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[PDF] Top 20 Measurement of differential cross sections for inclusive isolated-photon and photon+jets production in proton-proton collisions at $\sqrt{s} =$ 13 TeV

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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

Measurement of differential cross sections for inclusive isolated-photon and photon+jets production in proton-proton collisions at $\sqrt{s} =$ 13 TeV

... colleagues in the CERN accelerator departments for the excellent perfor- mance of the LHC and thank the technical and administrative staffs at CERN and at other CMS ... See full document

39

Measurements of differential cross sections of top quark pair production as a function of kinematic event variables in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Measurements of differential cross sections of top quark pair production as a function of kinematic event variables in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... S. Abdullin, M. Albrow, M. Alyari, G. Apollinari, A. Apresyan, A. Apyan, S. Banerjee, L.A.T. Bauerdick, A. Beretvas, J. Berryhill, P.C. Bhat, G. Bolla † , K. Burkett, J.N. Butler, A. Canepa, G.B. Cerati, ... See full document

56

Measurement of differential cross sections of isolated-photon plus heavy-flavour jet production in pp collisions at $\sqrt{s}=8$ TeV using the ATLAS detector

Measurement of differential cross sections of isolated-photon plus heavy-flavour jet production in pp collisions at $\sqrt{s}=8$ TeV using the ATLAS detector

... immersed in a 2 T axial magnetic field provided by an encompassing thin superconducting solenoid, is located nearest to the beam pipe and comprises a high-granularity pixel detec- tor, a silicon microstrip ... See full document

23

Measurement of quarkonium production cross sections in pp collisions at $\sqrt{s}=$ 13 TeV

Measurement of quarkonium production cross sections in pp collisions at $\sqrt{s}=$ 13 TeV

... colleagues in the CERN accelerator de- partments for the excellent performance of the LHC and thank the technical and administrative staffs at CERN and at other CMS ... See full document

22

Measurement of four-jet production in proton-proton collisions at $\sqrt{s}=7$  TeV

Measurement of four-jet production in proton-proton collisions at $\sqrt{s}=7$  TeV

... clustered in jets due to additional proton-proton interactions within the same bunch crossing ...simulation, and are confirmed with in situ measurements of the energy ... See full document

31

Measurement of four-jet differential cross sections in $\sqrt{s}=8$ TeV proton-proton collisions using the ATLAS detector

Measurement of four-jet differential cross sections in $\sqrt{s}=8$ TeV proton-proton collisions using the ATLAS detector

... LO cross sections and HEJ are normalised by fixed factors to facilitate the comparison of the spectra in the kinematic regions of interest; these factors vary between ...0.6 ... See full document

75

Measurement of the total and differential inclusive $B^+$ hadron cross sections in pp collisions at $\sqrt{s}$ = 13 TeV

Measurement of the total and differential inclusive $B^+$ hadron cross sections in pp collisions at $\sqrt{s}$ = 13 TeV

... S. Abdullin, M. Albrow, G. Apollinari, S. Banerjee, L.A.T. Bauerdick, A. Beretvas, J. Berryhill, P.C. Bhat, G. Bolla, K. Burkett, J.N. Butler, H.W.K. Cheung, F. Chlebana, S. Cihangir † , M. ... See full document

22

Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... feature of the CMS apparatus is a superconducting solenoid of 6 m internal diam- ...pixel and strip tracker, a lead tungstate crystal electromagnetic calorimeter, and a brass and ... See full document

38

Measurement of the top quark pair production cross section in proton-proton collisions at $\sqrt(s) =$ 13 TeV

Measurement of the top quark pair production cross section in proton-proton collisions at $\sqrt(s) =$ 13 TeV

... The measurement of t¯t production at a center-of-mass energy not previously accessed has great discovery poten- tial for physics beyond the standard model (SM), because new phenomena ... See full document

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Measurement of the inclusive jet cross-sections in proton-proton collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector

Measurement of the inclusive jet cross-sections in proton-proton collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector

