3,825 research outputs found
Antiferromagnetism in two-dimensional t-J model: pseudospin representation
We discuss a pseudospin representation of the two-dimensional t-J model. We
introduce pseudospins associated with empty sites, deriving a new
representation of the t-J model that consists of local spins and spinless
fermions. We show, within a mean-field approximation, that our representation
of t-J model corresponds to the {\it isotropic} antiferromagnetic Heisenberg
model in an effective magnetic field. The strength and the direction of the
effective field are determined by the hole doping and the
orientation of pseudospins associated with empty sites, respectively. We find
that the staggered magnetization in the standard representation corresponds to
the component of magnetization perpendicular to the effective field in our
pseudospin representation. Using a many-body Green's function method, we show
that the staggered magnetization decreases with increasing hole doping
and disappears at for . Our
results are in good agreement with experiments and numerical calculations in
contradistinction to usual mean-field methods.Comment: 6 pages, 3 figure
grc4f v1.0: a Four-fermion Event Generator for e+e- Collisions
grc4f is a Monte-Carlo package for generating e+e- to 4-fermion processes in
the standard model. All of the 76 LEP-2 allowed fermionic final state processes
evaluated at tree level are included in version 1.0. grc4f addresses event
simulation requirements at e+e- colliders such as LEP and up-coming linear
colliders. Most of the attractive aspects of grc4f come from its link to the
GRACE system: a Feynman diagram automatic computation system. The GRACE system
has been used to produce the computational code for all final states, giving a
higher level of confidence in the calculation correctness. Based on the
helicity amplitude calculation technique, all fermion masses can be kept finite
and helicity information can be propagated down to the final state particles.
The phase space integration of the matrix element gives the total and
differential cross sections, then unweighted events are Generated. Initial
state radiation (ISR) corrections are implemented in two ways, one is based on
the electron structure function formalism and the second uses the parton shower
algorithm called QEDPS. The latter can also be applied for final state
radiation (FSR) though the interference with the ISR is not yet taken into
account. Parton shower and hadronization of the final quarks are performed
through an interface to JETSET. Coulomb correction between two intermediate
W's, anomalous coupling as well as gluon contributions in the hadronic
processes are also included.Comment: 30 pages, LaTeX, 5 pages postscript figures, uuencode
Test of CDF dijet anomaly within the standard model
Dijet anomaly reported by the CDF (Collider Detector at Fermilab)
collaboration in 1.96 TeV p-pbar collisions is investigated within the standard
model by considering effects of parton distribution functions on various
processes: W+dijet, Z+dijet, WW, ZW, and top production. Since the anomalous
peak exists in the dijet-mass region of 140 GeV with the p-pbar center-of-mass
energy sqrt{s}=1.96 TeV, a relevant momentum fraction x of partons is roughly
0.1. In this x region, recent HERMES semi-inclusive charged-lepton scattering
experiment indicated that the strange-quark distribution could be very
different from a conventional one, which has been used for many years, based on
opposite-sign dimuon measurements in neutrino-induced deep inelastic
scattering. We investigated effects of such variations in the strange-quark
distribution s(x) on the anomaly. We found that distributions of W+dijets and
other process are affected by the strange-quark modifications in wide
dijet-mass regions including the 140 GeV one. Since the CDF anomaly was
observed in the shoulder region of the dijet-mass distribution, a slight
modification of the distribution shape could explain at least partially the CDF
excess. Therefore, it is important to consider such effects within the standard
model for judging whether the CDF anomaly indicates new physics beyond the
standard model. We also show modification effects of the strange-quark
distribution in the LHC (Large Hadron Collider) kinematics, where cross
sections are sensitive to a smaller-x region of s(x).Comment: 11 pages, LaTeX, submitted for publicatio
GR@PPA 2.7 event generator for / collisions
The GR@PPA event generator has been updated to version 2.7. This distribution
provides event generators for ( or ) + jets ( 4 jets), +
jets ( 2 jets) and QCD multi-jet ( 4 jets) production processes at
and collisions, in addition to the four bottom quark
productions implemented in our previous work (GR@PPA\_4b). Also included are
the top-pair and top-pair + jet production processes, where the correlation
between the decay products are fully reproduced at the tree level. Namely,
processes up to seven-body productions can be simulated, based on ordinary
Feynman diagram calculations at the tree level. In this version, the GR@PPA
framework and the process dependent matrix-element routines are separately
provided. This makes it easier to add further new processes, and allows users
to make a choice of processes to implement. This version also has several new
features to handle complicated multi-body production processes. A systematic
way to combine many subprocesses to a single base-subprocess has been
introduced, and a new method has been adopted to calculate the color factors of
complicated QCD processes. They speed up the calculation significantly.Comment: 21 pages, no figur
The scaling properties of dissipation in incompressible isotropic three-dimensional magnetohydrodynamic turbulence
The statistical properties of the dissipation process constrain the analysis
of large scale numerical simulations of three dimensional incompressible
magnetohydrodynamic (MHD) turbulence, such as those of Biskamp and Muller
[Phys. Plasmas 7, 4889 (2000)]. The structure functions of the turbulent flow
are expected to display statistical self-similarity, but the relatively low
Reynolds numbers attainable by direct numerical simulation, combined with the
finite size of the system, make this difficult to measure directly. However, it
is known that extended self-similarity, which constrains the ratio of scaling
exponents of structure functions of different orders, is well satisfied. This
implies the extension of physical scaling arguments beyond the inertial range
into the dissipation range. The present work focuses on the scaling properties
of the dissipation process itself. This provides an important consistency check
in that we find that the ratio of dissipation structure function exponents is
that predicted by the She and Leveque [Phys. Rev. Lett 72, 336 (1994)] theory
proposed by Biskamp and Muller. This supplies further evidence that the cascade
mechanism in three dimensional MHD turbulence is non-linear random eddy
scrambling, with the level of intermittency determined by dissipation through
the formation of current sheets.Comment: 9 pages, 6 figures. Figures embedded in text. Typos corrected in text
and references. Published in Physics of Plasmas. Abstract can be found
at:http://link.aip.org/link/?php/12/02230
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