2008/09/30 by V. V. Ponomarenko, Vadim V. Ponomarenko, D. V. Averin +1
Physics and Astronomy · #Physics of Superconductivity and Magnetism #Quantum and electron transport phenomena #Semiconductor Quantum Structures and Devices #cond-mat.mes-hall #cond-mat.str-el
paper · pdf · doi:10.1103/physrevb.79.045303
published as Phys. Rev. B 79, 045303 (2009) · fourteen two-column pages in RevTex4, 4 eps figure, extended final verson as appeared in PRB
openalex publication_date 2009/01/06 · arxiv created 2010/05/09 · arxiv updated 2010/05/11 · openalex created_date 2016/06/24 · openalex updated_date 2026/07/30
We have studied theoretically the tunneling between two edges of quantum Hall liquids of different filling factors, \ensuremathν0,1=1/(2m0,1+1), with m0\ensuremath≥m1\ensuremath≥0, through two separate point contacts in the geometry of Mach-Zehnder interferometer [Ji et al., Nature (London) 422, 415 (2003); Neder et al., Phys. Rev. Lett. 96, 016804 (2006)]. The quasiparticle formulation of the interferometer model is derived as a dual to the initial electron model in the limit of strong electron tunneling reached at large voltages or temperatures. For m\ensuremath≡1+m0+m1>1, the tunneling of quasiparticles of fractional charge e/m leads to nontrivial m-state dynamics of effective flux through the interferometer, which restores the regular ``electron'' periodicity of the current in flux despite the fractional charge and statistics of quasiparticles. The exact solution available for equal times of propagation between the contacts along the two edges demonstrates that the interference pattern of modulation of the tunneling current by flux depends on voltage and temperature only through a common amplitude.