... ] at the LHC is a multipurpose particle detector with a forward-backward symmetric cylindrical geometry and a near 4π coverage in solid ...consists of an inner tracking detector surrounded by ... See full document

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Measurement of differential cross sections for top quark pair production using the lepton+jets final state in proton-proton collisions at 13 TeV

Measurement of differential cross sections for top quark pair production using the lepton+jets final state in proton-proton collisions at 13 TeV

... J. Wright, 127 S. C. Zenz, 127 J. E. Cole, 128 P. R. Hobson, 128 A. Khan, 128 P. Kyberd, 128 D. Leslie, 128 I. D. Reid, 128 P. Symonds, 128 L. Teodorescu, 128 M. Turner, 128 A. Borzou, 129 K. Call, 129 J. ... See full document

39

Measurement of the cross section for isolated-photon plus jet production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector

Measurement of the cross section for isolated-photon plus jet production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector

... clusters of energy deposited in the EM calorimeter and classified [ 30 ] as uncon- verted photons (candidates without a matching track or matching reconstructed conversion vertex in the inner ... See full document

25

Search for new phenomena with photon+jet events in proton-proton collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector

Search for new phenomena with photon+jet events in proton-proton collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector

... clusters of calorimeter cells using the anti-k t algorithm with radius parameter R = ...0.4. Jets affected by noise or hardware problems in the detector, or identified as arising from non-collision ... See full document

38

Measurements of the electron and muon inclusive cross-sections in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Measurements of the electron and muon inclusive cross-sections in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

... Electron and muon reconstruction in the ATLAS detector The ATLAS detector consists of three main components: an Inner De- tector (ID) tracking system immersed in a 2 T magnetic field, ... See full document

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Ratios of dijet production cross sections as a function of the absolute difference in rapidity between jets in proton-proton collisions at $\sqrt{s}=7$ TeV

Ratios of dijet production cross sections as a function of the absolute difference in rapidity between jets in proton-proton collisions at $\sqrt{s}=7$ TeV

... probe of effects beyond collinear factorization [16]. Only jets with transverse momenta above a minimal value of p min T are ...with at least one pair of jets are denoted as ... See full document

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Measurement of the inclusive isolated prompt photon cross section in pp collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector

Measurement of the inclusive isolated prompt photon cross section in pp collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector

... support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, ... See full document

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Measurement of the inclusive energy spectrum in the very forward direction in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Measurement of the inclusive energy spectrum in the very forward direction in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... Particle production at very forward rapidities ( | η | > 5) in high energy hadronic collisions re- ceives contributions from multiparton interactions (MPI), initial- and final-state ... See full document

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Measurements of integrated and differential cross sections for isolated photon pair production in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

Measurements of integrated and differential cross sections for isolated photon pair production in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

... K. Einsweiler 16 , T. Ekelof 168 , M. El Kacimi 137c , R. El Kosseifi 88 , V. Ellajosyula 88 , M. Ellert 168 , S. Elles 5 , F. Ellinghaus 178 , A.A. Elliot 172 , N. Ellis 32 , J. Elmsheuser 27 , M. Elsing 32 , D. ... See full document

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Measurements of differential jet cross sections in proton-proton collisions at $\sqrt{s}=7$ TeV with the CMS detector

Measurements of differential jet cross sections in proton-proton collisions at $\sqrt{s}=7$ TeV with the CMS detector

... momentum jets in proton-proton collisions are described by quan- tum chromodynamics (QCD) in terms of parton-parton scattering, where the outgoing scat- tered partons ... See full document

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Measurement of electroweak production of a W boson and two forward jets in proton-proton collisions at $ \sqrt{s}=8 $ TeV

Measurement of electroweak production of a W boson and two forward jets in proton-proton collisions at $ \sqrt{s}=8 $ TeV

... influence of the choice of parametric function in the fit result, and it is considered as a source of systematic ...data and simulation in the BDT output distributions, we ... See full document

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