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[PDF] Top 20 Search For High-mass Z Gamma Resonances In E(+)e(-)gamma And Mu(+)mu(-)gamma Final States In Proton-proton Collisions At Root S=8 And 13 Tev

Has 10000 "Search For High-mass Z Gamma Resonances In E(+)e(-)gamma And Mu(+)mu(-)gamma Final States In Proton-proton Collisions At Root S=8 And 13 Tev" found on our website. Below are the top 20 most common "Search For High-mass Z Gamma Resonances In E(+)e(-)gamma And Mu(+)mu(-)gamma Final States In Proton-proton Collisions At Root S=8 And 13 Tev".

Search For High-mass Z Gamma Resonances In E(+)e(-)gamma And Mu(+)mu(-)gamma Final States In Proton-proton Collisions At Root S=8 And 13 Tev

Search For High-mass Z Gamma Resonances In E(+)e(-)gamma And Mu(+)mu(-)gamma Final States In Proton-proton Collisions At Root S=8 And 13 Tev

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

34

Search for high-mass Z gamma resonances in proton-proton collisions at root s=8 and 13 TeV using jet substructure techniques

Search for high-mass Z gamma resonances in proton-proton collisions at root s=8 and 13 TeV using jet substructure techniques

... postulated in theories beyond the standard model (SM), are a cornerstone of the CERN LHC physics ...for resonances decaying into a pair of massive SM gauge bosons (WW, WZ, ZZ, with the most recent results ... See full document

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Search for high-mass Z$\gamma$ resonances in $\mathrm{ e }^{+}\mathrm{ e }^{-}\gamma $ and $ \mu^{+}\mu^{-}\gamma$ final states in proton-proton collisions at $\sqrt{s} =$ 8 and 13 TeV

Search for high-mass Z$\gamma$ resonances in $\mathrm{ e }^{+}\mathrm{ e }^{-}\gamma $ and $ \mu^{+}\mu^{-}\gamma$ final states in proton-proton collisions at $\sqrt{s} =$ 8 and 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

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Search for Narrow High-Mass Resonances in Proton–Proton Collisions at $\sqrt{s}$ = 8 TeV Decaying to a Z and a Higgs Boson

Search for Narrow High-Mass Resonances in Proton–Proton Collisions at $\sqrt{s}$ = 8 TeV Decaying to a Z and a Higgs Boson

... deviations in the observed number of events from the expected background, we set upper limits on the production cross section of a new resonance in the ZH final ...CL s criterion [59, 60] to ... See full document

35

Search for an L-mu - L-tau gauge boson using Z -gt; 4 mu events in proton-proton collisions at root s=13 TeV

Search for an L-mu - L-tau gauge boson using Z -gt; 4 mu events in proton-proton collisions at root s=13 TeV

... one and two standard-deviation bands shown in green and yellow, ...y-axis) and B( ZZ  μμ ) B( Z  → μμ ) (right y-axis) as a function of m ( Z  ) for three ... See full document

25

Search for excited leptons in final states in proton-proton collisions at root s=13 TeV

Search for excited leptons in final states in proton-proton collisions at root s=13 TeV

... acceptance and event selection efficiency of signal events, simu- lated signal samples are generated with pythia ...5 TeV at intervals of 0.25 TeV up to 4 TeV and at ... See full document

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Search for a light charged higgs boson decaying to a W boson and a CP-Odd higgs boson in final states with e mu mu or mu mu mu in proton-proton collisions at root s=13 TeV

Search for a light charged higgs boson decaying to a W boson and a CP-Odd higgs boson in final states with e mu mu or mu mu mu in proton-proton collisions at root s=13 TeV

... selection and the calcu- lated yield from the tight-to-loose ratio method applied to the simulated tt ...used in the calculation. The two values agree within 27% (23%) in the eµµ (µµµ) ...channel. ... See full document

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Search for narrow high-mass resonances in proton-proton collisions at root s=8 TeV decaying to a Z and a Higgs boson

Search for narrow high-mass resonances in proton-proton collisions at root s=8 TeV decaying to a Z and a Higgs boson

... [16] ATLAS Collaboration, Search for Higgs boson pair production in the γ γ bb¯ final √ state using pp collision data at s = 8 TeV from the ATLAS detector, Phys.. High Energy Phys.[r] ... See full document

