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dc.contributor.authorRest, A.
dc.contributor.authorScolnic, D.
dc.contributor.authorFoley, R. J.
dc.contributor.authorHuber, M. E.
dc.contributor.authorChornock, R.
dc.contributor.authorNarayan, G.
dc.contributor.authorTonry, J. L.
dc.contributor.authorBerger, E.
dc.contributor.authorSoderberg, A. M.
dc.contributor.authorStubbs, C. W.
dc.contributor.authorRiess, A.
dc.contributor.authorKirshner, R. P.
dc.contributor.authorSmartt, S. J.
dc.contributor.authorSchlafly, E.
dc.contributor.authorRodney, S.
dc.contributor.authorBotticella, M. T.
dc.contributor.authorBrout, D.
dc.contributor.authorChallis, P.
dc.contributor.authorCzekala, I.
dc.contributor.authorDrout, M.
dc.contributor.authorHudson, M. J.
dc.contributor.authorKotak, R.
dc.contributor.authorLeibler, C.
dc.contributor.authorLunnan, R.
dc.contributor.authorMarion, G. H.
dc.contributor.authorMcCrum, M.
dc.contributor.authorMilisavljevic, D.
dc.contributor.authorPastorello, A.
dc.contributor.authorSanders, N. E.
dc.contributor.authorSmith, K.
dc.contributor.authorStafford, E.
dc.contributor.authorThilker, D.
dc.contributor.authorValenti, S.
dc.contributor.authorWood-Vasey, W. M.
dc.contributor.authorZheng, Z.
dc.contributor.authorBurgett, W. S.
dc.contributor.authorChambers, K. C.
dc.contributor.authorDenneau, L.
dc.contributor.authorDraper, P. W.
dc.contributor.authorFlewelling, H.
dc.contributor.authorHodapp, K. W.
dc.contributor.authorKaiser, N.
dc.contributor.authorKudritzki, R.-P.
dc.contributor.authorMagnier, E. A.
dc.contributor.authorMetcalfe, N.
dc.contributor.authorPrice, P. A.
dc.contributor.authorSweeney, W.
dc.contributor.authorWainscoat, R.
dc.contributor.authorWaters, C.
dc.date.accessioned2024-05-17T12:30:06Z
dc.date.available2024-05-17T12:30:06Z
dc.date.issued2014-11-01
dc.identifier295924947
dc.identifierf4bb02bc-a7da-4b5f-ac36-29ffeefb8c4d
dc.identifier84908095238
dc.identifier.citationRest , A , Scolnic , D , Foley , R J , Huber , M E , Chornock , R , Narayan , G , Tonry , J L , Berger , E , Soderberg , A M , Stubbs , C W , Riess , A , Kirshner , R P , Smartt , S J , Schlafly , E , Rodney , S , Botticella , M T , Brout , D , Challis , P , Czekala , I , Drout , M , Hudson , M J , Kotak , R , Leibler , C , Lunnan , R , Marion , G H , McCrum , M , Milisavljevic , D , Pastorello , A , Sanders , N E , Smith , K , Stafford , E , Thilker , D , Valenti , S , Wood-Vasey , W M , Zheng , Z , Burgett , W S , Chambers , K C , Denneau , L , Draper , P W , Flewelling , H , Hodapp , K W , Kaiser , N , Kudritzki , R-P , Magnier , E A , Metcalfe , N , Price , P A , Sweeney , W , Wainscoat , R & Waters , C 2014 , ' Cosmological constraints from measurements of type Ia supernovae discovered during the first 1.5 yr of the Pan-STARRS1 survey ' , Astrophysical Journal , vol. 795 , no. 1 , 44 . https://doi.org/10.1088/0004-637X/795/1/44en
dc.identifier.issn0004-637X
dc.identifier.otherBibCode: 2014ApJ...795...44R
dc.identifier.otherORCID: /0000-0002-1483-8811/work/146464252
dc.identifier.urihttps://hdl.handle.net/10023/29901
dc.description.abstractWe present grizP1 light curves of 146 spectroscopically confirmed Type Ia supernovae (SNe Ia 0.03 < z < 0.65) discovered during the first 1.5 yr of the Pan-STARRS1 Medium Deep Survey. The Pan-STARRS1 natural photometric system is determined by a combination of on-site measurements of the instrument response function and observations of spectrophotometric standard stars. We find that the systematic uncertainties in the photometric system are currently 1.2% without accounting for the uncertainty in the Hubble Space Telescope Calspec definition of the AB system. A Hubble diagram is constructed with a subset of 113 out of 146 SNe Ia that pass our light curve quality cuts. The cosmological fit to 310 SNe Ia (113 PS1 SNe Ia + 222 light curves from 197 low-z SNe Ia), using only supernovae (SNe) and assuming a constant dark energy equation of state and flatness, yields w=-1.120+0.360-0.206(Stat) +0.269-0.291(Sys). When combined with BAO+CMB(Planck)+H 0, the analysis yields ΩM=0.280+0.013-0.012 and w=-1.166+0.072-0.069 including all identified systematics. The value of w is inconsistent with the cosmological constant value of -1 at the 2.3σ level. Tension endures after removing either the baryon acoustic oscillation (BAO) or the H0 constraint, though it is strongest when including the H 0 constraint. If we include WMAP9 cosmic microwave background (CMB) constraints instead of those from Planck, we find w=-1.124+0.083-0.065, which diminishes the discord to
dc.format.extent34
dc.format.extent2122553
dc.language.isoeng
dc.relation.ispartofAstrophysical Journalen
dc.subjectCosmological parametersen
dc.subjectCosmology: observationsen
dc.subjectDark energyen
dc.subjectSupernovae: generalen
dc.subjectQB Astronomyen
dc.subject.lccQBen
dc.titleCosmological constraints from measurements of type Ia supernovae discovered during the first 1.5 yr of the Pan-STARRS1 surveyen
dc.typeJournal articleen
dc.contributor.institutionUniversity of St Andrews. School of Physics and Astronomyen
dc.identifier.doi10.1088/0004-637X/795/1/44
dc.description.statusPeer revieweden
dc.identifier.urlhttp://adsabs.harvard.edu/abs/2014ApJ...795...44Ren


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