Optical identification of XMM sources in the CFHTLS

dc.contributor.authorStalin, C. S.
dc.contributor.authorPetitjean, Patrick
dc.contributor.authorSrianand, R.
dc.contributor.authoret al.
dc.date.accessioned2012-03-05T10:02:41Z
dc.date.available2012-03-05T10:02:41Z
dc.date.issued2009-05-01
dc.description.abstractWe summarize the attempts by our group and others to derive constraints on variations of fundamental constants over cosmic time using quasar absorption lines. Most upper limits reside in the range 0.5 1.5 10 5 at the 3 level over a redshift range of approximately 0:5 2:5 for the fine-structure constant, , the proton-to-electron mass ratio, and a combination of the proton gyromagnetic factor and the two previous constants, gp( 2= ) , for only one claimed variation of . It is therefore very important to perform new measurements to improve the sensitivity of the numerous methods to at least <0.1 10 5 which should be possible in the next few years. Future instrumentations on ELTs in the optical and/or ALMA, EVLA and SKA pathfinders in the radio will undoutedly boost this field by allowing to reach much better signal-to-noise ratios at higher spectral resolution and to perform measurements on molecules in the ISM of high redshift galaxien_US
dc.identifier.urihttp://hdl.handle.net/11007/437
dc.language.isoenen_US
dc.relation.ispartofseriesIUCAA Preprint;29/09
dc.subjectQuasars absorption lines Physics Fundamental constantsen_US
dc.subjectQuasarsen_US
dc.subjectAbsorption linesen_US
dc.subjectPhysicsen_US
dc.subjectFundamental constantsen_US
dc.titleOptical identification of XMM sources in the CFHTLSen_US
dc.typeArticleen_US

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