176 research outputs found
Scattering of Bunched Fractionally Charged Quasiparticles
The charge of fractionally charged quasiparticles, proposed by Laughlin to
explain the fractional quantum Hall effect (FQHE), was recently verified by
measurements. Charge q=e/3 and e/5 (e is the electron charge), at filling
factors nu=1/3 and 2/5, respectively, were measured. Here we report the
unexpected bunching of fractional charges, induced by an extremely weak
backscattering potential at exceptionally low electron temperatures (T<10 mK) -
deduced from shot noise measurements. Backscattered charges q=nu e,
specifically, q=e/3, q=2e/5, and q<3e/7, in the respective filling factors,
were measured. For the same settings but at an only slightly higher electron
temperature, the measured backscattered charges were q=e/3, q=e/5, and q=e/7.
In other words, bunching of backscattered quasiparticles is taking place at
sufficiently low temperatures. Moreover, the backscattered current exhibited
distinct temperature dependence that was correlated to the backscattered charge
and the filling factor. This observation suggests the existence of 'low' and
'high' temperature backscattering states, each with its characteristic charge
and characteristic energy.Comment: 4 pages, 3 figure
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
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
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
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
- …