34,320 research outputs found

    Constraints on primordial black holes and primeval density perturbations from the epoch of reionization

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    We investigate the constraint on the abundance of primordial black holes (PBHs) and the spectral index nn of primeval density perturbations given by the ionizing photon background at the epoch of reionization. Within the standard inflationary cosmogony, we show that the spectral index nn of the power-law power spectrum of primeval density perturbations should be n<n<1.27. Since the universe is still optical thick at the reionization redshift z6z\sim 6 - 8, this constraint is independent of the unknown parameter of reheating temperature of the inflation. The ionizing photon background from the PBHs can be well approximated by a power law spectrum J(ν)ν3J(\nu)\propto{\nu}^3, which is greatly different from those given by models of massive stars and quasars.Comment: 4 pages, 3 eps figues, to be published in ApJ Letter

    Near-threshold K+K^{+} Production in Heavy-ion Collisions

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    Within a hadronic transport model we study in detail contributions to kaon yields and momentum spectra from various baryon (resonance)-baryon (resonance) and πN\pi N interactions in heavy-ion collisions at beam energies near the free-space kaon production threshold. It is found that the finite lifetime of baryon resonances affects significantly the shape of kaon spectra, and the high energy parts of the kaon spectra are dominated by kaons from πNΛK+\pi N\rightarrow \Lambda K^{+} processes. N(1440)N^{*}(1440) resonances are found to contribute about 10\% to the kaon yield. Effects of boosting the Fermi momentum distributions of the two colliding nuclei into their center of mass frame, centrality of the reaction as well as the nuclear equation of state on kaon yields and spectra are also discussed. Model calculations on K+K^{+}, π+\pi^{+} and π\pi^{-} spectra for the reaction of Au+Au at Ebeam/A=1.0E_{beam}/A= 1.0 GeV are compared with the experimental data from the KaoS collaboration.Comment: 18 pages, 11 figures available upon request. TAMU preprint #940403

    Lyα\alpha Leaks in the Absorption Spectra of High Redshift QSOs

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    Spectra of high redshift QSOs show deep Gunn-Peterson absorptions on the blue sides of the \Lya emissions lines. They can be decomposed into components called \Lya leaks, defined to be emissive regions in complementary to otherwise zero-fluxed absorption gaps. Just like \Lya absorption forests at low redshifts, \Lya leaks are both easy to find in observations and containing rich sets of statistical properties that can be used to study the early evolution of the IGM. Among all properties of a leak profile, we investigate its equivalent width in this paper, since it is weakly affected by instrumental resolution and noise. Using 10 Keck QSO spectra at z6z\sim6, we have measured the number density distribution function n(W,z)n(W,z), defined to be the number of leaks per equivalent width WW and per redshift zz, in the redshift range 5.46.05.4 - 6.0. These new observational statistics, in both the differential and cumulative forms, fit well to hydro numerical simulations of uniform ionizing background in the Λ\LambdaCDM cosmology. In this model, Ly α\alpha leaks are mainly due to low density voids. It supports the early studies that the IGM at z6z\simeq6 would still be in a highly ionized state with neutral hydrogen fraction 104\simeq 10^{-4}. Measurements of n(W,z)n(W,z) at z>6z>6 would be effective to probe the reionization of the IGM.Comment: 3 figs, accepted by ApJ

    Bifurcation Boundary Conditions for Switching DC-DC Converters Under Constant On-Time Control

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    Sampled-data analysis and harmonic balance analysis are applied to analyze switching DC-DC converters under constant on-time control. Design-oriented boundary conditions for the period-doubling bifurcation and the saddle-node bifurcation are derived. The required ramp slope to avoid the bifurcations and the assigned pole locations associated with the ramp are also derived. The derived boundary conditions are more general and accurate than those recently obtained. Those recently obtained boundary conditions become special cases under the general modeling approach presented in this paper. Different analyses give different perspectives on the system dynamics and complement each other. Under the sampled-data analysis, the boundary conditions are expressed in terms of signal slopes and the ramp slope. Under the harmonic balance analysis, the boundary conditions are expressed in terms of signal harmonics. The derived boundary conditions are useful for a designer to design a converter to avoid the occurrence of the period-doubling bifurcation and the saddle-node bifurcation.Comment: Submitted to International Journal of Circuit Theory and Applications on August 10, 2011; Manuscript ID: CTA-11-016

    Adiabatic and non-adiabatic perturbations for loop quantum cosmology

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    We generalize the perturbations theory of loop quantum cosmology to a hydrodynamical form and define an effective curvature perturbation on an uniform density hypersurfaces ζe\zeta_e. As in the classical cosmology, ζe\zeta_e should be gauge-invariant and conservation on the large scales. The evolutions of both the adiabatic and the non-adiabatic perturbations for a multi-fluids model are investigated in the framework of the effective hydrodynamical theory of loop quantum cosmology with the inverse triad correction. We find that, different from the classical cosmology, the evolution of the large-scales non-adiabatic entropy perturbation can be driven by an adiabatic curvature perturbation and this adiabatic source for the non-adiabatic perturbation is a quantum effect. As an application of the related formalism, we study a decay model and give out the numerical results.Comment: 10 pages, 3 figure

    The origin of scale-scale correlations of the density perturbations during inflation

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    We show that scale-scale correlations are a generic feature of slow-roll inflation theories. These correlations result from the long-time tails characteristic of the time dependent correlations because the long wavelength density perturbation modes are diffusion-like. A relationship between the scale-scale correlations and time-correlations is established providing a way to reveal the time correlations of the perturbations during inflation. This mechanism provides for a testable prediction that the scale-scale correlations at two different spatial points will vanish.Comment: Accepted for publication, International Journal of Modern Physics, vol. 8 No.6 (Dec 1999
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