329 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
Analysis of plasma instabilities and verification of the BOUT code for the Large Plasma Device
The properties of linear instabilities in the Large Plasma Device [W.
Gekelman et al., Rev. Sci. Inst., 62, 2875 (1991)] are studied both through
analytic calculations and solving numerically a system of linearized
collisional plasma fluid equations using the 3D fluid code BOUT [M. Umansky et
al., Contrib. Plasma Phys. 180, 887 (2009)], which has been successfully
modified to treat cylindrical geometry. Instability drive from plasma pressure
gradients and flows is considered, focusing on resistive drift waves, the
Kelvin-Helmholtz and rotational interchange instabilities. A general linear
dispersion relation for partially ionized collisional plasmas including these
modes is derived and analyzed. For LAPD relevant profiles including strongly
driven flows it is found that all three modes can have comparable growth rates
and frequencies. Detailed comparison with solutions of the analytic dispersion
relation demonstrates that BOUT accurately reproduces all characteristics of
linear modes in this system.Comment: Published in Physics of Plasmas, 17, 102107 (2010
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
Influence of point defects on magnetic vortex structures
We employed micro-Hall magnetometry and micromagnetic simulations to
investigate magnetic vortex pinning at single point defects in individual
submicron-sized permalloy disks. Small ferromagnetic particles containing
artificial point defects can be fabricated by using an image reversal electron
beam lithography process. Corresponding micromagnetic calculations, modeling
the defects within the disks as holes, give reasonable agreement between
experimental and simulated pinning and depinning field values
Energy dynamics in a simulation of LAPD turbulence
Energy dynamics calculations in a 3D fluid simulation of drift wave
turbulence in the linear Large Plasma Device (LAPD) [W. Gekelman et al., Rev.
Sci. Inst. 62, 2875 (1991)] illuminate processes that drive and dissipate the
turbulence. These calculations reveal that a nonlinear instability dominates
the injection of energy into the turbulence by overtaking the linear drift wave
instability that dominates when fluctuations about the equilibrium are small.
The nonlinear instability drives flute-like () density
fluctuations using free energy from the background density gradient. Through
nonlinear axial wavenumber transfer to fluctuations, the
nonlinear instability accesses the adiabatic response, which provides the
requisite energy transfer channel from density to potential fluctuations as
well as the phase shift that causes instability. The turbulence characteristics
in the simulations agree remarkably well with experiment. When the nonlinear
instability is artificially removed from the system through suppressing
modes, the turbulence develops a coherent frequency spectrum
which is inconsistent with experimental data
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