001     152784
005     20211110121933.0
024 7 _ |a arXiv:1303.5900
|2 arXiv
024 7 _ |a altmetric:1320870
|2 altmetric
024 7 _ |a inspire:1225274
|2 inspire
037 _ _ |a DESY-2013-00305
088 1 _ |a arXiv:1303.5900; CMS-BPH-11-001; CERN-PH-EP-2012-373
088 _ _ |a arXiv:1303.5900
|2 arXiv
088 _ _ |a CMS-BPH-11-001
|2 CMS
088 _ _ |a CERN-PH-EP-2012-373
|2 CERN
100 1 _ |a CMS Collaboration
|0 P:(DE-HGF)0
|b 0
|e Collaboration author
245 _ _ |a Measurement of the Y(1S), Y(2S), and Y(3S) cross sections in pp collisions at $\sqrt{s} = 7$ TeV
260 _ _ |c 2013
336 7 _ |a preprint
|2 DRIVER
336 7 _ |a Electronic Article
|0 28
|2 EndNote
336 7 _ |a Preprint
|b preprint
|m preprint
|0 PUB:(DE-HGF)25
|s 152784
|2 PUB:(DE-HGF)
336 7 _ |a ARTICLE
|2 BibTeX
336 7 _ |a Internal Report
|0 PUB:(DE-HGF)15
|2 PUB:(DE-HGF)
|m intrep
500 _ _ |a Submitted to Phys. Lett. B
520 _ _ |a The Upsilon(1S), Upsilon(2S), and Upsilon(3S) production cross sections are measured using a data sample corresponding to an integrated luminosity of 35.8 +/-1.4 inverse picobarns of proton-proton collisions at sqrt(s) = 7 TeV, collected with the CMS detector at the LHC. The Upsilon resonances are identified through their decays to dimuons. Integrated over the Upsilon transverse momentum range pt[Upsilon] < 50\GeV and rapidity range abs(y[Upsilon]) < 2.4, and assuming unpolarized Upsilon production, the products of the Upsilon production cross sections and dimuon branching fractions are sigma(pp to Upsilon(1S) X) B(Upsilon(1S) to mu+ mu-) = (8.55 +/- 0.05 +0.56/-0.50 +/- 0.34) nb, sigma(pp to Upsilon(2S) X) B(Upsilon(2S) to mu+ mu-) = (2.21 +/- 0.03 +0.16/-0.14 +/- 0.09) nb, sigma(pp to Upsilon(3S) X) B(Upsilon(3S) to mu+ mu-) = (1.11 +/- 0.02 +0.10/-0.08 +/- 0.04) nb, where the first uncertainty is statistical, the second is systematic, and the third is from the uncertainty in the integrated luminosity. The differential cross sections in bins of transverse momentum and rapidity, and the cross section ratios are presented. Cross section measurements performed within a restricted muon kinematic range and not corrected for acceptance are also provided. These latter measurements are independent of Upsilon polarization assumptions. The results are compared to theoretical predictions and previous measurements.
536 _ _ |a Experiments at LHC (CMS) (POF2-512)
|0 G:(DE-H253)POF2-LHC-Exp.-(CMS)-20130405
|c POF2-512
|f POF II
|x 0
588 _ _ |a Dataset connected to
693 _ _ |a LHC
|e LHC: CMS
|1 EXP:(DE-588)4398783-7
|0 EXP:(DE-H253)LHC-Exp-CMS-20150101
|5 EXP:(DE-H253)LHC-Exp-CMS-20150101
|x 0
856 4 _ |u https://bib-pubdb1.desy.de/record/152784/files/DESY-2013-00305.pdf
|y OpenAccess
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|y OpenAccess
909 C O |o oai:bib-pubdb1.desy.de:152784
|p openaire
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910 1 _ |a Deutsches Elektronen-Synchrotron
|0 I:(DE-588b)2008985-5
|k DESY
|b 0
|6 P:(DE-HGF)0
913 1 _ |b Struktur der Materie
|l Elementarteilchenphysik
|1 G:(DE-HGF)POF2-510
|0 G:(DE-HGF)POF2-512
|2 G:(DE-HGF)POF2-500
|v LHC
|9 G:(DE-H253)POF2-LHC-Exp.-(CMS)-20130405
|x 0
|4 G:(DE-HGF)POF
|3 G:(DE-HGF)POF2
|a DE-H253CMS
914 1 _ |y 2013
915 _ _ |a OpenAccess
|0 StatID:(DE-HGF)0510
|2 StatID
915 _ _ |a Published
|0 StatID:(DE-HGF)0580
|2 StatID
920 1 _ |0 I:(DE-H253)CMS-20120731
|k CMS
|l LHC/CMS Experiment
|x 0
980 _ _ |a preprint
980 _ _ |a VDB
980 _ _ |a UNRESTRICTED
980 _ _ |a FullTexts
980 _ _ |a intrep
980 _ _ |a I:(DE-H253)CMS-20120731
980 1 _ |a FullTexts


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