507 research outputs found
Hopping-resolved electron-phonon coupling in bilayer graphene
In this paper we investigate the electron-phonon coupling in bilayer
graphene, as a paradigmatic case for multilayer graphenes where interlayer
hoppings are relevant. Using a frozen-phonon approach within the context of
Density Functional Theory (DFT) and using different optical phonon
displacements we are able to evaluate quantitatively the electron-phonon
coupling associated with each hopping term . This analysis
also reveals a simple scaling law between the hopping terms and the
electron-phonon coupling which goes beyond the specific DFT
technique employed.Comment: 10 pages, 10 fig
Vertex renormalization in dc conductivity of doped chiral graphene
The remarkable transport properties of graphene follow not only from the the
Dirac-like energy dispersion, but also from the chiral nature of its
excitations, which makes unclear the limits of applicability of the standard
semiclassical Boltzmann approach. In this paper we provide a quantum derivation
of the transport scattering time in graphene in the case of electron-phonon
interaction. By using the Kubo formalism, we compute explicitly the vertex
corrections to the dc conductivity by retaining the full chiral matrix
structure of graphene. We show that at least in the regime of large chemical
potential the Boltzmann picture is justified, and it is also robust against a
small sublattice inequivalence which partly spoils the role of chirality.Comment: (pages late
Interplay of superconductivity with structural phases in a generalized t-J model
The phase diagram of the t-J-V model is discussed using a 1/N expansion in
terms of X operators. It is shown that a flux phase of d-wave symmetry is
stabilized by the Coulomb interaction V at intermediate dopings and competes
with d-wave superconductivity. Since the flux wave instability is stronger than
the superconducting one optimal doping is essentially determined by the onset
of the flux phase. Below optimal doping the flux phase coexists with
superconductivity at low and exists as a pseudo gap phase at higher
temperatures. It is also found that the flux phase boundary is much less
sensitive to impurity scattering than the boundary for superconductivity in
agreement with experiments in Zn doped La-214 and (Y,Ca)-123.Comment: 4 pages, 3 figures, Proceed. M2S-HTSC-VI Housto
Strong-coupling properties of unbalanced Eliashberg superconductors
In this paper we investigate the thermodynamical properties of ``unbalanced''
superconductors, namely, systems where the electron-boson coupling is
different in the self-energy and in the Cooper channels. This situation is
encountered in a variety of situation, as for instance in d-wave
superconductors. Quite interesting is the case where the pairing in the
self-energy is smaller than the one in the gap equation. In this case we
predict a finite critical value where the superconducting critical
temperature diverges but the zero temperature gap is still finite. The
specific heat, magnetic critical field and the penetration depth are also
evaluated.Comment: 9 Revtex pages, 7 eps figures include
Spin susceptibility in small Fermi energy systems: effects of nonmagnetic impurities
In small Fermi energy metals, disorder can deeply modify superconducting
state properties leading to a strong suppression of the critical temperature
. In this paper, we show that also normal state properties can be
seriously influenced by disorder when the Fermi energy is
sufficiently small. We calculate the normal state spin susceptibility
for a narrow band electron-phonon coupled metal as a function of the
non-magnetic impurity scattering rate . We find that as soon
as is comparable to , is strongly reduced
with respect to its value in the clean limit. The effects of the
electron-phonon interaction including the nonadiabatic corrections are
discussed. Our results strongly suggest that the recent finding on irradiated
MgB samples can be naturally explained in terms of small values
associated with the -bands of the boron plane, sustaining therefore the
hypothesis that MgB is a nonadiabatic metal.Comment: 7 pages, 6 eps figures, to appear on Eur. Phys. J.
Interactions and superconductivity in heavily doped MoS2
We analyze the microscopic origin and the physical properties of the
superconducting phase recently observed in MoS. We show how the combination
of the valley structure of the conduction band, the density dependence of the
screening of the long range Coulomb interactions, the short range electronic
repulsion, and the relative weakness of the electron-phonon interactions, makes
possible the existence of a phase where the superconducting order parameter has
opposite signs in different valleys, resembling the superconductivity found in
the pnictides and cuprates
Spectroscopic and thermodynamic properties in a four-band model for pnictides
In this paper we provide a comprehesive analysis of different properties of
pnictides both in the normal and superconducting state, with a particular focus
on the optimally-doped BaKFeAs system. We show that, by
using the band dispersions experimentally measured by ARPES, a four-band
Eliashberg model in the intermediate-coupling regime can account for both the
measured hierarchy of the gaps and for several spectroscopic and thermodynamic
signatures of low-energy renormalization. These include the kinks in the band
dispersion and the effective masses determined via specific-heat and
superfluid-density measurements. We also show that, although an
intermediate-coupling Eliashberg approach is needed to account for the
magnitude of the gaps, the temperature behavior of the thermodynamic quantities
does not show in this regime a significant deviation with respect to
weak-coupling BCS calculations. This can explain the apparent success of
two-band BCS fits of experimental data reported often in the literature.Comment: 12 pages, 6 figures, final versio
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