Measurement of the Production Cross Section Ratio Sigma(chi B2(1p))/Sigma(chi B1(1p)) in Pp Collisions at Root S=8tev
| dc.contributor.author | Karapınar, Güler | |
| dc.coverage.doi | 10.1016/j.physletb.2015.02.048 | |
| dc.date.accessioned | 2017-07-12T08:12:59Z | |
| dc.date.available | 2017-07-12T08:12:59Z | |
| dc.date.issued | 2015 | |
| dc.description.abstract | A measurement of the production cross section ratio σ(χb2(1P))/σ(χb1(1P)) is presented. The χb1(1P) and χb2(1P) bottomonium states, promptly produced in pp collisions at s=8TeV, are detected by the CMS experiment at the CERN LHC through their radiative decays χb1,2(1P)→ϒ(1S)+γ. The emitted photons are measured through their conversion to e+e- pairs, whose reconstruction allows the two states to be resolved. The ϒ(1S) is measured through its decay to two muons. An event sample corresponding to an integrated luminosity of 20.7fb-1 is used to measure the cross section ratio in a phase-space region defined by the photon pseudorapidity, |ηγ|<1.0; the ϒ(1S) rapidity, |yϒ|<1.5; and the ϒ(1S) transverse momentum, 7<pTϒ<40GeV. The cross section ratio shows no significant dependence on the ϒ(1S) transverse momentum, with a measured average value of 0.85±0.07(stat+syst)±0.08(BF), where the first uncertainty is the combination of the experimental statistical and systematic uncertainties and the second is from the uncertainty in the ratio of the χb branching fractions. © 2015 CERN for the benefit of the CMS Collaboration. | en_US |
| dc.description.sponsorship | The Scientific and Technical Research Council of Turkey, and Turkish Atomic Energy Authority | en_US |
| dc.identifier.citation | Khachatryan, V., Sirunyan, A.M., Tumasyan, A., Adam, W., Bergauer, T., Dragicevic, M.,...CMS Collaboration (2015). Measurement of the production cross section ratio σ(χb2(1P))/σ(χb1(1P)) in pp collisions at √s=8TeV. Physics Letters, Section B, 743, 383-402. doi:10.1016/j.physletb.2015.02.048 | en_US |
| dc.identifier.doi | 10.1016/j.physletb.2015.02.048 | en_US |
| dc.identifier.doi | 10.1016/j.physletb.2015.02.048 | |
| dc.identifier.issn | 0370-2693 | |
| dc.identifier.scopus | 2-s2.0-84924995960 | |
| dc.identifier.uri | http://doi.org/10.1016/j.physletb.2015.02.048 | |
| dc.identifier.uri | https://hdl.handle.net/11147/5929 | |
| dc.language.iso | en | en_US |
| dc.publisher | Elsevier Ltd. | en_US |
| dc.relation.ispartof | Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics | en_US |
| dc.rights | info:eu-repo/semantics/openAccess | en_US |
| dc.subject | Large Hadron Collider (LHC) | en_US |
| dc.subject | Compact Muon Solenoid | en_US |
| dc.subject | Quarkonium production | en_US |
| dc.subject | Bottomonium | en_US |
| dc.title | Measurement of the Production Cross Section Ratio Sigma(chi B2(1p))/Sigma(chi B1(1p)) in Pp Collisions at Root S=8tev | en_US |
| dc.type | Article | en_US |
| dspace.entity.type | Publication | |
| gdc.author.institutional | Karapınar, Güler | |
| gdc.coar.access | open access | |
| gdc.coar.type | text::journal::journal article | |
| gdc.collaboration.industrial | false | |
| gdc.description.department | İzmir Institute of Technology. Mathematics | en_US |
| gdc.description.endpage | 402 | en_US |
| gdc.description.publicationcategory | Makale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı | en_US |
| gdc.description.scopusquality | Q1 | |
| gdc.description.startpage | 383 | en_US |
| gdc.description.volume | 743 | en_US |
| gdc.description.wosquality | Q1 | |
| gdc.identifier.openalex | W1524187201 | |
| gdc.identifier.wos | WOS:000352147500058 | |
| gdc.index.type | WoS | |
| gdc.index.type | Scopus | |
| gdc.openalex.collaboration | International | |
| gdc.openalex.fwci | 1.99048739 | |
| gdc.openalex.normalizedpercentile | 0.96 | |
| gdc.plumx.crossrefcites | 16 | |
| gdc.plumx.mendeley | 178 | |
| gdc.scopus.citedcount | 26 | |
| gdc.wos.citedcount | 13 | |
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