96,433 research outputs found

    The Global 21-cm Signal in the Context of the High-z Galaxy Luminosity Function

    Get PDF
    Motivated by recent progress in studies of the high-zz Universe, we build a new model for the global 21-cm signal that is explicitly calibrated to measurements of the galaxy luminosity function (LF) and further tuned to match the Thomson scattering optical depth of the cosmic microwave background, τe\tau_e. Assuming that the z≲8z \lesssim 8 galaxy population can be smoothly extrapolated to higher redshifts, the recent decline in best-fit values of τe\tau_e and the inefficient heating induced by X-ray binaries (HMXBs; the presumptive sources of the X-ray background at high-zz) imply that the entirety of cosmic reionization and reheating occurs at redshifts z≲12z \lesssim 12. In contrast to past global 21-cm models, whose z∼20z \sim 20 (ν∼70\nu \sim 70 MHz) absorption features and strong ∼25\sim 25 mK emission features were driven largely by the assumption of efficient early star-formation and X-ray heating, our new fiducial model peaks in absorption at ν∼110\nu \sim 110 MHz at a depth of ∼−160\sim -160 mK and has a negligible emission component. As a result, a strong emission signal would provide convincing evidence that HMXBs are not the only drivers of cosmic reheating. Shallow absorption troughs should accompany strong heating scenarios, but could also be caused by a low escape fraction of Lyman-Werner photons. Generating signals with troughs at ν≲95\nu \lesssim 95 MHz requires a floor in the star-formation efficiency in halos below ∼109M⊙\sim 10^{9} M_{\odot}, which is equivalent to steepening the faint-end of the galaxy LF. These findings demonstrate that the global 21-cm signal is a powerful complement to current and future galaxy surveys and efforts to better understand the interstellar medium in high-zz galaxies.Comment: 17 pages, 9 figures, in pres

    Achieving Effective Innovation Based On TRIZ Technological Evolution

    Get PDF
    Organised by: Cranfield UniversityThis paper outlines the conception of effective innovation and discusses the method to achieve it. Effective Innovation is constrained on the path of technological evolution so that the corresponding path must be detected before conceptual design of the product. The process of products technological evolution is a technical developing process that the products approach to Ideal Final Result (IFR). During the process, the sustaining innovation and disruptive innovation carry on alternately. By researching and forecasting potential techniques using TRIZ technological evolution theory, the effective innovation can be achieved finally.Mori Seiki – The Machine Tool Compan

    Phantom Accretion by Five Dimensional Charged Black Hole

    Full text link
    This paper deals with the dynamical behavior of phantom field near five dimensional charged black hole. We formulate equations of motion for steady-state spherically symmetric flow of phantom fluids. It is found that phantom energy accretes onto black holes for u<0u<0. Further, the location of critical point of accretion are evaluated that leads to mass to charge ratio for 5D charged black hole. This ratio implies that accretion cannot transform a black hole into a naked singularity. We would like to mention here that this work is an irreducible extension of 4D charged black hole.Comment: 8 pages, accepted for publication in Mod. Phys. Lett.

    Transmission Phase of an Isolated Coulomb-Blockade Resonance

    Full text link
    In two recent papers, O. Entin-Wohlman et al. studied the question: ``Which physical information is carried by the transmission phase through a quantum dot?'' In the present paper, this question is answered for an islolated Coulomb-blockade resonance and within a theoretical model which is more closely patterned after the geometry of the actual experiment by Schuster et al. than is the model of O. Entin-Wohlman et al. We conclude that whenever the number of leads coupled to the Aharanov-Bohm interferometer is larger than two, and the total number of channels is sufficiently large, the transmission phase does reflect the Breit-Wigner behavior of the resonance phase shift.Comment: 6 pages and one figur

    Time reversal symmetry breaking superconductivity

    Full text link
    We study time reversal symmetry breaking superconductivity with Δk=Δx2−y2(k)+eiθΔα\Delta_k = \Delta_{x^2-y^2} (k) +e^{i\theta} \Delta_{\alpha} (α=s\alpha = s or dxyd_{xy}) symmetries. It is shown that the behavior of such superconductors could be {\em qualitatively} different depending on the minor components (α\alpha) and its phase at lower temperatures. It is argued that such {\em qualitatively different} behaviors in thermal as well as in angular dependencies could be a {\em source} of consequences in transport and Josephson physics. Orthorhombicity is found to be a strong mechanism for mixed phase (in case of α=s\alpha = s). We show that due to electron correlation the order parameter is more like a pure dx2−y2d_{x^2-y^2} symmetry near optimum doping.Comment: 5 pages, 5 figures (attached), to be published in Physical Review
    • …
    corecore