4,262 research outputs found
Dipole anisotropies of IRAS galaxies and the contribution of a large-scale local void
Recent observations of dipole anisotropies show that the velocity of the
Local Group (\Vec v_{\rm G}) induced by the clustering of IRAS galax ies has
an amplitude and direction similar to those of the velocity of Cosmic Microwave
Background dipole anisotropy (\Vec v_{\rm CMB}), but the difference | \Vec
v_{\rm G} - \Vec v_{\rm CMB} | is still km/s, which is about 28% of
|\Vec v_{\rm CMB} |. Here we consider the possibility that the origin of this
difference comes from a hypothetical large-scale local void, with which we can
account for the accelerating behavior of type Ia supernovae due to the spatial
inhomogeneity of the Hubble constant without dark energies and derive the
constraint to the model parameters of the local void. It is found as a result
that the distance between the Local Group and the center of the void must be
Mpc, whose accurate value depends on the background model
parameters.Comment: 13 pages, 1 figure, to be published in ApJ 584, No.2 (2003
Photometric Observations of Star Formation Activity in Early Type Spirals
We observationally study the current star formation activities of early type
spiral galaxies. We construct a complete sample of 15 early type spirals having
far-infrared (FIR) to optical B band luminosity ratios, L(FIR)/L(B), larger
than the average of the type, and make their CCD imaging of the R and H-alpha
bands. The equivalent widths of H-alpha emission increase with increasing
L(FIR)/L(B), indicating that L(FIR)/L(B) can be an indicator of star formation
for such early type spirals with star formation activities higher than the
average. For all of the observed early type spirals, the extended HII regions
exist at the central regions with some asymmetric features. H-alpha emission is
more concentrated to the galactic center than the R band light, and the degree
of the concentration increases with the star formation activity. We also
analyze the relation between the star formation activities and the existence of
companion galaxies in the sample galaxies and other bright early type spirals.
No correlation is found and this suggests that the interaction is not
responsible for all of the star formation activities of early type spirals.Comment: LaTex, 23 pages (2 tables included), plus 9 Postscript figures & 1
table. To be published in AJ (November issue
Finite-size Scaling of Correlation Ratio and Generalized Scheme for the Probability-Changing Cluster Algorithm
We study the finite-size scaling (FSS) property of the correlation ratio, the
ratio of the correlation functions with different distances. It is shown that
the correlation ratio is a good estimator to determine the critical point of
the second-order transition using the FSS analysis. The correlation ratio is
especially useful for the analysis of the Kosterlitz-Thouless (KT) transition.
We also present a generalized scheme of the probability-changing cluster
algorithm, which has been recently developed by the present authors, based on
the FSS property of the correlation ratio. We investigate the two-dimensional
quantum XY model of spin 1/2 with this generalized scheme, obtaining the
precise estimate of the KT transition temperature with less numerical effort.Comment: 4 pages, RevTeX4, to appear in Phys. Rev. B, Rapid Communication
Probability-Changing Cluster Algorithm: Study of Three-Dimensional Ising Model and Percolation Problem
We present a detailed description of the idea and procedure for the newly
proposed Monte Carlo algorithm of tuning the critical point automatically,
which is called the probability-changing cluster (PCC) algorithm [Y. Tomita and
Y. Okabe, Phys. Rev. Lett. {\bf 86} (2001) 572]. Using the PCC algorithm, we
investigate the three-dimensional Ising model and the bond percolation problem.
We employ a refined finite-size scaling analysis to make estimates of critical
point and exponents. With much less efforts, we obtain the results which are
consistent with the previous calculations. We argue several directions for the
application of the PCC algorithm.Comment: 6 pages including 8 eps figures, to appear in J. Phys. Soc. Jp
Quantitative Evaluation of Solidification Brittleness of Weld Metal during Solidification by In-situ Observation and Measurement (Report V) : Correlation between Critical Strain Rate and Critical Deformation Rate Required for Solidification Crack Initiation(Materials, Metallugy & Weldability)
Renormalization Group Approach to Einstein Equation in Cosmology
The renormalization group method has been adapted to the analysis of the
long-time behavior of non-linear partial differential equation and has
demonstrated its power in the study of critical phenomena of gravitational
collapse. In the present work we apply the renormalization group to the
Einstein equation in cosmology and carry out detailed analysis of
renormalization group flow in the vicinity of the scale invariant fixed point
in the spherically symmetric and inhomogeneous dust filled universe model.Comment: 16 pages including 2 eps figures, RevTe
Critical property of spin-glass transition in a bond-disordered classical antiferromagnetic Heisenberg model with a biquadratic interaction
Motivated by puzzling spin-glass behaviors observed in many pyrochlore-based
magnets, effects of magnetoelastic coupling to local lattice distortions were
recently studied by the authors for a bond-disordered antiferromagnet on a
pyrochlore lattice [Phys. Rev. Lett. 107, 047204 (2011)]. Here, we extend the
analyses with focusing on the critical property of the spin-glass transition
which occurs concomitantly with a nematic transition. Finite-size scaling
analyses are performed up to a larger system size with 8192 spins to estimate
the transition temperature and critical exponents. The exponents are compared
with those in the absence of the magnetoelastic coupling and with those for the
canonical spin-glass systems. We also discuss the temperature dependence of the
specific heat in comparison with that in canonical spin-glass systems as well
as an experimental result.Comment: 4 pages, 2 figures, proceedings for LT2
Perturbative Corrections to the Ohta-Jasnow-Kawasaki Theory of Phase-Ordering Dynamics
A perturbation expansion is considered about the Ohta-Jasnow-Kawasaki theory
of phase-ordering dynamics; the non-linear terms neglected in the OJK
calculation are reinstated and treated as a perturbation to the linearised
equation. The first order correction term to the pair correlation function is
calculated in the large-d limit and found to be of order 1/(d^2).Comment: Revtex, 27 pages including 2 figures, submitted to Phys. Rev. E,
references adde
Analytical solution of thermal magnetization on memory stabilizer structures
We return to the question of how the choice of stabilizer generators affects
the preservation of information on structures whose degenerate ground state
encodes a classical redundancy code. Controlled-not gates are used to transform
the stabilizer Hamiltonian into a Hamiltonian consisting of uncoupled single
spins and/or pairs of spins. This transformation allows us to obtain an
analytical partition function and derive closed form equations for the relative
magnetization and susceptibility. These equations are in agreement with the
numerical results presented in [arXiv:0907.0394v1] for finite size systems.
Analytical solutions show that there is no finite critical temperature, Tc=0,
for all of the memory structures in the thermodynamic limit. This is in
contrast to the previously predicted finite critical temperatures based on
extrapolation. The mismatch is a result of the infinite system being a poor
approximation even for astronomically large finite size systems, where
spontaneous magnetization still arises below an apparent finite critical
temperature. We extend our analysis to the canonical stabilizer Hamiltonian.
Interestingly, Hamiltonians with two-body interactions have a higher apparent
critical temperature than the many-body Hamiltonian.Comment: 13 pages, 7 figures, analytical solutions of problems studied
numerically in arXiv:0907.0394v1 [quant-ph
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