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@ARTICLE{Collaboration:152784,
      key          = {152784},
      collaboration = {{CMS Collaboration}},
      title        = {{M}easurement of the {Y}(1{S}), {Y}(2{S}), and {Y}(3{S})
                      cross sections in pp collisions at $\sqrt{s} = 7$ {T}e{V}},
      reportid     = {DESY-2013-00305, arXiv:1303.5900. CMS-BPH-11-001.
                      CERN-PH-EP-2012-373},
      year         = {2013},
      note         = {Submitted to Phys. Lett. B},
      abstract     = {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.},
      cin          = {CMS},
      cid          = {I:(DE-H253)CMS-20120731},
      pnm          = {Experiments at LHC (CMS) (POF2-512)},
      pid          = {G:(DE-H253)POF2-LHC-Exp.-(CMS)-20130405},
      experiment   = {EXP:(DE-H253)LHC-Exp-CMS-20150101},
      typ          = {PUB:(DE-HGF)25 / PUB:(DE-HGF)15},
      eprint       = {1303.5900},
      howpublished = {arXiv:1303.5900},
      archivePrefix = {arXiv},
      SLACcitation = {$\%\%CITATION$ = $arXiv:1303.5900;\%\%$},
      url          = {https://bib-pubdb1.desy.de/record/152784},
}