[PDF] Top 20 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
Has 10000 "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" found on our website. Below are the top 20 most common "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
... RAS and RFBR (Russia); MESTD (Serbia); SEIDI and CPAN (Spain); Swiss Funding Agencies (Switzerland); MST (Taipei); ThEPCenter, IPST, STAR and NSTDA (Thailand); TUBITAK and TAEK (Turkey); NASU ... See full document
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Search for $ \mathrm{t}\overline{\mathrm{t}} $ resonances in highly boosted lepton+jets and fully hadronic final states in proton-proton collisions at $ \sqrt{s}=13 $ TeV
... Youth and Sports (MEYS) of the Czech Republic; the Council of Sci- ence and Industrial Research, India; the HOMING PLUS programme of the Foundation for Polish Science, cofinanced from European Union, ... See full document
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Search for Higgs boson pair production in the $\gamma\gamma\mathrm{b\overline{b}}$ final state in pp collisions at $\sqrt{s}=$ 13 TeV
... system, and the main kine- matic variables used in the analysis are described in detail in .... 8 T. A silicon pixel and strip tracker covering the pseu- dorapidity range | η | ... See full document
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Measurement of the $ \mathrm{ Z } \gamma \rightarrow \nu \bar{\nu} \gamma$ production cross section in pp collisions at $\sqrt{s}=$ 8 TeV and limits on anomalous $ \mathrm{ ZZ } \gamma$ and $ \mathrm{Z} \gamma \gamma$ trilinear gauge boson couplings
... symmetry, and the values of the self-couplings are fixed in the ...model at that vertex. For production of a Z boson and a photon, these couplings are zero in the ...relevant ... 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
... J. Bendavid, L. Benhabib, J.F. Benitez, P. Bloch, A. Bocci, A. Bonato, O. Bondu, C. Botta, H. Breuker, T. Camporesi, G. Cerminara, S. Colafranceschi 34 , M. D’Alfonso, D. d’Enterria, A. Dabrowski, A. David, F. De ... See full document
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Search for narrow resonances in the b-tagged dijet mass spectrum in proton-proton collisions at $\sqrt{s} =$ 8 TeV
... 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, ...such resonances. The results are ... See full document
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Search for black holes in high-multiplicity final states in proton-proton collisions at $ \sqrt{s}=$13 TeV
... tensor and does not distinguish between various par- ticle species, microscopic BHs decay democratically into all SM degrees of freedom, ...W and Z bosons, or of heavy-flavor quarks, and the ... See full document
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Constraints on the $χ_\mathrm{c1}$ versus $χ_\mathrm{c2}$ polarizations in proton-proton collisions at $\sqrt{s} =$ 8 TeV
... c and b quarks makes it possible to describe the process in nonrelativistic quantum chromodynamics (NRQCD) [1–8] , a framework valid when the quark velocities are ...[9] at high ... See full document
18
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
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Search for new resonances in $W\gamma$ and $Z\gamma$ final states in $pp$ collisions at $\sqrt s=8$ TeV with the ATLAS detector
... background mass distribution for the range, between 180 GeV and ...presented in Sec. VII is also taken into account in evaluating the background parametrization systemat- ...γ and Zγ ... See full document
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Search for Evidence of the Type-III Seesaw Mechanism in Multilepton Final States in Proton-Proton Collisions at $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$
... predictions and the observed events with three leptons, OSSF1, above Z, and for events with four or more leptons, OSSF1, along with systematic ...50% in the theoretical cross section ... See full document
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Search for excited quarks of light and heavy flavor in $\gamma +$ jet final states in proton–proton collisions at $\sqrt{s} =$ 13TeV
... pixel and strip tracker, a lead tungstate crystal electromagnetic calorimeter (ECAL), and a brass and scintillator hadron calorimeter (HCAL), each com- posed of a barrel and two endcap ... See full document
22
Search for Low Mass Vector Resonances Decaying to Quark-Antiquark Pairs in Proton-Proton Collisions at $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$
... narrow resonances in the dijet invariant mass spectrum have been an important part of the physics program at every ...predict resonances with significant couplings to quarks ...ticles ... See full document
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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
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Search for $\mathrm{t}\overline{\mathrm{t}}$H production in the all-jet final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV
... signal and backgrounds is incorporated into the ...quarks and events containing jets from ...signal and the multijet background and, to a lesser extent, the tt+jets ...combined in a ... See full document
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Search for Resonant Production of High-Mass Photon Pairs in Proton-Proton Collisions at $\sqrt s$ =8 and 13 TeV
... G. Smith, 160 S. Taroni, 160 M. Wayne, 160 M. Wolf, 160 A. Woodard, 160 J. Alimena, 161 L. Antonelli, 161 J. Brinson, 161 B. Bylsma, 161 L. S. Durkin, 161 S. Flowers, 161 B. Francis, 161 A. Hart, 161 ... See full document
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Search for narrow resonances in dilepton mass spectra in proton-proton collisions at $\sqrt{s}$ = 13 TeV and combination with 8 TeV data
... the 8 TeV data in ...positive and uniform, as this is known to result in good frequentist coverage ...scenarios in which the hypothetical particle is ei- ther a spin-1 or a ... See full document
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Search for high-mass $\mathrm{ Z }\gamma$ resonances in proton-proton collisions at $\sqrt{s}=$ 8 and 13 TeV using jet substructure techniques
... D. Abbaneo, E. Auffray, G. Auzinger, P. Baillon, A.H. Ball, D. Barney, P. Bloch, A. Bocci, C. Botta, T. Camporesi, R. Castello, M. Cepeda, G. Cerminara, Y. Chen, D. d’Enterria, A. Dabrowski, V. Daponte, A. David, M. De ... See full document
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Search for Z$\gamma$ resonances using leptonic and hadronic final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV
... reconstruct and identify each individual particle in an event, based on an optimized combination of information from the various elements of the CMS ...momentum at the primary interaction vertex as ... See full document
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Search for high-mass resonances in dilepton final states 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 institutes ... See full document
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