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[PDF] Top 20 Search for new physics in dijet angular distributions using proton-proton collisions at root s=13 TeV and constraints on dark matter and other models

Has 10000 "Search for new physics in dijet angular distributions using proton-proton collisions at root s=13 TeV and constraints on dark matter and other models" found on our website. Below are the top 20 most common "Search for new physics in dijet angular distributions using proton-proton collisions at root s=13 TeV and constraints on dark matter and other models".

Search for new physics in dijet angular distributions using proton-proton collisions at root s=13 TeV and constraints on dark matter and other models

Search for new physics in dijet angular distributions using proton-proton collisions at root s=13 TeV and constraints on dark matter and other models

... LHC and thank the technical and administrative staffs at CERN and at other CMS institutes for their contributions to the success of the CMS ...effort. In addition, we ... See full document

27

Search for narrow and broad dijet resonances in proton-proton collisions at root s=13 TeV and constraints on dark matter mediators and other new particles

Search for narrow and broad dijet resonances in proton-proton collisions at root s=13 TeV and constraints on dark matter mediators and other new particles

... based on events with dijets reconstructed at the trigger level from calorimeter ...high-mass search, for resonances with masses above 1.6 TeV, is performed using dijets reconstructed ... See full document

58

Search for narrow and broad dijet resonances in proton-proton collisions at $ \sqrt{s}=13 $ TeV and constraints on dark matter mediators and other new particles

Search for narrow and broad dijet resonances in proton-proton collisions at $ \sqrt{s}=13 $ TeV and constraints on dark matter mediators and other new particles

... Education, and University of Malaya (Malaysia); the Mexican Funding Agencies (BUAP, CINVESTAV, CONACYT, LNS, SEP, and UASLP-FAI); the Ministry of Business, Innovation and Employment, New ... See full document

54

Search for quark contact interactions and extra spatial dimensions using dijet angular distributions in proton-proton collisions at root s=8 TeV

Search for quark contact interactions and extra spatial dimensions using dijet angular distributions in proton-proton collisions at root s=8 TeV

... process and exhibits behavior similar to Rutherford scatter- ing, characteristic of spin-1 particle ...of new physics (NP), such as quark contact interactions (CI) or virtual ex- change of ... See full document

22

Search for supersymmetric partners of electrons and muons in proton-proton collisions at root s=13 TeV

Search for supersymmetric partners of electrons and muons in proton-proton collisions at root s=13 TeV

... generated at LO with mcfm 7.0 [ 32 ], and all other diboson production processes [ 33 , 34 ], and tt [ 35 ] and the production of single top quark associated with a W bo- son [ 36 ], ... See full document

28

Search for new physics in the monophoton final state in proton-proton collisions at root s=13 TeV

Search for new physics in the monophoton final state in proton-proton collisions at root s=13 TeV

... Proton-proton collisions producing large missing transverse momentum and a high trans- verse momentum photon have been investigated to search for new phenomena, using a ... See full document

39

Search for excited leptons in proton-proton collisions at root s=8 TeV

Search for excited leptons in proton-proton collisions at root s=8 TeV

... particle physics describes the observed phenomena very suc- cessfully, however it provides no explanation for the three generations of the fermion fam- ...of models postulating that quarks and ... See full document

55

Search for new physics in the monophoton final state in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Search for new physics in the monophoton final state in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... Proton-proton collisions producing large missing transverse momentum and a high transverse momentum photon have been investigated to search for new phenomena, using a data ... See full document

36

Search For Dark Matter And Unparticles In Events With A Z Boson And Missing Transverse Momentum In Proton-proton Collisions At Root S=13 Tev

Search For Dark Matter And Unparticles In Events With A Z Boson And Missing Transverse Momentum In Proton-proton Collisions At Root S=13 Tev

... A search for dark matter and unparticle production at the LHC has been performed using events containing two charged leptons (electrons or muons), consistent with the decay of a ... See full document

46

Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... dominant in the region of low E miss T ...particles, and therefore the measured E T miss arises from limited detector acceptance and mismeasurement of particle ...events in a ... See full document

42

Search for new physics in top quark production in dilepton final states in proton-proton collisions at root s=13 TeV

Search for new physics in top quark production in dilepton final states in proton-proton collisions at root s=13 TeV

... The search is sensitive to new physics contributions to tW and t¯t production, and the six effective couplings, C G , C (3) φq , C tW , C tG , C uG , and C cG , are constrained ... See full document

30

Search for dark matter produced in association with heavy-flavor quark pairs in proton-proton collisions at root s=13 TeV

Search for dark matter produced in association with heavy-flavor quark pairs in proton-proton collisions at root s=13 TeV

... mass, and v = 246 GeV is the Higgs field vacuum expectation ...LHC Dark Matter Working Group [ 47 ], g q is taken to be flavor uni- versal and equal to ...1 and is independent of the DM ... See full document

37

Search for dijet resonances in proton–proton collisions at $\sqrt{s}$ = 13 TeV and constraints on dark matter and other models

Search for dijet resonances in proton–proton collisions at $\sqrt{s}$ = 13 TeV and constraints on dark matter and other models

... 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

23

Search for new physics in dijet angular distributions using proton–proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models

Search for new physics in dijet angular distributions using proton–proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models

... 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

38

Search for new physics with dijet angular distributions in proton-proton collisions at root S = 13 TeV

Search for new physics with dijet angular distributions in proton-proton collisions at root S = 13 TeV

... program and the European Research Council and EPLANET (European Union); the Leventis Foundation; the ...Youth and Sports (MEYS) of the Czech Republic; the Council of Science and Industrial ... See full document

37

Search for new physics with dijet angular distributions in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Search for new physics with dijet angular distributions in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... In models with large ED, the fundamental Planck scale can be comparable to the electroweak scale, which can make black hole production possible at the LHC ...scale and decay into multijets ... See full document

34

Constraints on the pMSSM, AMSB model and on other models from the search for long-lived charged particles in proton-proton collisions at root s=8 TeV

Constraints on the pMSSM, AMSB model and on other models from the search for long-lived charged particles in proton-proton collisions at root s=8 TeV

... present constraints on the pMSSM and the AMSB model, obtained using the results from the search for heavy stable charged particles (HSCP) in protonproton ... See full document

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Search for disappearing tracks in proton-proton collisions at root s=8 TeV

Search for disappearing tracks in proton-proton collisions at root s=8 TeV

... uncertainties in the integrated luminosity and in the signal efficiency are constrained with log-normal ...uncertainties in the background estimates, and they are specified sepa- rately ... See full document

44

Search for Z gamma resonances using leptonic and hadronic final states in proton-proton collisions at root s=13 TeV

Search for Z gamma resonances using leptonic and hadronic final states in proton-proton collisions at root s=13 TeV

... MSES and CSF (Croatia); RPF (Cyprus); SENESCYT (Ecuador); MoER, ERC IUT, and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF ... See full document

44

Combined search for electroweak production of charginos and neutralinos in proton-proton collisions at root s=13 TeV

Combined search for electroweak production of charginos and neutralinos in proton-proton collisions at root s=13 TeV

... used in the various searches to estimate the background from some SM processes, to assess systematic uncertainties in prediction methods that rely on data, and to calculate the selection ... See full document

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