24

Search for excited quarks in the gamma plus jet final state in proton-proton collisions at root s=8 TeV

Search for excited quarks in the gamma plus jet final state in proton-proton collisions at root s=8 TeV

... uncertainties in JER, PER, JES, PES, FSR, in the correction factors, and in the integrated luminosity are used in the limit setting procedure as nuisance parameters and affect ... See full document

21

Search for leptophobic Z ' bosons decaying into four-lepton final states in proton-proton collisions at root s=8 TeV

Search for leptophobic Z ' bosons decaying into four-lepton final states in proton-proton collisions at root s=8 TeV

... with high p T and two subleading leptons with relatively low p ...m Z  . This feature is generally found for high-mass (m Z  > 1 TeV) samples in the case of mϕ ... See full document

23

Search for pair-produced three-jet resonances in proton-proton collisions at root s=13 TeV

Search for pair-produced three-jet resonances in proton-proton collisions at root s=13 TeV

... scouting and jets þ H T event ...triplet mass in the four search regions are shown in ...The mass distributions expected for a typical gluino decay is shown in magenta, ... See full document

22

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

... uncertainty in this analysis is in the parame- ter R . Its uncertainty is 8% for the dielectron barrel–barrel chan- nel, 10% for the dielectron barrel–endcap channel, and + − 1 5 % for the ... See full document

24

Search for the pair production of light top squarks in the e(+/-)mu(-/+) final state in proton-proton collisions at root s=13 TeV

Search for the pair production of light top squarks in the e(+/-)mu(-/+) final state in proton-proton collisions at root s=13 TeV

... squark mass similar to that of the top quark, the production cross section of the signal process is expected to amount to up to 125 pb, cor- responding to about 15% of the SM tt production cross ...the ... See full document

41

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

... experiment at the LHC in proton-proton collisions at a center- of-mass energy of 13 TeV in ...regions in data without any reliance on ... See full document

47

Search for narrow resonances decaying to dijets in proton-proton collisions at root s=13 TeV

Search for narrow resonances decaying to dijets in proton-proton collisions at root s=13 TeV

... resolution, and tails towards lower mass values primarily from QCD ...gg). Resonances containing gluons, which emit QCD radiation more strongly than quarks, have a more pronounced ...the ... See full document

18

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

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

... A search for new physics in energetic, high-multiplicity final states has been performed using protonproton collision data collected with the CMS detector at a ... See full document

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Search for heavy Majorana neutrinos in $\mu^\pm \mu^\pm+$ jets events in proton-proton collisions at $\sqrt{s}$ = 8 TeV

Search for heavy Majorana neutrinos in $\mu^\pm \mu^\pm+$ jets events in proton-proton collisions at $\sqrt{s}$ = 8 TeV

... follows. In both the low-mass range (40 < m N < 90 GeV) and the high-mass range (m N > 90 GeV) the control region is the same as the signal selection, without the final ... See full document

35

Search for excited quarks of light and heavy flavor in $\gamma +$ jet final states in proton–proton collisions at $\sqrt{s} =$ 13TeV

Search for excited quarks of light and heavy flavor in $\gamma +$ jet final states in proton–proton collisions at $\sqrt{s} =$ 13TeV

... A search is presented for excited quarks of light and heavy flavor that decay to γ + jet final ...experiment in protonproton collisions ats = 13 TeV ... See full document

22

Search for new resonances in $W\gamma$ and $Z\gamma$ final states in $pp$ collisions at $\sqrt s=8$ TeV with the ATLAS detector

Search for new resonances in $W\gamma$ and $Z\gamma$ final states in $pp$ collisions at $\sqrt s=8$ TeV with the ATLAS detector

... role in electron and photon ...material and spans |η| < 3.2. In the region |η| < ...electrons and photons upstream of the ...tector and is located directly outside the ... See full document

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Search for resonances and quantum black holes using dijet mass spectra in proton-proton collisions at root s=8 TeV

Search for resonances and quantum black holes using dijet mass spectra in proton-proton collisions at root s=8 TeV

... A search for resonances and quantum black holes is performed using the dijet mass spectra measured in proton-proton collisions at p ffiffiffi s ¼ 8 ... See full document

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