236 research outputs found

    Cavitation Damage During Flexural Creep of SiAlON–YAG Ceramics

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    Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/65505/1/j.1151-2916.1991.tb07156.x.pd

    Electroweak Bubble Nucleation, Nonperturbatively

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    We present a lattice method to compute bubble nucleation rates at radiatively induced first order phase transitions, in high temperature, weakly coupled field theories, nonperturbatively. A generalization of Langer's approach, it makes no recourse to saddle point expansions and includes completely the dynamical prefactor. We test the technique by applying it to the electroweak phase transition in the minimal standard model, at an unphysically small Higgs mass which gives a reasonably strong phase transition (lambda/g^2 =0.036, which corresponds to m(Higgs)/m(W) = 0.54 at tree level but does not correspond to a positive physical Higgs mass when radiative effects of the top quark are included), and compare the results to older perturbative and other estimates. While two loop perturbation theory slightly under-estimates the strength of the transition measured by the latent heat, it over-estimates the amount of supercooling by a factor of 2.Comment: 48 pages, including 16 figures. Minor revisions and typo fixes, nothing substantial, conclusions essentially unchange

    Baryogenesis from Primordial Blackholes after Electroweak Phase Transition

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    Incorporating a realistic model for accretion of ultra-relativistic particles by primordial blackholes (PBHs), we study the evolution of an Einstein-de Sitter universe consisting of PBHs embedded in a thermal bath from the epoch ∌10−33\sim 10^{-33} sec to ∌5×10−9\sim 5\times 10^{-9} sec. In this paper we use Barrow et al's ansatz to model blackhole evaporation in which the modified Hawking temperature goes to zero in the limit of the blackhole attaining a relic state with mass ∌mpl\sim m_{pl}. Both single mass PBH case as well as the case in which blackhole masses are distributed in the range 8×102−3×1058\times 10^2 - 3\times 10^5 gm have been considered in our analysis. Blackholes with mass larger than ∌105\sim 10^5 gm appear to survive beyond the electroweak phase transition and, therefore, successfully manage to create baryon excess via X−XˉX-\bar X emissions, averting the baryon number wash-out due to sphalerons. In this scenario, we find that the contribution to the baryon-to-entropy ratio by PBHs of initial mass mm is given by ∌ϔζ(m/1gm)−1\sim \epsilon \zeta (m/1 {gm})^{-1}, where Ï”\epsilon and ζ\zeta are the CP-violating parameter and the initial mass fraction of the PBHs, respectively. For Ï”\epsilon larger than ∌10−4\sim 10^{-4}, the observed matter-antimatter asymmetry in the universe can be attributed to the evaporation of PBHs.Comment: Latex2e file with seven figures included as postscript file

    The order of the quantum chromodynamics transition predicted by the standard model of particle physics

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    We determine the nature of the QCD transition using lattice calculations for physical quark masses. Susceptibilities are extrapolated to vanishing lattice spacing for three physical volumes, the smallest and largest of which differ by a factor of five. This ensures that a true transition should result in a dramatic increase of the susceptibilities.No such behaviour is observed: our finite-size scaling analysis shows that the finite-temperature QCD transition in the hot early Universe was not a real phase transition, but an analytic crossover (involving a rapid change, as opposed to a jump, as the temperature varied). As such, it will be difficult to find experimental evidence of this transition from astronomical observations.Comment: 7 pages, 4 figure
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