428 research outputs found
Spinon-holon interactions in an anisotropic t-J chain: a comprehensive study
We consider a generalization of the one-dimensional t-J model with
anisotropic spin-spin interactions. We show that the anisotropy leads to an
effective attractive interaction between the spinon and holon excitations,
resulting in a localized bound state. Detailed quantitative analytic
predictions for the dependence of the binding energy on the anisotropy are
presented, and verified by precise numerical simulations. The binding energy is
found to interpolate smoothly between a finite value in the t-Jz limit and zero
in the isotropic limit, going to zero exponentially in the vicinity of the
latter. We identify changes in spinon dispersion as the primary factor for this
non-trivial behavior.Comment: 12 pages, 13 figures, long story. The short story is
cond-mat/0702213. Published versio
Binding of holons and spinons in the one-dimensional anisotropic t-J model
We study the binding of a holon and a spinon in the one-dimensional
anisotropic t-J model using a Bethe-Salpeter equation approach, exact
diagonalization, and density matrix renormalization group methods on chains of
up to 128 sites. We find that holon-spinon binding changes dramatically as a
function of anisotropy parameter \alpha=J_\perp/J_z: it evolves from an exactly
deducible impurity-like result in the Ising limit to an exponentially shallow
bound state near the isotropic case. A remarkable agreement between the theory
and numerical results suggests that such a change is controlled by the
corresponding evolution of the spinon energy spectrum.Comment: 4 pages, 5 figures, published versio
Acoustic instability of a circular vortex with a smoothed vorticity profile
It is known that a localized vortex can have two specific mechanisms of
interaction with the ambient flow. The first mechanism is associated with
acoustic radiation, which is accompanied by a loss of energy and causes
instability in the case of negative energy of vortex disturbances. The second
is a Miles mechanism of interaction of the vortex core oscillations with
disturbances in the vicinity of the critical layer (where the phase velocity of
the disturbances coincides with the velocity of the mean flow), accompanied by
an energy flux from the critical layer vicinity, which leads to damping in the
case of negative energy of the oscillations. For the first time, the flow with
both of these mechanisms is considered. The problem is solved from the first
principles. It is shown that the Miles mechanism can completely suppress
acoustic instability, however, in the case of a stronger loss of energy due to
acoustic radiation, acoustic instability will dominate. The role of various
parameters is analyzed and a quantitative criterion for the acoustic
instability of a vortex with a smoothed vorticity profile is obtained
4-(5-Amino-1H-1,2,4-triazol-3-yl)pyridinium chloride monohydrate
In the cation of the title compound, C7H8N5
+·Cl−·H2O, the mean planes of the pyridine and 1,2,4-triazole rings form a dihedral angle of 2.3 (1)°. The N atom of the amino group adopts a trigonal–pyramidal configuration. The N atom of the pyridine ring is protonated, forming a chloride salt. In the crystal, intermolecular N—H⋯O, N—H⋯N, N—H⋯Cl and O—H⋯Cl hydrogen bonds link the cations, anions and water molecules into layers parallel to the (1, 0, ) plane
8He Spectroscopy in Stopped Pion Absorption By 9Be
Level structure of 8He has been studied in the reaction of stopped pion absorption by 9Be nuclei. The missing mass spectrum in the range 0 MeV ≤ MM ≤ 10 MeV has been described by the superposition of phase-space distributions and the three states of 8He. Parameters of these states have been compared with data of other experimental and theoretical works
Spectroscopy of Helium Isotope 6He
The excited states of heavy helium isotope 6He were studied in stopped pion absorption in the reactions 9Be
Quantum vs. Geometric Disorder in a Two-Dimensional Heisenberg Antiferromagnet
We present a numerical study of the spin-1/2 bilayer Heisenberg
antiferromagnet with random interlayer dimer dilution. From the temperature
dependence of the uniform susceptibility and a scaling analysis of the spin
correlation length we deduce the ground state phase diagram as a function of
nonmagnetic impurity concentration p and bilayer coupling g. At the site
percolation threshold, there exists a multicritical point at small but nonzero
bilayer coupling g_m = 0.15(3). The magnetic properties of the single-layer
material La_2Cu_{1-p}(Zn,Mg)_pO_4 near the percolation threshold appear to be
controlled by the proximity to this new quantum critical point.Comment: minor changes, updated figure
Range of the t--J model parameters for CuO plane: experimental data constraints
The t-J model effective hopping integral is determined from the three-band
Hubbard model for the charge carriers in CuO plane. For this purpose the
values of the superexchange constant and the charge-transfer gap
are calculated in the framework of the three-band model. Fitting values of
and to the experimental data allows to narrow the uncertainty region
of the three-band model parameters. As a result, the ratio of the t-J
model is fixed in the range for holes and for
electrons. Formation of the Frenkel exciton is justified and the main features
of the charge-transfer spectrum are correctly described in the framework of
this approach.Comment: 20pp., REVTEX 3.0, (11 figures), report 66
Low energy states with different symmetries in the t-J model with two holes on a 32-site lattice
We study the low energy states of the t-J model with two holes on a 32-site
lattice with periodic boundary conditions. In contrary to common belief, we
find that the state with d_{x^2-y^2} symmetry is not always the ground state in
the realistic parameter range 0.2\le J/t\le 0.4. There exist low-lying
finite-momentum p-states whose energies are lower than the d_{x^2-y^2} state
when J/t is small enough. We compare various properties of these low energy
states at J/t=0.3 where they are almost degenerate, and find that those
properties associated with the holes (such as the hole-hole correlation and the
electron momentum distribution function) are very different between the
d_{x^2-y^2} and p states, while their spin properties are very similar.
Finally, we demonstrate that by adding ``realistic'' terms to the t-J model
Hamiltonian, we can easily destroy the d_{x^2-y^2} ground state. This casts
doubt on the robustness of the d_{x^2-y^2} state as the ground state in a
microscopic model for the high temperature superconductors
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