141 research outputs found
Why of (CaFeAs)PtAs is twice as high as (CaFePtAs)PtAs
Recently discovered (CaFePtAs)PtAs and
(CaFeAs)PtAs superconductors are very similar materials
having the same elemental composition and structurally similar superconducting
FeAs slabs. Yet the maximal critical temperature achieved by changing Pt
concentration is approximately twice higher in the latter. Using angle-resolved
photoemission spectroscopy(ARPES) we compare the electronic structure of their
optimally doped compounds and find drastic differences. Our results highlight
the sensitivity of critical temperature to the details of fermiology and point
to the decisive role of band-edge singularities in the mechanism of high-
superconductivity
Superconductivity from repulsion in LiFeAs: novel s-wave symmetry and potential time-reversal symmetry breaking
We analyze the structure of the pairing interaction and superconducting gap
in LiFeAs by decomposing the pairing interaction for various kz cuts into s-
and d-wave components and by studying the leading superconducting
instabilities. We use the ten orbital tight-binding model, derived from
ab-initio LDA calculations with hopping parameters extracted from the fit to
ARPES experiments. We find that the pairing interaction almost decouples
between two subsets, one consists of the outer hole pocket and two electron
pockets, which are quasi-2D and are made largely out of dxy orbital, and the
other consists of the two inner hole pockets, which are quasi-3D and are made
mostly out of dxz and dyz orbitals. Furthermore, the bare inter-pocket and
intra-pocket interactions within each subset are nearly equal. In this
situation, small changes in the intra-pocket and inter-pocket interactions due
to renormalizations by high-energy fermions give rise to a variety of different
gap structures. We find four different configurations of the s-wave gap
immediately below Tc: the one in which superconducting gap changes sign between
two inner hole pockets and between the outer hole pocket and two electron
pockets, the one in which the gap changes sign between two electron pockets and
three hole pockets, the one in which the gap on the outer hole pocket differs
in sign from the gaps on the other four pockets, and the one in which the gaps
on two inner hole pockets have one sign, and the gaps on the outer hole pockets
and on electron pockets have different sign. Different s-wave gap
configurations emerge depending on whether the renormalized interactions
increase attraction within each subset or increase the coupling between
particular components of the two subsets. We argue that the state with opposite
sign of the gaps on the two inner hole pockets has the best overlap with ARPES
data.Comment: 23 pages, 15 figure
Anomalously enhanced photoemission from the Dirac point and symmetry of the self-energy variations for the surface states in Bi2Se3
Accurate analysis of the photoemission intensity from the surface states of
Bi2Se3 reveals two unusual features: spectral line asymmetry and anomalously
enhanced photoemission from the Dirac point. The former indicates a certain
symmetry of a scattering process, which results in strongly k\omega-dependent
contribution to the imaginary part of the self-energy that changes sign while
crossing both the dispersion curves and the energy of the Dirac point. The
latter is hard to describe by one particle spectral function while a final
state interference seems to be plausible explanation
Photoemission induced gating of topological insulator
The recently discovered topological insulators exhibit topologically
protected metallic surface states which are interesting from the fundamental
point of view and could be useful for various applications if an appropriate
electronic gating can be realized. Our photoemission study of Cu intercalated
Bi2Se3 shows that the surface states occupancy in this material can be tuned by
changing the photon energy and understood as a photoemission induced gating
effect. Our finding provides an effective tool to investigate the new physics
coming from the topological surface states and suggests the intercalation as a
recipe for synthesis of the material suitable for electronic applications.Comment: + resistivity data and some discussio
Resistivity and Hall effect of LiFeAs: Evidence for electron-electron scattering
LiFeAs is unique among the broad family of FeAs-based superconductors,
because it is superconducting with a rather large K under
ambient conditions although it is a stoichiometric compound. We studied the
electrical transport on a high-quality single crystal. The resistivity shows
quadratic temperature dependence at low temperature giving evidence for strong
electron-electron scattering and a tendency towards saturation around room
temperature. The Hall constant is negative and changes with temperature, what
most probably arises from a van Hove singularity close to the Fermi energy in
one of the hole-like bands. Using band structure calculations based on angular
resolved photoemission spectra we are able to reproduce all the basic features
of both the resistivity as well as the Hall effect data.Comment: 6 pages, 3 figures included; V2 has been considerably revised and
contain a more detailed analysis of the Hall effect dat
Interaction-induced singular Fermi surface in a high-temperature oxypnictide superconductor
In the family of iron-based superconductors, LaFeAsO-type materials possess
the simplest electronic structure due to their pronounced two-dimensionality.
And yet they host superconductivity with the highest transition temperature
Tc=55K. Early theoretical predictions of their electronic structure revealed
multiple large circular portions of the Fermi surface with a very good
geometrical overlap (nesting), believed to enhance the pairing interaction and
thus superconductivity. The prevalence of such large circular features in the
Fermi surface has since been associated with many other iron-based compounds
and has grown to be generally accepted in the field. In this work we show that
a prototypical compound of the 1111-type, SmFe0.92Co0.08AsO, is at odds with
this description and possesses a distinctly different Fermi surface, which
consists of two singular constructs formed by the edges of several bands,
pulled to the Fermi level from the depths of the theoretically predicted band
structure by strong electronic interactions. Such singularities dramatically
affect the low-energy electronic properties of the material, including
superconductivity. We further argue that occurrence of these singularities
correlates with the maximum superconducting transition temperature attainable
in each material class over the entire family of iron-based superconductors.Comment: Open access article available online at
http://www.nature.com/srep/2015/150521/srep10392/full/srep10392.htm
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