153 research outputs found

    Statistical properties of single-file diffusion front

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    Statistical properties of the front of a semi-infinite system of single-file diffusion (one dimensional system where particles cannot pass each other, but in-between collisions each one independently follow diffusive motion) are investigated. Exact as well as asymptotic results are provided for the probability density function of (a) the front-position, (b) the maximum of the front-positions, and (c) the first-passage time to a given position. The asymptotic laws for the front-position and the maximum front-position are found to be governed by the Fisher-Tippett-Gumbel extreme value statistics. The asymptotic properties of the first-passage time is dominated by a stretched-exponential tail in the distribution. The farness of the front with the rest of the system is investigated by considering (i) the gap from the front to the closest particle, and (ii) the density profile with respect to the front-position, and analytical results are provided for late time behaviors.Comment: 4 revtex page

    Work fluctuations for a harmonic oscillator driven by an external random force

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    The fluctuations of the work done by an external Gaussian random force on a harmonic oscillator that is also in contact with a thermal bath is studied. We have obtained the exact large deviation function as well as the complete asymptotic forms of the probability density function. The distribution of the work done are found to be non-Gaussian. The steady state fluctuation theorem holds only if the ratio of the variances, of the external random forcing and the thermal noise respectively, is less than 1/3. On the other hand, the transient fluctuation theorem holds (asymptotically) for all the values of that ratio. The theoretical asymptotic forms of the probability density function are in very good agreement with the numerics as well as with an experiment.Comment: 6 pages, 4 figure

    Record Statistics of Continuous Time Random Walk

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    The statistics of records for a time series generated by a continuous time random walk is studied, and found to be independent of the details of the jump length distribution, as long as the latter is continuous and symmetric. However, the statistics depend crucially on the nature of the waiting time distribution. The probability of finding M records within a given time duration t, for large t, has a scaling form, and the exact scaling function is obtained in terms of the one-sided Levy stable law. The mean of the ages of the records, defined as , differs from t/. The asymptotic behaviour of the shortest and the longest ages of the records are also studied.Comment: 5 pages, 3 figures; EPL published versio

    Fluctuation theorem for entropy production of a partial system in the weak coupling limit

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    Small systems in contact with a heat bath evolve by stochastic dynamics. Here we show that, when one such small system is weakly coupled to another one, it is possible to infer the presence of such weak coupling by observing the violation of the steady state fluctuation theorem for the partial entropy production of the observed system. We give a general mechanism due to which the violation of the fluctuation theorem can be significant, even for weak coupling. We analytically demonstrate on a realistic model system that this mechanism can be realized by applying an external random force to the system. In other words, we find a new fluctuation theorem for the entropy production of a partial system, in the limit of weak coupling.Comment: 7 pages, 3 figure

    Driven inelastic Maxwell gases

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    We consider the inelastic Maxwell model, which consists of a collection of particles that are characterized by only their velocities, and evolving through binary collisions and external driving. At any instant, a particle is equally likely to collide with any of the remaining particles. The system evolves in continuous time with mutual collisions and driving taken to be point processes with rates τc1\tau_c^-{1} and τw1\tau_w^{-1} respectively. The mutual collisions conserve momentum and are inelastic, with a coefficient of restitution rr. The velocity change of a particle with velocity vv, due to driving, is taken to be Δv=(1+rw)v+η\Delta v=-(1+r_w) v+\eta, mimicking the collision with a vibrating wall, where rwr_w the coefficient of restitution of the particle with the "wall" and η\eta is Gaussian white noise. The Ornstein-Uhlenbeck driving mechanism given by dvdt=Γv+η\frac{dv}{dt}=-\Gamma v+\eta is found to be a special case of the driving modeled as a point process. Using both the continuum and discrete versions we show that while the equations for the one-particle and the two-particle velocity distribution functions do not close, the joint evolution equations of the variance and the two-particle velocity correlation functions close. With the exact formula for the variance we find that, for rw1r_w\ne-1, the system goes to a steady state. On the other hand, for rw=1r_w=-1, the system does not have a steady state. Similarly, the system goes to a steady state for the Ornstein-Uhlenbeck driving with Γ0\Gamma\not=0, whereas for the purely diffusive driving (Γ=0\Gamma=0), the system does not have a steady state.Comment: 9 pages, 4 figure

    Heat and work fluctuations for a harmonic oscillator

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    The formalism of Kundu et al. [J. Stat. Mech. (2011) P03007], for computing the large deviations of heat flow in harmonic systems, is applied to the case of single Brownian particle in a harmonic trap and coupled to two heat baths at different temperatures. The large-t form of the moment generating function ~ g(s) exp[t m(s)], of the total heat flow Q from one of the baths to the particle in a given time interval t, is studied and exact explicit expressions are obtained for both m(s) and g(s). For a special case of the single particle problem that corresponds to the work done by an external stochastic force on a harmonic oscillator coupled to a thermal bath, the large-t form of the moment generating function is analyzed to obtain the exact large deviation function as well as the complete asymptotic forms of the probability density function of the work.Comment: 11 pages, 6 figure
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