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[PDF] Top 20 ttH production at 13 TeV (CMS)

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ttH production at 13 TeV (CMS)

ttH production at 13 TeV (CMS)

... The H → γγ channel has a small branching ratio of 0.2%, but o ff ers a very clean final state [5]. The excellent photon identification and energy resolution enables a precise reconstruction of the diphoton invariant mass ... See full document

6

Inclusive Searches for Supersymmetry at √s = 13 TeV Using Razor Kinematic Variables, and Data Scouting Using the CMS Trigger System

Inclusive Searches for Supersymmetry at √s = 13 TeV Using Razor Kinematic Variables, and Data Scouting Using the CMS Trigger System

... 316 of 18.8 fb −1 . The novel technique of data scouting was 317 used; by reducing the information stored per event, multijet 318 events could be collected in sufficiently large samples that a 319 sensitive search for ... See full document

313

First results on precision constraints on Z - Z′ mixing with ATLAS and CMS diboson production data at the LHC at 13 TeV and predictions for Run II

First results on precision constraints on Z - Z′ mixing with ATLAS and CMS diboson production data at the LHC at 13 TeV and predictions for Run II

... The exclusion region has been significantly extended compared to that obtained from the previous analysis performed with Tevatron data, as well as with LHC data collected at 7 and 8 TeV. Also, we found that these ... See full document

8

Multiple production up to √s = 13 TeV with the generator GHOST adapted to cosmic ray simulation

Multiple production up to √s = 13 TeV with the generator GHOST adapted to cosmic ray simulation

... The energy dependence in the Fig. 6 of the total mean charged multiplicity (NSD component) is shown hereafter adding to the S p ¯pS collider measurements [1] the data of CMS and TOTEM at √ s = 8 TeV. An ... See full document

6

Naturalness Confronts Nature: Searches for Supersymmetry with the CMS Detector in pp Collisions at √s = 8 and 13 TeV

Naturalness Confronts Nature: Searches for Supersymmetry with the CMS Detector in pp Collisions at √s = 8 and 13 TeV

... As discussed in Sec. 3.8, models of SUSY predict additional, undiscovered fundamental particles which correspond to the heavy superpartners of SM particles. Of particular interest is the production of top squarks, ... See full document

297

Measurement of the J/ψ pair production cross section in pp collisions at s=13 TeV

Measurement of the J/ψ pair production cross section in pp collisions at s=13 TeV

... the CMS collabo- ration, J/ψ + W [50] and J/ψ + Z [51] by the ATLAS collaboration, and double charm [52], Z + open charm [53] and Υ + open charm [54] by the LHCb ...pair production has been measured in pp ... See full document

38

Top-Quark pT-Spectra at LHC and Flavor Independence of z-Scaling

Top-Quark pT-Spectra at LHC and Flavor Independence of z-Scaling

... top-quark production obtained in pp collisions at the LHC energies √ s = 7, 8 and 13 TeV in the central rapidity ...the CMS [9–11] and ATLAS [12, 13] ...inclusive production ... See full document

6

Z/W + jets production at 8/13 TeV in CMS

Z/W + jets production at 8/13 TeV in CMS

... jets production are reviewed based on mostly 8 TeV and 13 TeV proton-proton (pp) collisions data recorded by the Compact Muon Solenoid (CMS) detector [1] at the CERN Large Hadron ... See full document

6

First CMS results at 13 TeV

First CMS results at 13 TeV

... at CMS [1] include the probe of the underlying QCD processes, obtained by measuring b-hadron production cross-section and quarkonium polarization and by looking for new and exotic ...the production ... See full document

6

First 13 TeV results from CMS

First 13 TeV results from CMS

... A search for narrow resonances decaying into a pair of jets has been performed using 42 pb −1 of pp collisions at √ s = 13 TeV. The dijet invariant mass distribution is measured to be a smoothly falling ... See full document

8

Measurements of hadron production at CMS

Measurements of hadron production at CMS

... Phenomenological parameterizations with an exponen- tial shape fit the data significantly better than with a Gaus- sian shape. The parameters , radius and correlation strength, extracted from fits using an exponential ... See full document

8

QCD with jets and heavy flavour in pp and PbPb collisions in ATLAS

QCD with jets and heavy flavour in pp and PbPb collisions in ATLAS

... The Large Hadron Collider (LHC) is the energy frontier of high energy particle physics, providing the highest energy and highest luminosity environment for proton-proton (pp) and heavy ion (HI) colli- sions to date. ... See full document

6

V+jets production at the CMS

V+jets production at the CMS

... [8] Chatrchyan, S. et al. (CMS Collaboration), Phys. Rev. Lett. 109, 251801 (2012). [9] Chatrchyan, S. et al. (CMS Collaboration), CMS-PAS-FSQ-12-022 (2012). [10] Chatrchyan, S. et al. (CMS ... See full document

7

Beyond the standard model searches with b jets and hadronically decaying τ leptons with the ATLAS detector

Beyond the standard model searches with b jets and hadronically decaying τ leptons with the ATLAS detector

... Resonant Higgs pair-production can occur through the creation of a spin-2 Kaluza Klein (KK) Graviton in Warped Extra Dimension (WED) models and can provide a solution to the Planck-weak hierarchy problem of the ... See full document

207

Measurement of top quark polarization in $tt$ $lepton+jets$ final states

Measurement of top quark polarization in $tt$ $lepton+jets$ final states

... We simulate t t ¯ events at the next-to-leading-order (NLO) in perturbative QCD with the mc@nlo event generator version 3.4 [22] and at the leading-order (LO) with alpgen event generator version 2.11 [23]. Parton ... See full document

9

Exclusive production of W pairs in CMS

Exclusive production of W pairs in CMS

... exclusive production of W pairs in the LHC with data collected by the Compact Muon Solenoid detector in proton-proton collisions at √ s = 7 ...two-photon production of a W pairs, pp → p W + W − p → p νe ± ... See full document

8

Heavy Meson Production and Spectroscopy at CMS

Heavy Meson Production and Spectroscopy at CMS

... Besides the results described above, the CMS experiment has also performed other studies of heavy meson production and spectroscopy. For instance, search for possible new bottomonium states decaying into Υπ ... See full document

6

CMS results on collectivity in PbPb collisions at √sNN = 2.76 and 5.02 TeV

CMS results on collectivity in PbPb collisions at √sNN = 2.76 and 5.02 TeV

... Figure 4. The non-linear response coefficients as a function of centrality in PbPb collisions at 2.76 and 5.02 TeV [9]. Statistical (systematic) uncertainties are shown as error bars (shadow boxes). With the lines ... See full document

8

Application of a Convolutional Neural Network for image classification for the analysis of collisions in High Energy Physics

Application of a Convolutional Neural Network for image classification for the analysis of collisions in High Energy Physics

... In a first approach, we have tested the use of convolutional networks for the classification of collisions at LHC using Open Data Monte Carlo samples. The Compact Muon Solenoid (CMS) experiment [5] has pioneered, ... See full document

8

Measurement of the B± production cross section in pp collisions at s=7 and 13 TeV

Measurement of the B± production cross section in pp collisions at s=7 and 13 TeV

... Simulated events are used to optimise the selection, determine some of the efficiencies and estimate the background contamination. The simulation is based on the Pythia8 generator [13] with a specific LHCb ... See full document

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