Remarks on stochastic non-linear birth and death models

The first part of this paper is an attempt to formulate and motivate additional work on the important problem of obtaining global bounds applicable to the controlled truncation of the paper relates specifically to the linear birth, quadratic death model. Asymptotic results are given for the first finite difference ΔT_m where T_m is the exactly known mean time to extinction starting from state m (m= 0,1,…). These results are in terms of the environmental carrying capacity n^* taken to be large. For m near zero ΔT_me^n*/(n^*)²; whereas, for m near n^*ΔT_m ≈ (π/2)^1/2/(n^*)^3/2. This indicates the vastly different time scales in those two regions of state space - with considerably slower action near extinction than near n^*.     

On birth and death processes in symmetric random environment

We prove a limit theorem for a process in a random one-dimensional medium, which has been considered before as a model for hopping conduction in a disordered medium. To the edge between the two integersj and (j+ 1) a rate _j > 0 is attached. These _j :j integral are taken as independent, identically distributed random variables, and represent the medium. For given values _j, X(t) is a Markov chain in continuous time which jumps fromj to (j + 1) and from (j + 1) toj at the same rate _j. We show that in many cases there exists normalizing constants y(t) (which tend to oo witht) such that the distribution of X(t)/(t), or more generally of the whole processX(st)/(t) _S0, converges to a limit as t . The limit process is continuous and self-similar.     

Relaxation mode analysis of nonlinear birth and death processes

Nonlinear birth and death processes with one variable are considered. The general master equations describing these processes are analyzed in terms of their eigenmodes and eigenvalues using the method of a WKB approximation. Formulas for the density of eigenstates are obtained. The lower lying eigenmodes are calculated to investigate long-time relaxation, such as relaxations of metastable and unstable states. Anomalous accumulation of the lower lying eigenvalues is shown to exist when the system is infinitesimally close to a critical or marginal state. The general results obtained are applied to some instructive examples, such as the kinetic Weiss-Ising model and a stochastic model of nonlinear chemical reactions.The work at UCSD was supported in part by the National Science Foundation under Grants MPS72-04363A03 and CHE75-20624.Adapted from the author's Ph.D. dissertation at University of Tokyo, December 1974.     

A note on thermal models

The “thermal models” are discussed in general in thermodynamic context, and then predictions of some hadronisation models are compared to each other and to experimental results at 20+200 GeV/N beam energy.     

A note on the general class of blackbody fractional functions

It is shown how a recent proposal for what was thought to be a new blackbody fractional function is identical with one of the less familiar blackbody fractional functions of old.     

A note on pure bending of a piezoelectric rectangular plate

The problem of pure bending of a piezoelectric rectangular plate is considered in this paper by using the electromagnetic equations of Maxwell and equations of elasticity along with the constitutive equations of a piezoelectric quartz.The author extends his sincere gratitude to Dr. D. K. Sinha of Jadavpur University for his kind help and guidance in the preparation of this paper.     

A Cautionary note on modeling with fractional Lévy flights

Temporal scaling and infinite variance are two stylized features often seen together in times series of complex systems. We find that because of their infinite moments samples from fractional Lévy flights produce bi-linear scaling functions which may be incorrectly attributed as evidence of multifractality. We argue that it is unnecessary to consider truncated fractional Lévy flights which are inherently problematic.     

A note on the area spectrum of d-dimensional pure de Sitter Space-time

Consistent supercurrent multiplets are naturally associated with linearized off-shell supergravity models. In S.M. Kuzenko, J. High Energy Phys. 1004, 022 (2010) we presented the hierarchy of such supercurrents which correspond to all the models for linearized 4D $\mathcal{N}=1$ supergravity classified a few years ago. Here we analyze the correspondence between the most general supercurrent given in S.M. Kuzenko, J. High Energy Phys. 1004, 022 (2010) and the one obtained eight years ago in M. Magro et al., Ann. Phys. 298, 123 (2002) using the superfield Noether procedure. We apply the Noether procedure to the general $\mathcal{N}=1$ supersymmetric nonlinear sigma-model and show that it naturally leads to the so-called $\mathcal{S}$ -multiplet, revitalized in Z. Komargodski, N. Seiberg, J. High Energy Phys. 1007, 017 (2010).     

A note on the effect of non-elastic processes on elastic scattering

We study the effect of non-elastic processes on elastic scattering by means of Froissart's method. We derive the conditions under which this method leads to a unique solution and those under which inelastic processes lead to the creation of more resonances in the elastic channel. We derive further the generalization of Levinson's theorem for the case of the existence of nonelastic processes and we introduce an illustratrive explicitly solvable example.     

