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037 | _ | _ | |a PUBDB-2015-05698 |
041 | _ | _ | |a en |
088 | 1 | _ | |a DESY-PROC-2014-04 |
088 | _ | _ | |a DESY-PROC-2014-04 |2 DESY |
100 | 1 | _ | |a Vincter, Manuella G. |b 0 |
111 | 2 | _ | |a Panic2014 |g Panic2014 |c Hamburg |d 2014-08-25 - 2014-08-29 |w Germany |
245 | _ | _ | |a Measurements of vector-boson production in ATLAS and CMS |
260 | _ | _ | |a Hamburg |c 2014 |b Deutsches Elektronen-Synchrotron, DESY |
300 | _ | _ | |a 473-476 |
336 | 7 | _ | |a Conference Paper |0 33 |2 EndNote |
336 | 7 | _ | |a conferenceObject |2 DRIVER |
336 | 7 | _ | |a Contribution to a conference proceedings |b contrib |m contrib |0 PUB:(DE-HGF)8 |s 1450094072_7046 |2 PUB:(DE-HGF) |
336 | 7 | _ | |a Internal Report |0 PUB:(DE-HGF)15 |2 PUB:(DE-HGF) |m intrep |
336 | 7 | _ | |a INPROCEEDINGS |2 BibTeX |
520 | _ | _ | |a Vector-boson production in $p-p$ collisions in LHC Run-1 has been extensively studied by ATLAS and CMS. Charged andneutral-current Drell-Yan cross sections are sensitive to the parton distribution functions of the proton andelectroweak corrections. The measurements of the neutral-current Drell-Yan process in three distinct kinematicregions, i.e. at the $Z$ boson mass peak, below, and above, are performed. The results are compared to NLO Monte Carlosimulations and to NNLO QCD predictions corrected for NLO EW effects calculated using various parameterisations of theparton distribution functions. An overview of these results is given. |
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588 | _ | _ | |a Dataset connected to DataCite, INSPIRE |
650 | _ | 7 | |a talk: Hamburg 2014/08/24 |2 INSPIRE |
650 | _ | 7 | |a p p: scattering |2 INSPIRE |
650 | _ | 7 | |a p p: colliding beams |2 INSPIRE |
650 | _ | 7 | |a parton: distribution function |2 INSPIRE |
650 | _ | 7 | |a vector boson: hadroproduction |2 INSPIRE |
650 | _ | 7 | |a electroweak interaction: correction |2 INSPIRE |
650 | _ | 7 | |a p: distribution function |2 INSPIRE |
650 | _ | 7 | |a Z0: mass |2 INSPIRE |
650 | _ | 7 | |a Drell-Yan process |2 INSPIRE |
650 | _ | 7 | |a neutral current |2 INSPIRE |
650 | _ | 7 | |a ATLAS |2 INSPIRE |
650 | _ | 7 | |a CMS |2 INSPIRE |
650 | _ | 7 | |a quantum chromodynamics: perturbation theory |2 INSPIRE |
650 | _ | 7 | |a higher-order |2 INSPIRE |
650 | _ | 7 | |a CERN LHC Coll |2 INSPIRE |
650 | _ | 7 | |a numerical calculations: Monte Carlo |2 INSPIRE |
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650 | _ | 7 | |a experimental results |2 INSPIRE |
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700 | 1 | _ | |a ATLAS Collaboration |0 P:(DE-HGF)0 |b 1 |e Collaboration author |
700 | 1 | _ | |a CMS Collaboration |0 P:(DE-HGF)0 |b 2 |e Collaboration author |
773 | _ | _ | |a 10.3204/DESY-PROC-2014-04/213 |
787 | 0 | _ | |a Schmidt, Alexander et.al. |d Hamburg : Deutsches Elektronen-Synchrotron, DESY, Hamburg, 2014 |i IsPartOf |0 PUBDB-2015-03603 |r DESY-PROC-2014-04 |t Proceedings, 20th International Conference on Particles and Nuclei (PANIC 14) |
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