Show simple item record

dc.contributor.authorCooksey, Kathy
dc.contributor.authorThom, Christopher
dc.contributor.authorProchaska, J. Xavier
dc.contributor.authorChen, Hsiao-Wen
dc.date.accessioned2015-03-26T15:57:11Z
dc.date.available2015-03-26T15:57:11Z
dc.date.issued2010-01
dc.date.submitted2009-06
dc.identifier.issn0004-637X
dc.identifier.issn1538-4357
dc.identifier.urihttp://hdl.handle.net/1721.1/96201
dc.description.abstractWe surveyed the Hubble Space Telescope UV spectra of 49 low-redshift quasars for z < 1 C IV candidates, relying solely on the characteristic wavelength separation of the doublet. After consideration of the defining traits of C IV doublets (e.g., consistent line profiles, other associated transitions, etc.), we defined a sample of 38 definite (group G = 1) and five likely (G = 2) doublets with rest equivalent widths Wr for both lines detected at $\ge 3\sigma _{W_{r}}$. We conducted Monte Carlo completeness tests to measure the unblocked redshift (Δz) and co-moving path length (ΔX) over which we were sensitive to C IV doublets of a range of equivalent widths and column densities. The absorber line density of (G = 1+2) doublets is ${d}\mathcal {N}_{\mathrm{C\,IV}}/{d}X= 4.1^{+0.7}_{-0.6}$ for log N(C+3) ≥ 13.2, and ${d}\mathcal {N}_{\mathrm{C\,IV}}/{d}X$ has not evolved significantly since z = 5. The best-fit power law to the G = 1 frequency distribution of column densities $f(N(\mathrm{C}^{+3})) \equiv k(N(\mathrm{C}^{+3})/N_{0})^{\alpha _{N}}$ has coefficient k = 0.67+0.18 –0.16 × 10–14 cm2 and exponent α N = –1.50+0.17 –0.19, where N 0 = 1014 cm–2. Using the power-law model of f(N(C+3)), we measured the C+3 mass density relative to the critical density: $\Omega _{\mathrm{C}^{+3}}= (6.20^{+1.82}_{-1.52}) \times 10^{-8}$ for 13 ≤ log N(C+3) ≤ 15. This value is a 2.8 ± 0.7 increase in $\Omega _{\mathrm{C}^{+3}}$ compared to the error-weighted mean from several 1 < z < 5 surveys for C IV absorbers. A simple linear regression to $\Omega _{\mathrm{C}^{+3}}$ over the age of the universe indicates that $\Omega _{\mathrm{C}^{+3}}$ has slowly but steadily increased from z = 5 → 0, with ${d}\Omega _{\mathrm{C}^{+3}}/ {d}t_{\rm age} = (0.42\pm 0.2)\times 10^{-8}\,{\rm Gyr}^{-1}$.en_US
dc.description.sponsorshipSpace Telescope Science Institute (U.S.) (HST archival grant 10679)en_US
dc.description.sponsorshipNational Science Foundation (U.S.) (NSF CAREER grant AST 05_48180)en_US
dc.description.sponsorshipUnited States. National Aeronautics and Space Administration (NASA contract NAS 5-2655)en_US
dc.language.isoen_US
dc.publisherInstitute of Physics/American Astronomical Societyen_US
dc.relation.isversionofhttp://dx.doi.org/10.1088/0004-637x/708/1/868en_US
dc.rightsArticle is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use.en_US
dc.sourceAmerican Astronomical Societyen_US
dc.titleTHE LAST EIGHT-BILLION YEARS OF INTERGALACTIC C IV EVOLUTIONen_US
dc.typeArticleen_US
dc.identifier.citationCooksey, Kathy L., Christopher Thom, J. Xavier Prochaska, and Hsiao-Wen Chen. “THE LAST EIGHT-BILLION YEARS OF INTERGALACTIC C IV EVOLUTION.” The Astrophysical Journal 708, no. 1 (December 15, 2009): 868–908. © 2009 American Astronomical Society.en_US
dc.contributor.departmentMIT Kavli Institute for Astrophysics and Space Researchen_US
dc.contributor.mitauthorCooksey, Kathyen_US
dc.relation.journalAstrophysical Journalen_US
dc.eprint.versionFinal published versionen_US
dc.type.urihttp://purl.org/eprint/type/JournalArticleen_US
eprint.statushttp://purl.org/eprint/status/PeerRevieweden_US
dspace.orderedauthorsCooksey, Kathy L.; Thom, Christopher; Prochaska, J. Xavier; Chen, Hsiao-Wenen_US
mit.licensePUBLISHER_POLICYen_US
mit.metadata.statusComplete


Files in this item

Thumbnail

This item appears in the following Collection(s)

Show simple item record