A note on the dynamic boundary conditions in Munk-like circulation models

The present note deals with Munk's ocean model and proposes an alternative approach to find its solution, with special regard to the western boundary layer. We introduce a suitable “distance” between the related Sverdrup streamfunction and all the admissible streamfunctions which are valid in the western boundary layer. We prove that such distance has a minimum that singles out a unique solution. Unlike the traditional method, this procedure works without assuming a priori any dynamic boundary condition. Received 16 July 2002 Published online 6 March 2003 RID="a" ID="a"e-mail: fulcri@itt.ts.cnr.it     

A numerical study of fractional rheological models and fractional Newell-Whitehead-Segel equation with non-local and non-singular kernel

In the recent years, few type of fractional derivatives which have non-local and non-singular kernel are introduced. In this work, we present fractional rheological models and Newell-Whitehead-Segel equations with non-local and non-singular kernel. For solving these equations, we present a spectral collocation method based on the shifted Legendre polynomials. To do this, we extend the unknown functions and its derivatives using the shifted Legendre basis. These expansions and the properties of the shifted Legendre polynomials along with the spectral collocation method will help us to reduce the main problem to a set of nonlinear algebraic equations. Finally, The accuracy and efficiency of the proposed method are reported by some illustrative examples.     

A note on vector flux models for radiation dose calculations

This paper reviews and extends modelling of anisotropic fluxes for radiation belt protons to provide closed-form equations for vector proton fluxes and proton flux anisotropy in terms of standard omnidirectional flux models. These equations provide a flexible alternative to the data-based vector flux models currently available. At higher energies, anisotropy of trapped proton flux in the upper atmosphere depends strongly on the variation of atmospheric density with altitude. Calculations of proton flux anisotropies using present models require specification of the average atmospheric density along trapped particle trajectories and its variation with mirror point altitude. For an isothermal atmosphere, calculations show that in a dipole magnetic field, the scale height of this trajectory-averaged density closely approximates the scale height of the atmosphere at the mirror point of the trapped particle. However, for the earth's magnetic field, the altitudes of mirror points vary for protons drifting in longitude. This results in a small increase in longitude-averaged scale heights compared to the atmospheric scale heights at minimum mirror point altitudes. The trajectory-averaged scale heights are increased by about 10-20% over scale heights from standard atmosphere models for protons mirroring at altitudes less than 500 km in the South Atlantic Anomaly. Atmospheric losses of protons in the geomagnetic field minimum in the South Atlantic Anomaly control proton flux anisotropies of interest for radiation studies in low earth orbit. Standard atmosphere models provide corrections for diurnal, seasonal and solar activity-driven variations. Thus, determination of an "equilibrium" model of trapped proton fluxes of a given energy requires using a scale height that is time-averaged over the lifetime of the protons. The trajectory-averaged atmospheric densities calculated here lead to estimates for trapped proton lifetimes. These lifetimes provide appropriate time-averaging intervals for equilibrium models of trapped proton fluxes.     

A note on fermion and gauge couplings in field theory models for tachyon condensation

We study soliton solutions in supersymmetric scalar field theory with a class of potentials. We study both bosonic and fermionic zero-modes around the soliton solution. We study two possible couplings of gauge fields to these models. While the Born–Infeld like coupling has one normalizable mode (the zero mode), the other kind of coupling has no normalizable modes. We show that quantum mechanical problem which determines the spectrum of fluctuation modes of the scalar, fermion and the gauge field is identical. We also show that only the lowest lying mode, i.e., the zero mode, is normalizable and the rest of the spectrum is continuous.     

Shackless on linear absorption models

We examine the fundamental constraints that all Linear Absorption Models must possess, independent of the rescattering amplitude. These constraints are most direct in impact parameter space, where the re-scattering appears simply as a multiplicative factor. It is a crucial test of such models that the ratio of two exchanges — for example vector and tensor exchanges — is completely specified in b-space by the ratio of input Regge pole amplitudes. Amplitude analysis exist for vector π exchange, in π⁻p→π^On. Lacking experimental A₂ tensor amplitudes, we use the Linear Absorption Models constraint to calculate A₂ exchange from ? input, and compare the results with π⁻p→η^On data. Both simplicity and duality assumptions for Regge pole couplings are considered. The results suggest that Linear Absorption Models constraint is not fully consistent with data.     

A note on the lumped parameter beam models based on mechanical impedance

Investigation of the three-parameter lumped mass model for a Bernoulli-Euler clamped-clamped beam has shown that the model is a universal model with respect to simple boundary conditions. Numerical results for the transient response due to a low frequency ground shock demonstrate the superiority of the beam model based on impedance methods.     

A note on the cathodic processes during electrolytic coloration of alkali halides

By using optical and scanning electron microscope techniques it has been shown that prior to electrolytic coloration of KBr the ionic transport taking place in the crystal leads to the formation of a new alkali metal cathode. Electrons emitted from this cathode and injected into the crystal create F-center.^{4, 5}