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Revista mexicana de física
versão impressa ISSN 0035-001X
Rev. mex. fis. vol.53 supl.2 México Fev. 2007
Noncommutative field theory approach to the fractional quantum Hall effect with the filling factor onehalf
Sendic EstradaJiménez and Hugo GarcíaCompeán
Departamento de Física Centro de Investigación y de Estudios Avanzados del IPN Apdo. Postal 14740, 07000, México D.F., México
Recibido el 18 de julio de 2005
Aceptado el 14 de marzo de 2005
Abstract
The fractional quantum Hall effect is studied in the context of the noncommutative quantum field theory in (2+1) dimensions. For the filling factor v = 1/2, the noncommutative effective field theory incorporates a ChernSimons gauge field (in the temporal gauge) coupled to the matter in the presence of a suitable quenched external magnetic field. After providing the Feynman rules for this system, the noncommutative corrections to the selfenergy of quasiparticles are computed, showing that it is zero at HartreeFock approximation. Finally, in this approach it is proved that the density ρ satisfies a noncommutative deformation of the w∞algebra.
Keywords: Noncommutative field theory; fractional quantum Hall effect; ChernSimons theory.
Resumen
El efecto Hall cuántico fraccionario se estudia en el contexto de la teoría cuántica de campos no conmutativa en (2+1) dimensiones. Para el factor de llenado v = 1/2, la teoría de campos efectiva incorpora un campo de norma de ChernSimons (en la norma temporal) acoplado a la materia en la presencia de un campo magnético externo apropiadamente cancelado. Después de dar las reglas de Feynman para este sistema, las correcciones no conmutativas de la autoenegía de las cuasipartículas son calculadas y se muestra que son cero en la aproximación de HartreeFock. Finalmente, en este enfoque se prueba que la densidad ρ satisface una deformación no conmutativa del álgebra w∞.
Descriptores: Teoría de campos no conmutativa; efecto Hall cuántico fraccionario; teoría de ChernSimons.
PACS: 11.10.Nx;73.43.Lp; 11.10.Gh
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Acknowledgments
This work was supported in part by a CONACyT México grant No. 33951E. The work of S.E.J. is supported by a CONACyT graduate fellowship. S. EstradaJiménez whishes to thank Prof. YongShi Wu for useful discussions and suggestions concerning the subject of this paper and for his kind hospitality at the University of Utah, where part of this work was outlined.
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