2,167 research outputs found
Double Exchange Ferromagnetism in the Peierls Insulator State
We study the effects of opening of the band gap on the double exchange
ferromagnetism. Applying the density-matrix renormalization group method and an
analytical expansion from the dimer limit to the one-dimensional double
exchange model, we demonstrate for a relevant region of the exchange coupling
that, in the weak dimerization regime, the Peierls gap opens in the fully
spin-polarized conduction band without affecting its ferromagnetism, whereas in
the strong dimerization regime, the ferromagnetism is destroyed and the Mott
gap opens instead, leading the system to the antiferromagnetic quasi-long-range
order. An insulator version of the double exchange ferromagnetism is thus
established.Comment: 5 pages, 3 figures, Phys. Rev. Lett., in pres
Anomalous impurity effect on magnetization in frustrated one-dimensional ferro- and ferrimagnets
Significant decrease of spontaneous magnetization in frustrated
one-dimensional ferro- and ferrimagnets due to non-magnetic impurities is
predicted. Using the density-matrix renormalization group method and the exact
diagonalization method, we confirm that the total spin can vanish due to a
single impurity in finite chains. Introducing the picture of magnetic domain
inversion, we numerically investigate the impurity-density dependence of
magnetization. In particular, we show that even with an infinitesimal density
of impurities the magnetization in the ground state is reduced by about 40%
from that of the corresponding pure system. Conditions for the materials which
may show this anomalous impurity effect are formulated.Comment: 4 pages, 6 figure
Quantum-classical transition in the Caldeira-Leggett model
The quantum-classical transition in the Caldeira-Leggett model is
investigated in the framework of the functional renormalization group method.
It is shown that a divergent quadratic term arises in the action due to the
heat bath in the model. By removing the divergence with a frequency cutoff we
considered the critical behavior of the model. The critical exponents belonging
to the susceptibility and the correlation length are determined and their
independence of the frequency cutoff and the renormalization scheme is shown.Comment: 8 pages, 4 figure
Quantum Disordered Ground States in Frustrated Antiferromagnets with Multiple Ring Exchange Interactions
We present a certain class of two-dimensional frustrated quantum Heisenberg
spin systems with multiple ring exchange interactions which are rigorously
demonstrated to have quantum disordered ground states without magnetic
long-range order. The systems considered in this paper are s=1/2
antiferromagnets on a honeycomb and square lattices, and an s=1 antiferromagnet
on a triangular lattice. We find that for a particular set of parameter values,
the ground state is a short-range resonating valence bond state or a valence
bond crystal state. It is shown that these systems are closely related to the
quantum dimer model introduced by Rokhsar and Kivelson as an effective
low-energy theory for valence bond states.Comment: 6 pages, 4 figure
Low density ferromagnetism in the Hubbard model
A single-band Hubbard model with nearest and next-nearest neighbour hopping
is studied for , 2, 3, using both analytical and numerical techniques. In
one dimension, saturated ferromagnetism is found above a critical value of
for a band structure with two minima and for small and intermediate densities.
This is an extension of a scenario recently proposed by M\"uller--Hartmann. For
three dimensions and non-pathological band structures, it is proven that such a
scenario does not work.Comment: 4 pages, 3 postscript figure
Optimal T of cuprates: role of screening and reservoir layers
We explore the role of charge reservoir layers (CRLs) on the superconducting
transition temperature of cuprate superconductors. Specifically, we study the
effect of CRLs with efficient short distance dielectric screening coupled
capacitively to copper oxide metallic layers. We argue that dielectric
screening at short distances and at frequencies of the order of the
superconducting gap, but small compared to the Fermi energy can significantly
enhance T, the transition temperature of an unconventional superconductor.
We discuss the relevance of our qualitative arguments to a broader class of
unconventional superconductors.Comment: 8 Pages, 4 figure
Effects of antiferromagnetic planes on the superconducting properties of multilayered high-Tc cuprates
We propose a mechanism for high critical temperature (T_c) in the coexistent
phase of superconducting- (SC) and antiferromagnetic (AF) CuO_2 planes in
multilayered cuprates. The Josephson coupling between the SC planes separated
by an AF insulator (Mott insulator) is calculated perturbatively up to the
fourth order in terms of the hopping integral between adjacent CuO_2 planes. It
is shown that the AF exchange splitting in the AF plane suppresses the
so-called pi-Josephson coupling, and the long-ranged 0-Josephson coupling leads
to coexistence with a rather high value of T_c.Comment: 4 pages including 4 figure
Resonating singlet valence plaquettes
We consider the simplest generalizations of the valence bond physics of SU(2)
singlets to SU(N) singlets that comprise objects with N sites -- these are
SU(N) singlet plaquettes with N=3 and N=4 in three spatial dimensions.
Specifically, we search for a quantum mechanical liquid of such objects -- a
resonating singlet valence plaquette phase that generalizes the celebrated
resonating valence bond phase for SU(2) spins. We extend the Rokhsar-Kivelson
construction of the quantum dimer model to the simplest SU(4) model for valence
plaquette dynamics on a cubic lattice. The phase diagram of the resulting
quantum plaquette model is analyzed both analytically and numerically. We find
that the ground state is solid everywhere, including at the Rokhsar-Kivelson
point where the ground state is an equal amplitude sum. By contrast, the equal
amplitude sum of SU(3) singlet triangular plaquettes on the face centered cubic
lattice is liquid and thus a candidate for describing a resonating single
valence plaquette phase, given a suitably defined local Hamiltonian.Comment: 12 pages, 15 figures, minor changes, references added, Phys Rev B
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