1,363 research outputs found
Abelian deterministic self organized criticality model: Complex dynamics of avalanche waves
The aim of this study is to investigate a wave dynamics and size scaling of
avalanches which were created by the mathematical model {[}J. \v{C}ern\'ak
Phys. Rev. E \textbf{65}, 046141 (2002)]. Numerical simulations were carried
out on a two dimensional lattice in which two constant thresholds
and were randomly distributed. A density
of sites with the threshold and threshold are
parameters of the model. I have determined autocorrelations of avalanche size
waves, Hurst exponents, avalanche structures and avalanche size moments for
several densities and thresholds . I found correlated avalanche
size waves and multifractal scaling of avalanche sizes not only for specific
conditions, densities , 1.0 and thresholds , in
which relaxation rules were precisely balanced, but also for more general
conditions, densities and thresholds $8\leq E_{c}^{II}\leq3 in
which relaxation rules were unbalanced. The results suggest that the hypothesis
of a precise relaxation balance could be a specific case of a more general
rule
Reduced nonlinear description of Farley-Buneman instability
In the study on nonlinear wave-wave processes in an ionosphere and a
magnetosphere usually the main attention is paid to investigation of plasma
turbulence at well developed stage, when the wide spectrum of plasma wave is
present. On the other side, it is well known that even if the number of
cooperating waves remains small due to a competition of processes of their
instability and attenuation, the turbulence appears in the result of their
stochastic behavior. The regimes of nonlinear dynamics of low frequency waves
excited due to Farley-Buneman instability in weakly ionized and inhomogeneous
ionospheric plasma in the presence of electric current perpendicular to ambient
magnetic field are considered. The problem is essentially three dimensional and
difficult for full numerical simulation, but the strong collisional damping of
waves allow to assume that in this case a perturbed state of plasma can be
described as finite set of interacting waves, some of which are unstable and
other strongly damping. The proposed nonlinear model allow to make full study
of nonlinear stabilization, conditions of stochasticity and to consider the
different regimes and properties of few mode plasma turbulence.Comment: The extended version of work, published in AIP Conf. Proc. 993, 113
(2008
Renormalized mean-field t-J model of high-Tc superconductivity: comparison with experiment
Using an advanced version of the renormalized mean-field theory (RMFT) for
the t-J model, we examine spin-singlet superconducting (SC) state of -symmetry. Overall doping dependence of the SC gap magnitude is in good
agreement with experimental results for (BSCCO) and
(LSCO) compounds at the
optimal doping and in the overdoped regime. We also calculate the dispersion
relation for the Bogoliubov quasiparticles and compare our findings both with
the angle resolved photoemission data for the cuprates, as well as with the
variational Monte Carlo and other mean-field studies. Within the method
proposed by Fukushima [cf. Phys. Rev. B \textbf{78}, 115105 (2008)], we analyze
different forms of the t-J Hamiltonian, i.e. modifications caused by the form
of exchange interaction, and by the presence of three-site terms. It is shown
that although the former has a small influence, the latter suppresses strongly
the superconductivity. We also analyze the temperature dependence of the gap
magnitude and compare the results with those of the recently introduced
finite-temperature renormalized mean-field theory (TRMFT) of Wang et al. [cf.
Phys. Rev. B \textbf{82}, 125105 (2010)].Comment: 7 pages, 6 figures, 2 tables. Submitted to Physical Review
Exotic and excited-state radiative transitions in charmonium from lattice QCD
We compute, for the first time using lattice QCD methods, radiative
transition rates involving excited charmonium states, states of high spin and
exotics. Utilizing a large basis of interpolating fields we are able to project
out various excited state contributions to three-point correlators computed on
quenched anisotropic lattices. In the first lattice QCD calculation of the
exotic 1-+ eta_c1 radiative decay, we find a large partial width Gamma(eta_c1
-> J/psi gamma) ~ 100 keV. We find clear signals for electric dipole and
magnetic quadrupole transition form factors in chi_c2 -> J/psi gamma,
calculated for the first time in this framework, and study transitions
involving excited psi and chi_c1,2 states. We calculate hindered magnetic
dipole transition widths without the sensitivity to assumptions made in model
studies and find statistically significant signals, including a non-exotic
vector hybrid candidate Y_hyb? -> eta_c gamma. As well as comparison to
experimental data, we discuss in some detail the phenomenology suggested by our
results and the extent to which it mirrors that of quark potential models and
make suggestions for the interpretation of our results involving exotic quantum
numbered states
Who Are The Difficult Employees? Psychopathological Attributions Of Their Co-workers
On a given workday, over 700 workers are attacked, 43,800 employees are harassed and 16,400 are threatened (Hynes, 2001). Yet the literature focuses upon environmental causes; none attempt to identify personal characteristics of the uncivil, deviant or maladaptive employee. This study helps fill this void by exploring the personality correlates of uncivil employee behavior. These employees violate mutual norms of respect, negatively affect organizational performance, and are thus the prototypical difficult employee. Utilizing a unique psycho-pathological approach, the DSM-IV (Diagnostic Statistical Manual) was used as the basis for defining and assessing the perceived personality correlates of these employees’ behaviors. Results suggest that narcissistic traits are the modal descriptors for the Difficult Employee, regardless of hierarchical role (boss, peer, subordinate). Implications are discussed with suggestions for future research
N-(2,5-Dichlorophenyl)maleamic acid
The asymmetric unit of the title compound, C10H7Cl2NO3, contains two independent molecules. The molecular conformation of each maleamic unit is stabilized by an intramolecular O—H⋯Ocarbonyl hydrogen bond owing to the anti disposition of the participating entities. The mean planes through the benzene ring and the amido group are inclined at angles of 45.7 (1) and 40.8 (1)° in the two molecules. In the crystal, the independent molecules self-associate via N—H⋯O hydrogen bonds into zigzag ribbons propagating along the a axis. The ribbons are weakly coupled by C—H⋯π and C—H⋯O interactions
4-Chloro-N-(3,5-dimethylphenyl)benzamide
In the molecular structure of the title compound, C15H14ClNO, the amide group forms dihedral angles of 15.8 (2) and 27.2 (2)°, respectively, with the benzoyl and aniline rings, while the angle between the benzoyl and aniline rings is 11.5 (1)°. The crystal structure is stabilized by N—H⋯O hydrogen bonds, which give rise to infinite chains running along the c axis
3-Chloro-N-(2-methylphenyl)benzamide
In the molecular structure of the title compound, C14H12ClNO, the meta-Cl atom in the benzoyl ring is positioned anti to the C=O bond, while the ortho-methyl group in the aniline ring is positioned syn to the N—H bond. The two benzene rings are nearly coplanar [dihedral angle = 3.48 (5)°]. The crystal structure is stabilized by N—H⋯O hydrogen bonds, which link the molecules into chains along the b axis
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