[PDF] Top 20 Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at $ \sqrt{s}=13 $ TeV
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Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at $ \sqrt{s}=13 $ TeV
... Republic of Ko- rea; the Lithuanian Academy of Sciences; the Ministry of Education, and University of Malaya (Malaysia); the Mexican Funding Agencies (BUAP, CINVESTAV, ... See full document
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Measurement of $WZ$ production in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
... are the only significant source of background that does not contain a Z bo- ...enriched in t¯ t background events is defined by changing the charge combination of the ... See full document
27
Measurement of charged-particle distributions sensitive to the underlying event in $ \sqrt{s}=13 $ TeV proton-proton collisions with the ATLAS detector at the LHC
... observables the models describe the underlying-event data to better than 5% ...level of variation is far greater than the experimental uncertainty of the ... See full document
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Measurement of distributions sensitive to the underlying event in inclusive Z-boson production in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
... C. Goeringer 82 , S. Goldfarb 88 , T. Golling 177 , D. Golubkov 129 , A. Gomes 125a,125b,125d , L.S. Gomez Fajardo 42 , R. Gonçalo 125a , J. Goncalves Pinto Firmino Da Costa 137 , L. Gonella 21 , S. ... See full document
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Measurement of the differential cross sections for the associated production of a $W$ boson and jets in proton-proton collisions at $\sqrt{s}=13$ TeV
... J. Lykken, 143 K. Maeshima, 143 N. Magini, 143 J. M. Marraffino, 143 S. Maruyama, 143 D. Mason, 143 P. McBride, 143 P. Merkel, 143 S. Mrenna, 143 S. Nahn, 143 V. O ’Dell, 143 K. Pedro, 143 O. ... See full document
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Measurement of differential cross sections for inclusive isolated-photon and photon+jets production in proton-proton collisions at $\sqrt{s} =$ 13 TeV
... physics at the TeV scale. The central fea- ture of the CMS apparatus is a superconducting solenoid of 6 m internal diameter, providing a magnetic field of ...Within ... See full document
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Measurement of the top quark pair production cross section in proton-proton collisions at $\sqrt(s) =$ 13 TeV
... P. Lujan, 155 D. Marlow, 155 T. Medvedeva, 155 M. Mooney, 155 J. Olsen, 155 C. Palmer, 155 P. Piroué, 155 H. Saka, 155 D. Stickland, 155 C. Tully, 155 A. Zuranski, 155 S. Malik, 156 V. E. Barnes, 157 D. Benedetti, ... See full document
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Measurement of the double-differential inclusive jet cross section in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $
... Predictions of perturbative quantum chromodynamics at next-to-leading order pre- cision, complemented with electroweak and nonperturbative corrections, are used to compute the absolute scale and ... See full document
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Measurement of inclusive jet and dijet cross-sections in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
... ] at the LHC is a multi-purpose particle detector with a forward-backward symmetric cylindrical geometry and a near 4π coverage in solid ...consists of an inner track- ing detector, ... See full document
48
Measurement of electroweak production of a W boson and two forward jets in proton-proton collisions at $ \sqrt{s}=8 $ TeV
... from the primary vertex are not considered for jet clustering ...on the energy ratio between the charged and neu- tral hadrons within the jet cone [51], is also applied in order to ... See full document
36
Measurement of inclusive W and Z boson production cross sections in pp collisions at $\sqrt{s}$ = 8 TeV
... feature of the CMS apparatus is a superconducting solenoid, of 6 m internal diame- ter, providing a field of ...Within the field volume are a silicon pixel and strip tracker, a crys- ... See full document
31
Measurement of the production cross-section of a single top quark in association with a Z boson in proton–proton collisions at 13 TeV with the ATLAS detector
... R.F.H. Hunter 31 , P. Huo 150 , N. Huseynov 68,b , J. Huston 93 , J. Huth 59 , R. Hyneman 92 , G. Iacobucci 52 , G. Iakovidis 27 , I. Ibragimov 143 , L. Iconomidou-Fayard 119 , Z. Idrissi 137e , P. Iengo 32 , O. ... See full document
35
Search for long-lived charged particles in proton-proton collisions at $\sqrt s=$ 13 TeV
... with the underlying event tune CUETP8M1 [38] , is used to generate the 13 TeV MC ...samples. The fraction, f, of produced ~g hadronizing into a ~g-gluon state is an ... See full document
23
Measurement of $b$-hadron pair production with the ATLAS detector in proton-proton collisions at $\sqrt{s}=8$ TeV
... A.A. O’Rourke 45 , V. O’Shea 56 , F.G. Oakham 31,d , H. Oberlack 103 , T. Obermann 23 , J. Ocariz 83 , A. Ochi 70 , I. Ochoa 38 , J.P. Ochoa-Ricoux 34a , S. Oda 73 , S. Odaka 69 , H. Ogren 64 , A. Oh 87 , ... See full document
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Combined search for electroweak production of charginos and neutralinos in proton-proton collisions at $\sqrt{s} =$ 13 TeV
... combination of several searches for the electroweak production of charginos and neutralinos is ...use proton-proton collision data at √ s = 13 TeV, ... See full document
46
Search for standard model production of four top quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV
... t production, which is simulated at NLO using powheg v2 [17–20] .... The events com- ing from Drell–Yan (qq → Z / γ ∗ → + − , with = e or μ ) + jets and W boson + jets ... See full document
23
Measurement of the cross section for top quark pair production in association with a W or Z boson in proton-proton collisions at $\sqrt{s} =$ 13 TeV
... with the higher integrated luminosity collected at 13 TeV collisions, allows for a much more ac- curate study of these ...measurements of the production ... See full document
46
Search for single production of a vector-like T quark decaying to a Z boson and a top quark in proton-proton collisions at $\sqrt s$ = 13 TeV
... colleagues in the CERN accelerator depart- ments for the excellent performance of the LHC and thank the technical and administrative staffs at CERN and at other CMS ... See full document
27
Jet and underlying event properties as a function of charged-particle multiplicity in proton–proton collisions at $\sqrt{s}$ = 7 TeV
... multi-particle production in pp collisions at LHC energies provide a clear indication that our understanding of the different components contributing to the to- tal ... See full document
43
Measurement of the inclusive jet cross-sections in proton-proton collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector
... J. Jimenez Pena 170 , S. Jin 35a , A. Jinaru 28b , O. Jinnouchi 159 , H. Jivan 147c , P. Johansson 141 , K.A. Johns 7 , C.A. Johnson 64 , W.J. Johnson 140 , K. Jon-And 148a,148b , R.W.L. Jones 75 , S.D. Jones 151 ... See full document
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