0121

http://hdl.handle.net/11449/24652

10.1103/PhysRevB.86.035326

WOS:000306924000003

WOS000306924000003.pdf

Idioma(s)

eng

Publicador

Amer Physical Soc

Relação

Physical Review B

Direitos

closedAccess

Tipo

info:eu-repo/semantics/article