128 research outputs found
Magnetooptical effects in quantum wells irradiated with light pulses
The method of detection and investigation of the magnetopolaron effect in the
semiconductor quantum wells (QW) in a strong magnetic field, based on pulse
light irradiation and measuring the reflected and transmitted pulses, has been
proposed. It has been shown that a beating amplitude on the frequencies,
corresponding to the magnetopolaron energy level splitting, depends strongly
from the exciting pulse width. The existence of the time points of the total
reflection and total transparency has been predicted. The high orders of the
perturbation theory on electron-electromagnetic field interaction have been
taken into account.Comment: 5 pages, 5 figures with captions, corrected typos, figures are
reedeted to improve their quality in accordance with the Referee requirement;
Phys. Rev. B, Brief Reports, submitted for publicatio
Bipolarons in the Extended Holstein Hubbard Model
We numerically and analytically calculate the properties of the bipolaron in
an extended Hubbard Holstein model, which has a longer range electron-phonon
coupling like the Fr\" ohlich model. In the strong coupling regime, the
effective mass of the bipolaron in the extended model is much smaller than the
Holstein bipolaron mass. In contrast to the Holstein bipolaron, the bipolaron
in the extended model has a lower binding energy and remains bound with
substantial binding energy even in the large-U limit. In comparison with the
Holstein model where only a singlet bipolaron is bound, in the extended
Holstein model a triplet bipolaron can also form a bound state. We discuss the
possibility of phase separation in the case of finite electron doping.Comment: 5 pages, 3 figure
The Holstein Polaron
We describe a variational method to solve the Holstein model for an electron
coupled to dynamical, quantum phonons on an infinite lattice. The variational
space can be systematically expanded to achieve high accuracy with modest
computational resources (12-digit accuracy for the 1d polaron energy at
intermediate coupling). We compute ground and low-lying excited state
properties of the model at continuous values of the wavevector in
essentially all parameter regimes. Our results for the polaron energy band,
effective mass and correlation functions compare favorably with those of other
numerical techniques including DMRG, Global Local and exact diagonalization. We
find a phase transition for the first excited state between a bound and unbound
system of a polaron and an additional phonon excitation. The phase transition
is also treated in strong coupling perturbation theory.Comment: 24 pages, 11 figures submitted to PR
Spin-polaron model: transport properties of EuB
To understand anomalous transport properties of EuB, we have studied the
spin-polaron Hamiltonian incorporating the electron-phonon interaction.
Assuming a strong exchange interaction between the carriers and the localized
spins, the electrical conductivity is calculated. The temperature and magnetic
field dependence of the resistivity of EuB are well explained. At low
temperature, magnons dominate the conduction process, whereas the lattice
contribution becomes significant at very high temperature due to the scattering
with the phonons. Large negative magnetoresistance near the ferromagnetic
transition is also reproduced as observed in EuB.Comment: 4 pages, 3 figures, accepted in Phys. Rev.
Semiclassical action based on dynamical mean-field theory describing electrons interacting with local lattice fluctuations
We extend a recently introduced semiclassical approach to calculating the
influence of local lattice fluctuations on electronic properties of metals and
metallic molecular crystals. The effective action of electrons in degenerate
orbital states coupling to Jahn-Teller distortions is derived, employing
dynamical mean-field theory and adiabatic expansions. We improve on previous
numerical treatments of the semiclassical action and present for the
simplifying Holstein model results for the finite temperature optical
conductivity at electron-phonon coupling strengths from weak to strong.
Significant transfer of spectral weight from high to low frequencies is
obtained on isotope substitution in the Fermi-liquid to polaron crossover
regime.Comment: 10 pages, 7 figure
Indications of coherence-incoherence crossover in layered transport
For many layered metals the temperature dependence of the interlayer
resistance has a different behavior than the intralayer resistance. In order to
better understand interlayer transport we consider a concrete model which
exhibits this behavior. A small polaron model is used to illustrate how the
interlayer transport is related to the coherence of quasi-particles within the
layers. Explicit results are given for the electron spectral function,
interlayer optical conductivity and the interlayer magnetoresistance. All these
quantities have two contributions: one coherent (dominant at low temperatures)
and one incoherent (dominant at high temperatures).Comment: 6 pages, 4 figures, REVTEX
Holstein model in infinite dimensions at half-filling
The normal state of the Holstein model is studied at half-filling in infinite
dimensions and in the adiabatic regime. The dynamical mean-field equations are
solved using perturbation expansions around the extremal paths of the effective
action for the atoms. We find that the Migdal-Eliashberg expansion breaks down
in the metallic state if the electron-phonon coupling exceeds a value
of about 1.3 in spite of the fact that the formal expansion parameter ( is the phonon frequency, the Fermi energy) is
much smaller than 1. The breakdown is due to the appearance of more than one
extremal path of the action. We present numerical results which illustrate in
detail the evolution of the local Green's function, the self-energy and the
effective atomic potential as a function of .Comment: Revtex + 17 postscript figures include
Critical fluctuation conductivity in layered superconductors in strong electric field
The paraconductivity, originating from critical superconducting
order-parameter fluctuations in the vicinity of the critical temperature in a
layered superconductor is calculated in the frame of the self-consistent
Hartree approximation, for an arbitrarily strong electric field and zero
magnetic field. The paraconductivity diverges less steep towards the critical
temperature in the Hartree approximation than in the Gaussian one and it shows
a distinctly enhanced variation with the electric field. Our results indicate
that high electric fields can be effectively used to suppress order-parameter
fluctuations in high-temperature superconductors.Comment: 11 pages, 2 figures, to be published in Phys. Rev.
Electron self-trapping in intermediate-valent SmB6
SmB6 exhibits intermediate valence in the ground state and unusual behaviour
at low temperatures. The resistivity and the Hall effect cannot be explained
either by conventional sf-hybridization or by hopping transport in an impurity
band. At least three different energy scales determine three temperature
regimes of electron transport in this system. We consider the ground state
properties, the soft valence fluctuations and the spectrum of band carriers in
n-doped SmB6. The behaviour of excess conduction electrons in the presence of
soft valence fluctuations and the origin of the three energy scales in the
spectrum of elementary excitations is discussed. The carriers which determine
the low-temperature transport in this system are self-trapped electron-polaron
complexes rather than simply electrons in an impurity band. The mechanism of
electron trapping is the interaction with soft valence fluctuations.Comment: 12 pages, 3 figure
Band-filling effects on electron-phonon properties of normal and superconducting state
We address the effect of band filling on the effective electron mass
and the superconducting critical temperature in a electron-phonon system.
We compare the vertex corrected theory with the non-crossing approximation of
the Holstein model within a local approximation. We identify two regions of the
electron density where and are enhanced or decreased by the
inclusion of the vertex diagrams. We show that the crossover between the
enhancement at low density and the decrease towards half filling is almost
independent of the microscopic electron-phonon parameters. These different
behaviors are explained in terms of the net sign of the vertex diagrams which
is positive at low densities and negative close to half filling. Predictions of
the present theory for doped MgB, which is argued to be in the low density
regime, are discussed.Comment: 13 revtex pages, figures eps include
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