2003
DOI: 10.1103/physrevlett.91.046804
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Conductivity of Paired Composite Fermions

Abstract: We develop a phenomenological description of the nu=5/2 quantum Hall state in which the Halperin-Lee-Read theory of the half-filled Landau level is combined with a p-wave pairing interaction between composite fermions (CFs). The electromagnetic response functions for the resulting mean-field superconducting state of the CFs are calculated and used in an RPA calculation of the q and omega dependent longitudinal conductivity of the physical electrons, a quantity which can be measured experimentally.

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Cited by 5 publications
(4 citation statements)
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“…The MR state has been studied in great detail [8][9][10][11] and interpreted by two complementary 12 pictures: as a Laughlin state of tightly bound electron pairs 13,14 or a superfluid of weakly bound CF pairs. [15][16][17] The first numerical calculations for interacting electrons in a partially filled LL 1 were carried out by Morf. 18 They seemed to confirm that a half-filled LL 1 has a spin-polarized incompressible ground state accurately described by the MR wave function.…”
Section: Introductionmentioning
confidence: 99%
“…The MR state has been studied in great detail [8][9][10][11] and interpreted by two complementary 12 pictures: as a Laughlin state of tightly bound electron pairs 13,14 or a superfluid of weakly bound CF pairs. [15][16][17] The first numerical calculations for interacting electrons in a partially filled LL 1 were carried out by Morf. 18 They seemed to confirm that a half-filled LL 1 has a spin-polarized incompressible ground state accurately described by the MR wave function.…”
Section: Introductionmentioning
confidence: 99%
“…Exactly at ν = 5/2, if we treat the CS gauge field at mean-field level, the electrons form a Fermi sea of composite fermions in zero net field [7]. Following the lead of previous studies [12], we add an explicit p−wave attraction between the composite fermions (which in a more complete treatment should properly be derived by integrating out high energy degrees of freedom in some fashion). At T = 0, a further BCS mean-field decoupling of this attraction produces a p + ip superconducting state with coherence length ξ and a gap to creating Bogoliubov quasiparticles ('Bogolons') ∆ = v F /ξ.…”
mentioning
confidence: 99%
“…Excitations in this superconductor are vortices carrying half a flux quantum and an electric charge of e /4, and fermions created in twos by breaking pairs with an appropriate energy gap. 2,3 The Bogoliubov-de Gennes ͑BdG͒ equation describing the fermionic excitations of a twodimensional ͑2D͒ p-wave superconductor admits zero-energy solutions in the presence of well-separated vortices, one solution near each vortex' core; these solutions are Majorana fermions ␥, satisfying ␥ † = ␥. As a consequence, the ground state is degenerate; for 2N well-separated vortices, the ground state degeneracy is 2 N .…”
mentioning
confidence: 99%