60 research outputs found
Phase Evolution in a Kondo Correlated System
The coherence and phase evolution of electrons in a mesoscopic system in the
Kondo correlated regime were studied. The Kondo effect, in turn, is one of the
most fundamental many-body effects where a localized spin interacts with
conduction electrons in a conductor. Results were obtained by embedding a
quantum dot (QD) in a double path electronic interferometer and measuring
interference of electron waves. The Phase was found to evolve in a range twice
as large as the theoretically predicted one. Moreover, the phase proved to be
highly sensitive to the onset of Kondo correlation, thus serving as a new
fingerprint of the Kondo effect.Comment: 4 pages, 4 figures. typos corrected. Changed to APS PRL styl
Entanglement, Dephasing, and Phase Recovery via Cross-Correlation Measurements of Electrons
Determination of the path taken by a quantum particle leads to a suppression
of interference and to a classical behavior. We employ here a quantum 'which
path' detector to perform accurate path determination in a
two-path-electron-interferometer; leading to full suppression of the
interference. Following the dephasing process we recover the interference by
measuring the cross-correlation between the interferometer and detector
currents. Under our measurement conditions every interfering electron is
dephased by approximately a single electron in the detector - leading to mutual
entanglement of approximately single pairs of electrons.Comment: 13 Pages, 5 Figure
Controlled dephasing of a quantum dot in the Kondo regime
Kondo correlation in a spin polarized quantum dot (QD) results from the
dynamical formation of a spin singlet between the dot's net spin and a Kondo
cloud of electrons in the leads, leading to enhanced coherent transport through
the QD. We demonstrate here significant dephasing of such transport by coupling
the QD and its leads to potential fluctuations in a near by 'potential
detector'. The qualitative dephasing is similar to that of a QD in the Coulomb
Blockade regime in spite of the fact that the mechanism of transport is quite
different. A much stronger than expected suppression of coherent transport is
measured, suggesting that dephasing is induced mostly in the 'Kondo cloud' of
electrons within the leads and not in the QD.Comment: to be published in PR
The microscopic nature of localization in the quantum Hall effect
The quantum Hall effect arises from the interplay between localized and
extended states that form when electrons, confined to two dimensions, are
subject to a perpendicular magnetic field. The effect involves exact
quantization of all the electronic transport properties due to particle
localization. In the conventional theory of the quantum Hall effect,
strong-field localization is associated with a single-particle drift motion of
electrons along contours of constant disorder potential. Transport experiments
that probe the extended states in the transition regions between quantum Hall
phases have been used to test both the theory and its implications for quantum
Hall phase transitions. Although several experiments on highly disordered
samples have affirmed the validity of the single-particle picture, other
experiments and some recent theories have found deviations from the predicted
universal behaviour. Here we use a scanning single-electron transistor to probe
the individual localized states, which we find to be strikingly different from
the predictions of single-particle theory. The states are mainly determined by
Coulomb interactions, and appear only when quantization of kinetic energy
limits the screening ability of electrons. We conclude that the quantum Hall
effect has a greater diversity of regimes and phase transitions than predicted
by the single-particle framework. Our experiments suggest a unified picture of
localization in which the single-particle model is valid only in the limit of
strong disorder
The Role of Interactions in an Electronic Fabry-Perot Interferometer Operating in the Quantum Hall Effect Regime
Interference of edge channels is expected to be a prominent tool for studying
statistics of charged quasiparticles in the quantum Hall effect (QHE) [A. Stern
(2008), Ann. Phys. 1:204; C. Chamon et al. (1997), Phys. Rev. B, 55:2331]. We
present here a detailed study of an electronic Fabry-Perot interferometer (FPI)
operating in the QHE regime [C. Chamon et al. (1997), Phys. Rev. B, 55:2331],
with the phase of the interfering quasiparticles controlled by the
Aharonov-Bohm (AB) effect. Our main finding is that Coulomb interactions among
the electrons dominate the interference, even in a relatively large area FPI,
leading to a strong dependence of the area enclosed by the interference loop on
the magnetic field. In particular, for a composite edge structure, with a few
independent edge channels propagating along the edge, interference of the
outmost edge channel (belonging to the lowest Landau level) was insensitive to
magnetic field; suggesting a constant enclosed flux. However, when any of the
inner edge channels interfered, the enclosed flux decreased when the magnetic
field increased. By intentionally varying the enclosed area with a biased
metallic gate and observing the periodicity of the interference pattern,
charges e (for integer filling factors) and e/3 (for a fractional filling
factor) were found to be expelled from the FPI. Moreover, these observations
provided also a novel way of detecting the charge of the interfering
quasiparticles.Comment: 8 pages, 8 figure
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