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[PDF] Top 20 Search for dijet resonances in proton–proton collisions at $\sqrt{s}$ = 13 TeV and constraints on dark matter and other models

Has 10000 "Search for dijet resonances in proton–proton collisions at $\sqrt{s}$ = 13 TeV and constraints on dark matter and other models" found on our website. Below are the top 20 most common "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

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

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

... GeV and lifetimes from 1 ns to 10 µs are produced with PYTHIA ...spectrum and the decay tables are calculated using ISASUSY with ISAJET ...production and the acceptance of the search for ... See full document

39

Search for high-mass resonances in dilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for high-mass resonances in dilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... A search is presented for new high-mass resonances decaying into electron or muon ...The search uses proton-proton collision data at a centre-of-mass energy of 13 ... See full document

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Search for dark matter particles in proton-proton collisions at $ \sqrt{s}=8 $ TeV using the razor variables

Search for dark matter particles in proton-proton collisions at $ \sqrt{s}=8 $ TeV using the razor variables

... reconstruct and identify individual particles with an optimized combination of information from the various elements of the CMS detec- ...momentum at the primary interaction vertex as measured by the ... See full document

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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

... known matter only comprises about 5% of the total energy content of the universe, with 27% contributed by dark matter (DM) and the rest being dark energy ...DM and standard model ... See full document

42

Search for dark matter produced in association with heavy-flavor quark pairs in proton-proton collisions at $\sqrt{s}=13$ TeV

Search for dark matter produced in association with heavy-flavor quark pairs in proton-proton collisions at $\sqrt{s}=13$ TeV

... A search for an excess of events with large missing transverse momentum (p miss T ) produced in association with a pair of heavy-flavor quarks has been performed with a sample of proton- ... See full document

50

Search for narrow resonances in the b-tagged dijet mass spectrum in proton-proton collisions at $\sqrt{s} =$ 8 TeV

Search for narrow resonances in the b-tagged dijet mass spectrum in proton-proton collisions at $\sqrt{s} =$ 8 TeV

... each other, as they vary in sensitivity to different production and decay mechanisms of new, light ...first search for b ¯b resonances with masses as low as 325 GeV, ...generic ... See full document

19

Search for pair-produced resonances decaying to quark pairs in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for pair-produced resonances decaying to quark pairs in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... A search has been performed for the pair production of diquark resonances in two-jet events in a boosted jet topology and in four-jet events in a resolved jet ...from ... See full document

25

Search for narrow resonances in dilepton mass spectra in proton-proton collisions at $\sqrt{s}$ = 13 TeV and combination with 8 TeV data

Search for narrow resonances in dilepton mass spectra in proton-proton collisions at $\sqrt{s}$ = 13 TeV and combination with 8 TeV data

... 8 TeV data in ...positive and uniform, as this is known to result in good frequentist coverage ...Limits on Rσ are evaluated for scenarios in which the hypothetical particle is ... See full document

24

Search for pair-produced resonances each decaying into at least four quarks in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for pair-produced resonances each decaying into at least four quarks in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... estimates. In summary, a search has been conducted at the LHC for light pair-produced resonances that each decay into at least four ...limits on R- parity-violating supersymmetry ... See full document

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Search for low mass vector resonances decaying into quark-antiquark  pairs in proton-proton collisions at $\sqrt{s} =$ 13 TeV

Search for low mass vector resonances decaying into quark-antiquark pairs in proton-proton collisions at $\sqrt{s} =$ 13 TeV

... including models with extra dimensions or with new gauge sym- metries, amongst others, predict the existence of leptopho- bic vector or axial-vector mediators that couple to SM quarks (q) ...as resonances ... See full document

24

Search for low mass vector resonances decaying into quark-antiquark pairs in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Search for low mass vector resonances decaying into quark-antiquark pairs in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... = 13 TeV with the CMS detector at the LHC, corresponding to an integrated lu- minosity of ...background in the distribution of the invariant mass of the jet, using novel jet sub- structure ... See full document

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Search for low-mass resonances decaying into bottom quark-antiquark pairs in proton-proton collisions at $\sqrt{s} =$ 13 TeV

Search for low-mass resonances decaying into bottom quark-antiquark pairs in proton-proton collisions at $\sqrt{s} =$ 13 TeV

... A search for narrow, low-mass, scalar, and pseudoscalar resonances decaying to bottom quark-antiquark pairs is ...The search is based on events recorded in p ffiffiffi s ¼ ... See full document

25

Search for high-mass $\mathrm{ Z }\gamma$ resonances in proton-proton collisions at $\sqrt{s}=$ 8 and 13 TeV using jet substructure techniques

Search for high-mass $\mathrm{ Z }\gamma$ resonances in proton-proton collisions at $\sqrt{s}=$ 8 and 13 TeV using jet substructure techniques

... feature in a variety of proposed theoretical extensions of the ...12], and little Higgs [13] models, as well other beyond the SM ...important, and yet to be established, decay of ... See full document

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Search for leptoquarks coupled to third-generation quarks in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for leptoquarks coupled to third-generation quarks in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... quark and a muon, BðLQ → tμÞ ¼ 1, are excluded at 95% ...a search for supersymmetry [96] , by more than 600 ...[48] and LQ → bν [49] decay channels to set exclusions limits in the plane ... See full document

19

Search for black holes and sphalerons in high-multiplicity final states in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Search for black holes and sphalerons in high-multiplicity final states in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... theoretical models of physics beyond the standard model (SM) [1–3] predict strong pro- duction of particles decaying into high-multiplicity final states, ...these models are supersymmetry [4–11], with or ... See full document

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Search for narrow resonances decaying to dijets in proton-proton collisions at $\sqrt(s) =$ 13 TeV

Search for narrow resonances decaying to dijets in proton-proton collisions at $\sqrt(s) =$ 13 TeV

... resonance in the data, as seen from Fig. 1. The most signifi- cant excess in the data relative to the background fit occurs for a dijet mass of ...bin at 3.9 TeV and neighboring ... See full document

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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 Zealand; the ... See full document

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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

... produced at high rates in proton-proton collisions at the CERN LHC through pointlike scattering of quarks and ...quarks and gluons from that predicted by ... See full document

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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

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