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      Evolution of linear wave dark matter perturbations in the radiation-dominant era

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          Abstract

          Linear perturbations of the wave dark matter, or \(\psi\) dark matter (\(\psi\)DM), of particle mass \(\sim 10^{-22}\)eV in the radiation-dominant era are analyzed, and the matter power spectrum at the photon-matter equality is obtained. We identify four phases of evolution for \(\psi\)DM perturbations, where the dynamics can be vastly different from the counterparts of cold dark matter (CDM). While in late stages after mass oscillation long-wave \(\psi\)DM perturbations are almost identical to CDM perturbations, some subtle differences remain, let alone intermediate-to-short waves that bear no resemblance with those of CDM throughout the whole evolutionary history. The dissimilarity is due to quantum mechanical effects which lead to severe mode suppression. We also discuss the axion model with a cosine field potential. The power spectrum of axion models are generally almost identical to those of \(\psi\)DM, but in the extreme case when the initial axion angle is near the field potential top, this axion model predicts a higher spectral cutoff than \(\psi\)DM, which is equivalent to having a higher particle mass for \(\psi\)DM.

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          Cosmic Structure as the Quantum Interference of a Coherent Dark Wave

          The conventional cold, particle interpretation of dark matter (CDM) still lacks laboratory support and struggles with the basic properties of common dwarf galaxies, which have surprisingly uniform central masses and shallow density profiles. In contrast, galaxies predicted by CDM extend to much lower masses, with steeper, singular profiles. This tension motivates cold, wavelike dark matter (\(\psi\)DM) composed of a non-relativistic Bose-Einstein condensate, so the uncertainty principle counters gravity below a Jeans scale. Here we achieve the first cosmological simulations of this quantum state at unprecedentedly high resolution capable of resolving dwarf galaxies, with only one free parameter, \(\bf{m_B}\), the boson mass. We demonstrate the large scale structure of this \(\psi\)DM simulation is indistinguishable from CDM, as desired, but differs radically inside galaxies. Connected filaments and collapsed haloes form a large interference network, with gravitationally self-bound solitonic cores inside every galaxy surrounded by extended haloes of fluctuating density granules. These results allow us to determine \(\bf{m_B=(8.1^{+1.6}_{-1.7})\times 10^{-23}~eV}\) using stellar phase-space distributions in dwarf spheroidal galaxies. Denser, more massive solitons are predicted for Milky Way sized galaxies, providing a substantial seed to help explain early spheroid formation. Suppression of small structures means the onset of galaxy formation for \(\psi\)DM is substantially delayed relative to CDM, appearing at \(\bf{z\lesssim 13}\) in our simulations.
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            A candidate redshift z ~ 10 galaxy and rapid changes in that population at an age of 500 Myr

            Searches for very-high-redshift galaxies over the past decade have yielded a large sample of more than 6,000 galaxies existing just 900-2,000 million years (Myr) after the Big Bang (redshifts 6 > z > 3; ref. 1). The Hubble Ultra Deep Field (HUDF09) data have yielded the first reliable detections of z ~ 8 galaxies that, together with reports of a gamma-ray burst at z ~ 8.2 (refs 10, 11), constitute the earliest objects reliably reported to date. Observations of z ~ 7-8 galaxies suggest substantial star formation at z > 9-10. Here we use the full two-year HUDF09 data to conduct an ultra-deep search for z ~ 10 galaxies in the heart of the reionization epoch, only 500 Myr after the Big Bang. Not only do we find one possible z ~ 10 galaxy candidate, but we show that, regardless of source detections, the star formation rate density is much smaller (~10%) at this time than it is just ~200 Myr later at z ~ 8. This demonstrates how rapid galaxy build-up was at z ~ 10, as galaxies increased in both luminosity density and volume density from z ~ 8 to z ~ 10. The 100-200 Myr before z ~ 10 is clearly a crucial phase in the assembly of the earliest galaxies.
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              Flummoxed by fake fruits

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                Author and article information

                Journal
                2017-02-22
                Article
                1702.07065
                a7c269e7-8111-454f-ba98-1669258ac6c7

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

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                Custom metadata
                20 pages, 7 figures
                astro-ph.CO

                Cosmology & Extragalactic astrophysics
                Cosmology & Extragalactic astrophysics

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