002213418 001__ 2213418
002213418 003__ SzGeCERN
002213418 005__ 20180924164857.0
002213418 0247_ $$2DOI$$a10.22323/1.276.0049
002213418 0248_ $$aoai:cds.cern.ch:2213418$$pINIS$$pcerncds:CERN:FULLTEXT$$pcerncds:FULLTEXT$$pcerncds:CERN
002213418 037__ $$aCMS-CR-2016-204
002213418 035__ $$9Inspire$$a1589703
002213418 041__ $$aeng
002213418 100__ $$aWoods, Nathaniel$$iINSPIRE-00348449$$jCCID-738182$$uWisconsin U., Madison
002213418 245__ $$aDiboson and multiboson results with CMS
002213418 260__ $$c2016
002213418 269__ $$aGeneva$$bCERN$$c31 Aug 2016
002213418 300__ $$a12 p
002213418 520__ $$aWe summarize the results of recent studies of diboson and multiboson production performed on proton-proton collision data from the CMS detector at the LHC. Results discussed include ZZ, W$^\pm$Z, and W$^+$W$^-$ inclusive cross section measurements at $\sqrt{s} = 13$~TeV, as well as measurements of the Z$\gamma\gamma$, W$^\pm\gamma\gamma$, $\gamma\gamma \to $W$^+$W$^-$, and electroweak Z$\gamma + 2$jets and W$^\pm\gamma + 2$jets cross sections at $\sqrt{s} = 8$~TeV. Measurements done at $\sqrt{s} = 8$~TeV are used to place limits on anomalous quartic gauge boson couplings.
002213418 540__ $$3Preprint$$aCC-BY-4.0
002213418 595__ $$aCERN EDS
002213418 65017 $$2SzGeCERN$$aDetectors and Experimental Techniques
002213418 6531_ $$9CMS$$aPhysics
002213418 690C_ $$aINTNOTE
002213418 690C_ $$aCERN
002213418 690C_ $$aPUBLCMS
002213418 693__ $$aCERN LHC$$eCMS
002213418 710__ $$5PH
002213418 710__ $$gCMS Collaboration
002213418 773__ $$c49$$pPoS$$vLHCP2016$$wC16-06-13$$y2016
002213418 8564_ $$81241428$$s1951915$$uhttps://cds.cern.ch/record/2213418/files/CR2016_204.pdf
002213418 8564_ $$81335378$$s1891084$$uhttps://cds.cern.ch/record/2213418/files/PoS(LHCP2016)049.pdf
002213418 916__ $$sn$$w201637
002213418 963__ $$aPUBLIC
002213418 962__ $$b2010942$$k49$$nlund20160613
002213418 980__ $$aINTNOTECMSPUBL
002213418 980__ $$aConferencePaper
002213418 980__ $$aARTICLE