18,565 research outputs found

    Critical dynamics of the Potts model: short-time Monte Carlo simulations

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    We calculate the new dinamic exponent θ\theta of the 4-state Potts model, using short-time simulations. Our estimates θ1=0.0471(33)\theta_{1}=-0.0471(33) and θ2=% \theta_{2}= 0.0429(11)-0.0429(11) obtained by following the behavior of the magnetization or measuring the evolution of the time correlation function of the magnetization corroborate the conjecture by Okano et. al. In addition, these values agree with previous estimate of the same dynamic exponent for the two-dimensional Ising model with three-spin interactions in one direction, that is known to belong to the same universality class as the 4-state Potts model. The anomalous dimension of initial magnetization % x_{0}=z\theta +\beta /\nu is calculated by an alternative way that mixes two different initial conditions. We have also estimated the values of the static exponents β\beta and ν\nu . They are in complete agreement with the pertinent results of the literature.Comment: 12 pages, 7 figure

    An alternative order parameter for the 4-state Potts model

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    We have investigated the dynamic critical behavior of the two-dimensional 4-state Potts model using an alternative order parameter first used by Vanderzande [J. Phys. A: Math. Gen. \textbf{20}, L549 (1987)] in the study of the Z(5) model. We have estimated the global persistence exponent θg\theta_g by following the time evolution of the probability P(t)P(t) that the considered order parameter does not change its sign up to time tt. We have also obtained the critical exponents θ\theta, zz, ν\nu, and β\beta using this alternative definition of the order parameter and our results are in complete agreement with available values found in literature.Comment: 6 pages, 6 figure

    A possible Macronova in the late afterglow of the `long-short' burst GRB 060614

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    Long-duration (>2>2 s) γ\gamma-ray bursts that are believed to originate from the death of massive stars are expected to be accompanied by supernovae. GRB 060614, that lasted 102 s, lacks a supernova-like emission down to very stringent limits and its physical origin is still debated. Here we report the discovery of near-infrared bump that is significantly above the regular decaying afterglow. This red bump is inconsistent with even the weakest known supernova. However, it can arise from a Li-Paczy\'{n}ski macronova - the radioactive decay of debris following a compact binary merger. If this interpretation is correct GRB 060614 arose from a compact binary merger rather than from the death of a massive star and it was a site of a significant production of heavy r-process elements. The significant ejected mass favors a black hole-neutron star merger but a double neutron star merger cannot be ruled out.Comment: Minor revision; The version published in Nature Communication

    GRB 120729A: External Shock Origin for Both the Prompt Gamma-Ray Emission and Afterglow

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    Gamma-ray burst (GRB) 120729A was detected by Swift/BAT and Fermi/GBM, and then rapidly observed by Swift/XRT, Swift/UVOT, and ground-based telescopes. It had a single long and smooth \gamma-ray emission pulse, which extends continuously to the X-rays. We report Lick/KAIT observations of the source, and make temporal and spectral joint fits of the multiwavelength light curves of GRB 120729A. It exhibits achromatic light-curve behavior, consistent with the predictions of the external shock model. The light curves are decomposed into four typical phases: onset bump (Phase I), normal decay (Phase II), shallow decay (Phase III), and post-jet break (Phase IV). The spectral energy distribution (SED) evolves from prompt \gamma-ray emission to the afterglow with photon index from Γγ=1.36 to Γ≈1.75. There is no obvious evolution of the SED during the afterglow. ...(Please see article full tet for complete abstract.
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