28 research outputs found
Frictional magnetodrag between spatially separated two-dimensional electron systems: Coulomb versus phonon mediated electron-electron interaction
We study the frictional drag due to Coulomb and phonon mediated
electron-electron interaction in a double layer electron system exposed to a
perpendicular magnetic field. Within the random phase approximation we
calculate the dispersion relation of the intra Landau level magnetoplasmons at
finite temperatures and distinguish their contribution to the magnetodrag. We
calculate the transresistivity as a function of magnetic field
, temperature , and interlayer spacing for a matched electron
density. For nm we find that is solely due to
phonon exchange and shows no double-peak structure as a function of . For
nm, shows the double-peak structure and is mainly
due to Coulomb interaction. The value of is about 0.3
at T=2 K and for the half-filled second Lanadau level, which is about 13 times
larger than the value for nm. At lower edge of the temperature
interval from 0.1 to 8 K, remains finite for
nm while it tends to zero for nm. Near the upper edge of this
interval, for nm is approximately linear in
while for nm it decreases slowly in . Therefore, the peak of
is very sharp for nm. This strikingly
different magnetic field and temperature dependence of ascribe we
mainly to the weak screening effect at large interlayer separations.Comment: replaced with revised versio
Coulomb drag of Luttinger liquids and quantum-Hall edges
We study the transconductance for two coupled one-dimensional wires or edge
states described by Luttinger liquid models. The wires are assumed to interact
over a finite segment. We find for the interaction parameter that the
drag rate is finite at zero temperature, which cannot occur in a Fermi-liquid
system. The zero temperature drag is, however, cut off at low temperature due
to the finite length of the wires. We also consider edge states in the
fractional quantum Hall regime, and we suggest that the low temperature
enhancement of the drag effect might be seen in the fractional quantum Hall
regime.Comment: 5 pages, 2 figures; to appear in Phys. Rev. Let
Semiclassical theory of electron drag in strong magnetic fields
We present a semiclassical theory for electron drag between two parallel
two-dimensional electron systems in a strong magnetic field, which provides a
transparent picture of the most salient qualitative features of anomalous drag
phenomena observed in recent experiments, especially the striking sign reversal
of drag at mismatched densities. The sign of the drag is determined by the
curvature of the effective dispersion relation obeyed by the drift motion of
the electrons in a smooth disorder potential. Localization plays a role in
explaining activated low temperature behavior, but is not crucial for anomalous
drag per se.Comment: 10 page
Phonon drag in ballistic quantum wires
The acoustic phonon-mediated drag-contribution to the drag current created in
the ballistic transport regime in a one-dimensional nanowire by phonons
generated by a current-carrying ballistic channel in a nearby nanowire is
calculated. The threshold of the phonon-mediated drag current with respect to
bias or gate voltage is predicted.Comment: 5 pages, 2 figure
Coulomb Drag for Strongly Localized Electrons: Pumping Mechanism
The mutual influence of two layers with strongly loclized electrons is
exercised through the random Coulomb shifts of site energies in one layer
caused by electron hops in the other layer. We trace how these shifts give rise
to a voltage drop in the passive layer, when a current is passed through the
active layer. We find that the microscopic origin of drag lies in the time
correlations of the occupation numbers of the sites involved in a hop. These
correlations are neglected within the conventional Miller-Abrahams scheme for
calculating the hopping resistance.Comment: 5 pages, 3 figure
Frictional Coulomb drag in strong magnetic fields
A treatment of frictional Coulomb drag between two 2-dimensional electron
layers in a strong perpendicular magnetic field, within the independent
electron picture, is presented. Assuming fully resolved Landau levels, the
linear response theory expression for the transresistivity is
evaluated using diagrammatic techniques. The transresistivity is given by an
integral over energy and momentum transfer weighted by the product of the
screened interlayer interaction and the phase-space for scattering events. We
demonstrate, by a numerical analysis of the transresistivity, that for
well-resolved Landau levels the interplay between these two factors leads to
characteristic features in both the magnetic field- and the temperature
dependence of . Numerical results are compared with recent
experiments.Comment: RevTeX, 34 pages, 8 figures included in tex
Coulomb Drag in the Extreme Quantum Limit
Coulomb drag resulting from interlayer electron-electron scattering in double
layer 2D electron systems at high magnetic field has been measured. Within the
lowest Landau level the observed drag resistance exceeds its zero magnetic
value by factors of typically 1000. At half-filling of the lowest Landau level
in each layer (nu = 1/2) the data suggest that our bilayer systems are much
more strongly correlated than recent theoretical models based on perturbatively
coupled composite fermion metals.Comment: 4 pages, 4 figure
Frictional Drag between Two Dilute Two-Dimensional Hole Layers
We report drag measurements on dilute double layer two-dimensional hole
systems in the regime of r_s=19~39. We observed a strong enhancement of the
drag over the simple Boltzmann calculations of Coulomb interaction, and
deviations from the T^2 dependence which cannot be explained by
phonon-mediated, plasmon-enhanced, or disorder-related processes. We suggest
that this deviation results from interaction effects in the dilute regime.Comment: 4 pages, 3 figures, accepted in Phys. Rev. Lett. Added single layer
transport dat
Phonon mediated drag in double layer two dimensional electron systems
Experiments studying phonon mediated drag in the double layer two dimensional
electron gas system are reported. Detailed measurements of the dependence of
drag on temperature, layer spacing, density ratio, and matched density are
discussed. Comparisons are made to theoretical results [M. C. Bonsager et al.,
Phys. Rev. B 57, 7085 (1998)] which propose the existence of a new coupled
electron-phonon collective mode. The layer spacing and density dependence at
matched densities for samples with layer spacings below 2600 A do not support
the existence of this mode, showing behavior expected for independent electron
and phonon systems. The magnitude of the drag, however, suggests the alternate
limit; one in which electrons and phonons are strongly coupled. The results for
still larger layer spacing show significant discrepancies with the behavior
expected for either limit.Comment: 9 pages, 9 figures, Late
Coulomb Drag at the Onset of Anderson Insulators
It is shown that the Coulomb drag between two identical layers in the
Anderson insulting state indicates a striking difference between the Mott and
Efros-Shklovskii (ES) insulators. In the former, the trans-resistance
is monotonically increasing with the localization length ; in the latter,
the presence of a Coulomb gap leads to an opposite result: is enhanced
with a decreasing , with the same exponential factor as the single layer
resistivity. This distinction reflects the relatively pronounced role of
excited density fluctuations in the ES state, implied by the enhancement in the
rate of hopping processes at low frequencies. The magnitude of drag is
estimated for typical experimental parameters in the different cases. It is
concluded that a measurement of drag can be used to distinguish between
interacting and non-interacting insulating state.Comment: 15 pages, revte