12,638 research outputs found

    Fluctuation theorems and orbital magnetism in nonequilibrium state

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    We study Langevin dynamics of a driven charged particle in the presence as well as in the absence of magnetic field. We discuss the validity of various work fluctuation theorems using different model potentials and external drives. We also show that one can generate an orbital magnetic moment in a nonequilibrium state which is absent in equilibrium.Comment: Based on a talk by A. M. J at international workshop MESODIS'06 (IIT Kanpur,Dec-2006

    A Regulatory approach to financial product advice and distribution

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    Financial distribution, where the distributor is the agent of both the product provider and the customer has been found to inherently work against the interests of customers, in the form of high service fees and perverse incentives in sales practices. This paper proposes segregation of financial advice from financial distribution. It proposes a Financial Advisers Bill, 2012, to promote the development of a market for advice. The Bill suggests that financial advisers be recognised as professionals and be regulated under a new statutory body called the Institute of Financial Advisers of India. The paper suggests that regulation of distributors continue to remain under the purview of product regulators. It outlines alternative models in which the distribution market may be organised. It also points out that the Ministry of Finance and the Financial Stability and Development Council need to play an active role in co-ordinating the setting of common standards for distribution across all product regulators.Consumer Protection; distribution regulation; mutual funds; insurance; pensions; investment advice

    Neutrino Mass, Coupling Unification, Verifiable Proton Decay, Vacuum Stability and WIMP Dark Matter in SU(5)

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    Nonsupersymmetric minimal SU(5) with Higgs representations 24H{24}_H and 5H5_H and standard fermions in 5ˉF⊕10F{\bar 5}_F\oplus {10}_F is well known for its failure in unification of gauge couplings and lack of predicting neutrino masses. Like standard model, it is also affected by the instability of the Higgs scalar potential. We note that extending the Higgs sector by 75H{75}_H and 15H{15}_H not only leads to the popular type-II seesaw ansatz for neutrino masses with a lower bound on the triplet mass MΔ>2×109M_{\Delta} > 2\times 10^9 GeV, but also achieves precision unification of gauge couplings without proliferation of non-standard light Higgs scalars or fermions near the TeV scale. Consistent with recent LUX-2016 lower bound, the model easily accommodates a singlet scalar WIMP dark matter near the TeV scale which resolves the vacuum stability issue even after inclusion of heavy triplet threshold effect. We estimate proton lifetime predictions for p→e+π0p\to e^+\pi^0 including uncertainties due to input parameters and threshold effects due to superheavy Higgs scalars and superheavy X±4/3,Y±1/3X^{\pm 4/3},Y^{\pm 1/3} gauge bosons. The predicted lifetime is noted to be verifiable at Super Kamiokande and Hyper Kamiokande experiments.Comment: 36 pages, 9 figures (Accepted for publication in Advances in High Energy Physics

    Quantum Stochastic Absorption

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    We report a detailed and systematic study of wave propagation through a stochastic absorbing random medium. Stochastic absorption is modeled by introducing an attenuation constant per unit length α\alpha in the free propagation region of the one-dimensional disordered chain of delta function scatterers. The average value of the logarithm of transmission coefficient decreases linearly with the length of the sample. The localization length is given by ξ = ξwξα/(ξw+ξα)\xi ~ = ~ \xi_w \xi_\alpha / (\xi_w + \xi_\alpha), where ξw\xi_w and ξα\xi_\alpha are the localization lengths in the presence of only disorder and of only absorption respectively. Absorption does not introduce any additional reflection in the limit of large α\alpha, i.e., reflection shows a monotonic decrease with α\alpha and tends to zero in the limit of α→∞\alpha\to\infty, in contrast to the behavior observed in case of coherent absorption. The stationary distribution of reflection coefficient agrees well with the analytical results obtained within random phase approximation (RPA) in a larger parameter space. We also emphasize the major differences between the results of stochastic and coherent absorption.Comment: RevTex, 6 pages,2 column format, 9 .eps figures include

    Modelling of Stochastic Absorption in a Random Medium

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    We report a detailed and systematic study of wave propagation through a stochastic absorbing random medium. Stochastic absorption is modeled by introducing an attenuation constant per unit length α\alpha in the free propagation region of the one-dimensional disordered chain of delta function scatterers. The average value of the logarithm of transmission coefficient decreases linearly with the length of the sample. The localization length is given by ξ = ξwξα/(ξw+ξα)\xi ~ = ~ \xi_w \xi_\alpha / (\xi_w + \xi_\alpha), where ξw\xi_w and ξα\xi_\alpha are the localization lengths in the presence of only disorder and of only absorption respectively. Absorption does not introduce any additional reflection in the limit of large α\alpha, i.e., reflection shows a monotonic decrease with α\alpha and tends to zero in the limit of α→∞\alpha\to\infty, in contrast to the behavior observed in case of coherent absorption. The stationary distribution of reflection coefficient agrees well with the analytical results obtained within random phase approximation (RPA) in a larger parameter space. We also emphasize the major differences between the results of stochastic and coherent absorption.Comment: 7 pages RevTex, 9 eps figures included, modified version of cond-mat/9909327, to appear in PRB, mpeg simulations at http://www.iopb.res.in/~joshi/mpg.htm
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