60 research outputs found
From local to nonlocal Fermi liquid in doped antiferromagnets
The variation of single-particle spectral functions with doping is studied
numerically within the t-J model. It is shown that corresponding self energies
change from local ones at the intermediate doping to strongly nonlocal ones for
a weakly doped antiferromagnet. The nonlocality shows up most clearly in the
pseudogap emerging in the density of states, due to the onset of short-range
antiferromagnetic correlations.Comment: 4 pages, 3 Postscript figures, revtex, submitted to Phys.Rev.Let
Interactions for odd-omega gap singlet superconductors
A class of singlet superconductors with a gap function which is {\it odd} in both momentum and Matsubara frequency was
proposed recently \cite{ba}. To show an instability in the {\it odd} gap
channel, a model phonon propagator was used with the -wave interaction
strength larger than the -wave. We argue that the positive scattering matrix
element entering the Eliashberg equations leads to a constraint on the relative
strength of - and -wave interactions which inhibits odd pairing. However,
a general spin dependent electron-electron interaction can satisfy all
constraints and produce the odd singlet gap. A possibility which may lead to an
odd gap is a strongly antiferromagnetically correlated system, such as a
high- material.Comment: This paper corrects some errors (including the omission of one of the
authors) in the original 9206003 and also a minor error in the published
version, Phys. Rev. B {\bf 47}, 513 (1993). It also contains some comments on
subsequent claims of the impossibility of odd-frequency pairing. Latex fil
Collective Spin Fluctuation Mode and Raman Scattering in Superconducting Cuprates
Although the low frequency electronic Raman response in the superconducting
state of the cuprates can be largely understood in terms of a d-wave energy
gap, a long standing problem has been an explanation for the spectra observed
in the polarization orientations. We present calculations which
suggest that the peak position of the observed spectra is due to a
collective spin fluctuation mode.Comment: 4 pages, 5 eps figure
Charge and spin density wave ordering transitions in strongly correlated metals
We study the quantum transition from a strongly correlated metal, with heavy
fermionic quasiparticles, to a metal with commensurate charge or spin density
wave order. To this end, we introduce and numerically analyze a large
dimensionality model of Ising spins in a transverse field, coupled to two
species of fermions; the analysis borrows heavily from recent progress in the
solution of the Hubbard model in large dimensions. At low energies, the Ising
order parameter fluctuations are characterized by the critical exponent , while above an energy scale, , there is a crossover to criticality. We show that is of the order of the width of the
heavy quasiparticle band, and can be made arbitrarily small for a correlated
metal close to a Mott-Hubbard insulator. Therefore, such a correlated metal has
a significant intermediate energy range of behavior, a single
particle spectrum with a narrow quasiparticle band, and well-formed analogs of
the lower and upper Hubbard bands; we suggest that these features are
intimately related in general.Comment: 14 pages, REVTEX 3.0, 2 postscript figure
Thermodynamic and thermoelectric properties of high-temperature cuprate superconductors in the stripe phase
We examine the thermodynamic and thermoelectric properties in the stripe
phase of high-Tc cuprates, by using the finite-temperature Lanczos technique
for the t-J model with a potential that stabilizes vertical charge stripes.
When the stripe potential is turned on, the entropy is suppressed as a
consequence of the formation of one-dimensional charge stripes accompanied by
an enhancement of antiferromagnetic spin correlation in the spin domains. The
stripe formation leads also to weak temperature dependence of the chemical
potential, leading to the suppression of the thermoelectric power. The
suppression of the entropy and thermoelectric power is consistent with
experimental data in the stripe phase of La_{1.6-x}Nd_{0.4}Sr_xCuO_4.Comment: REVTeX4, 4 pages, 4 figures, to appear in Phys.Rev.B Rapid Comm
Theory for the excitation spectrum of High-T$_c superconductors : quasiparticle dispersion and shadows of the Fermi surface
Using a new method for the solution of the FLEX-equations, which allows the
determination of the self energy of the Hubbard
model on the real frequency axis, we calculate the doping dependence of the
quasi-particle excitations of High-T superconductors. We obtain new results
for the shadows of the Fermi surface, their dependence on the deformation of
the quasi particle dispersion, an anomalous -dependence of and a related violation of the Luttinger theorem.
This sheds new light on the influence of short range magnetic order on the low
energy excitations and its significance for photoemission experiments.Comment: 4 pages (REVTeX) with 3 figure
Spectral functions and pseudogap in the t-J model
We calculate spectral functions within the t-J model as relevant to cuprates
in the regime from low to optimum doping. On the basis of equations of motion
for projected operators an effective spin-fermion coupling is derived. The self
energy due to short-wavelength transverse spin fluctuations is shown to lead to
a modified selfconsistent Born approximation, which can explain strong
asymmetry between hole and electron quasiparticles. The coupling to
long-wavelength longitudinal spin fluctuations governs the low-frequency
behavior and results in a pseudogap behavior, which at low doping effectively
truncates the Fermi surface.Comment: Minor corrections; to appear in Phys. Rev. B (RC
Dynamical Properties of Two Coupled Hubbard Chains at Half-filling
Using grand canonical Quantum Monte Carlo (QMC) simulations combined with
Maximum Entropy analytic continuation, as well as analytical methods, we
examine the one- and two-particle dynamical properties of the Hubbard model on
two coupled chains at half-filling. The one-particle spectral weight function,
, undergoes a qualitative change with interchain hopping
associated with a transition from a four-band insulator to a two-band
insulator. A simple analytical model based on the propagation of exact rung
singlet states gives a good description of the features at large . For
smaller , is similar to that of the
one-dimensional model, with a coherent band of width the effective
antiferromagnetic exchange reasonably well-described by renormalized
spin-wave theory. The coherent band rides on a broad background of width
several times the parallel hopping integral , an incoherent structure
similar to that found in calculations on both the one- and two-dimensional
models. We also present QMC results for the two-particle spin and charge
excitation spectra, and relate their behavior to the rung singlet picture for
large and to the results of spin-wave theory for small .Comment: 9 pages + 10 postscript figures, submitted to Phys.Rev.B, revised
version with isotropic t_perp=t data include
Quantum lattice dynamical effects on the single-particle excitations in 1D Mott and Peierls insulators
As a generic model describing quasi-one-dimensional Mott and Peierls
insulators, we investigate the Holstein-Hubbard model for half-filled bands
using numerical techniques. Combining Lanczos diagonalization with Chebyshev
moment expansion we calculate exactly the photoemission and inverse
photoemission spectra and use these to establish the phase diagram of the
model. While polaronic features emerge only at strong electron-phonon
couplings, pronounced phonon signatures, such as multi-quanta band states, can
be found in the Mott insulating regime as well. In order to corroborate the
Mott to Peierls transition scenario, we determine the spin and charge
excitation gaps by a finite-size scaling analysis based on density-matrix
renormalization group calculations.Comment: 5 pages, 5 figure
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