453 research outputs found
Screening effects in the electron-optical phonon interaction
We show that recently reported unusual hardening of optical phonons
renormalized by the electron-phonon interaction is due to the neglect of
screening effects. When the electron-ion interaction is properly screened
optical phonons soften in three dimension. It is important that for
short-wavelength optical phonons screening is static while for long-wavelength
optical phonons screening is dynamic. In two-dimensional and one-dimensional
cases due to crossing of the nonperturbed optical mode with gapless plasmons
the spectrum of renormalized optical phonon-plasmon mode shows split momentum
dependence.Comment: 7 page
Electron energy relaxation by phonons in the Kondo condensate
We have used normal metal-insulator-superconductor tunnel junctions as
thermometers at sub-Kelvin temperatures to study the electron-phonon (e-p)
interaction in thin Aluminum films doped with Manganese, as a function of
Manganese concentration. Mn in Al is known to be a Kondo impurity with
extremely high Kondo temperature 500 K, thus our results probe the
e-p coupling in the fully spin compensated, unitary limit. The temperature
dependence of the e-p interaction is consistent with the existing theory for
disordered metals, however full theory including the Kondo effect has not been
worked out yet. The strength of the interaction decreases with increasing
Manganese concentration, providing a means to improve sensitivity of detectors
and efficiency of solid state coolers
Comment on "Giant Nernst Effect due to Fluctuating Cooper Pairs in Superconductors" by M.N. Serbyn, M.A. Skvortsov, A.A. Varlamov, and V. Galitski
In a recent Letter, Serbyn et al. [A] investigated thermomagnetic effects
above the superconducting transition and generalized previous works for
arbitrary magnetic fields and temperatures. While the results of [A] have been
confirmed in [B], we have strong objections: (i) According to our results [C],
the linear response calculation does not require any correction from the
magnetization currents; (ii) The result of [A,B] is giant, because unlike the
normal Fermi liquid, it is of zero order in the particle-hole asymmetry.
Changing the interaction constant in the Cooper channel leads to ridiculously
large results even for nonsuperconducting metals; (iii)Derived in [A] the
Einstein-type relation for thermomagnetic coefficient contradicts to text-book
results.
[A] M.N. Serbyn, M.A. Skvortsov, A.A. Varlamov, V. Galitski, Phys. Rev. Lett.
102, 067001 (2009).
[B] K. Michaeli and A.M. Finkel'stein, EPL 86, 27007 (2009).
[C] A. Sergeev et al., Phys. Rev. B 77, 064501 (2008)
Coherent description of electrical and thermal impurity-and-phonon limited transport in simple metals
The electrical resistivity, thermoelectric power and electronic thermal
conductivity of simple (isotropic) metals are studied in a uniform way.
Starting from results of a variational solution of the Boltzmann equation, a
generalized Matthiessen rule is used in order to superpose the inelastic (or
not) electron-phonon and elastic electron-impurity scattering cross sections
("matrix elements"). The temperature dependence relative to these processes is
given through simple functions and physical parameters over the usually
investigated range of temperature for each transport coefficient. The coherence
of such results is emphasized.Comment: 22 pages, 5 figures; to appear in International Journal of Modern
Physics
Coulomb blockade in quantum dots under AC pumping
We study conductance through a quantum dot under Coulomb blockade conditions
in the presence of an external periodic perturbation. The stationary state is
determined by the balance between the heating of the dot electrons by the
perturbation and cooling. We analyze two cooling mechanisms: electron exchange
with the cold contacts and emission of phonons. Together with the usual linear
Ohmic heating of the dot electrons we consider possible effects of dynamic
localization. The combination of the abovementioned factors may result in a
drastic change of the shape of the Coulomb blockade peak with respect to the
usual equilibrium one.Comment: 12 pages, 8 figure
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