1,815 research outputs found
Hybridization-induced superconductivity from the electron repulsion on a tetramer lattice having a disconnected Fermi surface
Plaquette lattices with each unit cell containing multiple atoms are good
candidates for disconnected Fermi surfaces, which are shown by Kuroki and Arita
to be favorable for spin-flucutation mediated superconductivity from electron
repulsion. Here we find an interesting example in a tetramer lattice where the
structure within each unit cell dominates the nodal structure of the gap
function. We trace its reason to the way in which a Cooper pair is formed
across the hybridized molecular orbitals, where we still end up with a T_c much
higher than usual.Comment: 4 pages, 6 figure
Effect of the Vortices on the Nuclear Spin Relaxation Rate in the Unconventional Pairing States of the Organic Superconductor (TMTSF)PF
This Letter theoretically discusses quasiparticle states and nuclear spin
relaxation rates in a quasi-one-dimensional superconductor
(TMTSF)PF under a magnetic field applied parallel to the conduction
chains. We study the effects of Josephson-type vortices on by
solving the Bogoliubov de Gennes equation for -, - or -wave pairing
interactions. In the presence of line nodes in pairing functions, is
proportional to in sufficiently low temperatures because quasiparticles
induced by vortices at the Fermi energy relax spins. We also try to identify
the pairing symmetry of (TMTSF)PF.Comment: 4+ pages, 4 figure
A Mechanism of Spin-Triplet Superconductivity in Hubbard Model on Triangular La ttice: Application to UNi_2Al_3
We discuss the possibility of spin-triplet superconductivity in a
two-dimensional Hubbard model on a triangular lattice within the third-order
perturbation theory. When we vary the symmetry in the dispersion of the bare
energy band from D_2 to D_6, spin-singlet superconductivity in the
D_2-symmetric system is suppressed and we obtain spin-triplet superconductivity
in near the D_6-symmetric system. In this case, it is found that the vertex
terms, which are not included in the interaction mediated by the spin
fluctuation, are essential for realizing the spin-triplet pairing. We point out
the possibility that obtained results correspond to the difference between the
superconductivity of UNi_2Al_3 and that of UPd_2Al_3.Comment: 11pages, 5figure
Superconductivity from a long-range interaction: a crossover between the electron gas and the lattice model
We explore how the superconductivity arising from the on-site
electron-electron repulsion will change when the repulsion is changed to a
long-ranged, 1/r-like one by introducing an extended Hubbard model with the
repulsion extending to distant (12th) neighbors. With a simplified
fluctuation-exchange approximation, we have found for the square lattice that
(i) as the band filling becomes dilute enough, the charge susceptibility
becomes comparable with the spin susceptibility, where p and then s pairings
become dominant, in agreement with the result for the electron gas by Takada,
while (ii) the d-wave, which reflects the lattice structure, dominates well
away from the half filling. All these can be understood in terms of the spin
and charge structures along with the shape and size of the Fermi surface.Comment: 5 pages, 6 figure
Electronic structure and spontaneous internal field around non-magnetic impurities in spin-triplet chiral p-wave superconductors
The electronic structure around an impurity in spin triplet p-wave
superconductors is studied by the Bogoliubov-de Gennes theory on a
tight-binding model, where we have chosen -wave
or -wave states which are
considered to be candidates for the pairing state in SrRuO.
We calculate the spontaneous current and the local density of states around
the impurity and discuss the difference between the two types of pairing.
We propose that it is possible to discriminate the two pairing states by
studying the spatial dependence of the magnetic field around a pair of
impurities.Comment: 4 pages, 4 figure
Dynamical Generation of Non-Abelian Gauge Group via the Improved Perturbation Theory
It was suggested that the massive Yang-Mills-Chern-Simons matrix model has
three phases and that in one of them a non-Abelian gauge symmetry is
dynamically generated. The analysis was at the one-loop level around a
classical solution of fuzzy sphere type. We obtain evidences that three phases
are indeed realized as nonperturbative vacua by using the improved perturbation
theory. It also gives a good example that even if we start from a trivial
vacuum, the improved perturbation theory around it enables us to observe
nontrivial vacua.Comment: 31 pages, published versio
Electronic states and pairing symmetry in the two-dimensional 16 band d-p model for iron-based superconductor
The electronic states of the FeAs plane in iron-based superconductors are
investigated on the basis of the two-dimensional 16-band d-p model, where the
tight-binding parameters are determined so as to fit the band structure
obtained by the density functional calculation for LaFeAsO. The model includes
the Coulomb interaction on a Fe site: the intra- and inter-orbital direct terms
U and U', the exchange coupling J and the pair-transfer J'. Within the random
phase approximation (RPA), we discuss the pairing symmetry of possible
superconducting states including s-wave and d-wave pairing on the U'-J plane.Comment: 2 pages, 4 figures; Proceedings of the Int. Symposium on
Fe-Oxipnictide Superconductors (Tokyo, 28-29th June 2008
Analysis of Superconductivity in d-p Model on Basis of Perturbation Theory
We investigate the mass enhancement factor and the superconducting transition
temperature in the d-p model for the high-\Tc cuprates. We solve the
\'Eliashberg equation using the third-order perturbation theory with respect to
the on-site Coulomb repulsion . We find that when the energy difference
between d-level and p-level is large, the mass enhancement factor becomes large
and \Tc tends to be suppressed owing to the difference of the density of
state for d-electron at the Fermi level. From another view point, when the
energy difference is large, the d-hole number approaches to unity and the
electron correlation becomes strong and enhances the effective mass. This
behavior for the electron number is the same as that of the f-electron number
in the heavy fermion systems. The mass enhancement factor plays an essential
role in understanding the difference of \Tc between the LSCO and YBCO
systems.Comment: 4pages, 9figures, to be published in J. Phys. Soc. Jp
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