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dc.contributor.authorDopita, Michael A.
dc.contributor.authorKrauss, Lawrence M.
dc.contributor.authorSutherland, Ralph S.
dc.contributor.authorKobayashi, Chiaki
dc.contributor.authorLineweaver, Charles H.
dc.date.accessioned2011-12-20T15:01:04Z
dc.date.available2011-12-20T15:01:04Z
dc.date.issued2011-10
dc.identifier.citationDopita , M A , Krauss , L M , Sutherland , R S , Kobayashi , C & Lineweaver , C H 2011 , ' Re-ionizing the universe without stars ' , Astrophysics and Space Science , vol. 335 , no. 2 , pp. 345-352 . https://doi.org/10.1007/s10509-011-0786-7
dc.identifier.issn0004-640X
dc.identifier.otherPURE: 492676
dc.identifier.otherPURE UUID: 8b66b5b4-f615-450a-a05d-7559e5090a4d
dc.identifier.otherWOS: 000294680300004
dc.identifier.otherScopus: 80052459871
dc.identifier.otherORCID: /0000-0002-4343-0487/work/62750448
dc.identifier.urihttp://hdl.handle.net/2299/7417
dc.description.abstractRecent observations show that the measured rates of star formation in the early universe are insufficient to produce re-ionization, and therefore, another source of ionizing photons is required. In this Letter, we examine the possibility that these can be supplied by the fast accretion shocks formed around the cores of the most massive haloes (10.5 < log M/M (aS (TM))< 12) on spatial scales of order 1 kpc. We model the detailed physics of these fast accretion shocks, and apply these to a simple 1-D spherical hydrodynamic accretion model for baryonic infall in dark matter halos with an Einasto density distribution. The escape of UV photons from these halos is delayed by the time taken to reach the critical accretion shock velocity for escape of UV photons; 220 km s(-1), and by the time it takes for these photons to ionize the surrounding baryonic matter in the accretion flow. Assuming that in the universe at large the baryonic matter tracks the dark matter, we can estimate the epoch of re-ionization in the case that accretion shocks act alone as the source of UV photons. We find that 50% of the volume (and 5-8% of the mass) of the universe can be ionized by z similar to 7-8. The UV production rate has an uncertainty of a factor of about 5 due to uncertainties in the cosmological parameters controlling the development of large scale structure. Because our mechanism is a steeply rising function of decreasing redshift, this uncertainty translates to a re-ionization redshift uncertainty of less than +/- 0.5. We also find that, even without including the UV photon production of stars, re-ionization is essentially complete by z similar to 5.8. Thus, fast accretion shocks can provide an important additional source of ionizing photons in the early universe.en
dc.format.extent8
dc.language.isoeng
dc.relation.ispartofAstrophysics and Space Science
dc.subjectGalaxies: formation
dc.subjectGalaxies: halos
dc.subjectCosmology: theory
dc.subjectCosmology: early universe
dc.subjectUltraviolet: ISM
dc.subjectShock waves
dc.subjectULTRA-DEEP-FIELD
dc.subjectLYMAN-BREAK GALAXIES
dc.subjectSPECTRAL SIGNATURES
dc.subjectLUMINOSITY DENSITY
dc.subjectHIGH-REDSHIFT
dc.subjectFAST SHOCKS
dc.subjectREIONIZATION
dc.subjectHALOES
dc.subjectMODEL
dc.titleRe-ionizing the universe without starsen
dc.contributor.institutionCentre for Astrophysics Research
dc.contributor.institutionSchool of Physics, Engineering & Computer Science
dc.contributor.institutionDepartment of Physics, Astronomy and Mathematics
dc.description.statusPeer reviewed
rioxxterms.versionAM
rioxxterms.versionofrecordhttps://doi.org/10.1007/s10509-011-0786-7
rioxxterms.typeJournal Article/Review
herts.preservation.rarelyaccessedtrue


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