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[PDF] Top 20 Search for new physics in the monophoton final state in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Has 10000 "Search for new physics in the monophoton final state in proton-proton collisions at $ \sqrt{s}=13 $ TeV" found on our website. Below are the top 20 most common "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

Search for new physics in the monophoton final state 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 ... See full document

36

Search for $\mathrm{t}\overline{\mathrm{t}}$H production in the all-jet final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for $\mathrm{t}\overline{\mathrm{t}}$H production in the all-jet final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... to 13%, depending on the process. The PDF uncertainties [70] range between 2 and 4%, and are treated as fully correlated for all processes that share the same dominant ini- tial state ... See full document

44

Search for disappearing tracks as a signature of new long-lived particles in proton-proton collisions at $\sqrt{s} =$ 13 TeV

Search for disappearing tracks as a signature of new long-lived particles in proton-proton collisions at $\sqrt{s} =$ 13 TeV

... by the ATLAS Collaboration searched for short disappearing tracks in 13 TeV data ...[14]. The previous CMS search excluded at 95% confidence level (CL) direct electroweak ... See full document

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Search for new phenomena with the $M_{\mathrm {T2}}$ variable in the all-hadronic final state produced in proton–proton collisions at $\sqrt{s} = 13$ $\,\text {TeV}$

Search for new phenomena with the $M_{\mathrm {T2}}$ variable in the all-hadronic final state produced in proton–proton collisions at $\sqrt{s} = 13$ $\,\text {TeV}$

... of the CMS apparatus is a superconducting solenoid of 6 m internal diam- eter, providing a magnetic field of ...Within the solenoid volume are a silicon pixel and strip tracker, a lead tungstate crystal ... See full document

46

Search for ZZ resonances in the 2$\ell$2$\nu$ final state in proton-proton collisions at 13 TeV

Search for ZZ resonances in the 2$\ell$2$\nu$ final state in proton-proton collisions at 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 ... See full document

36

Search for $W' \to tb$ in proton-proton collisions at $\sqrt{s} = $ 8 TeV

Search for $W' \to tb$ in proton-proton collisions at $\sqrt{s} = $ 8 TeV

... of the standard model (SM) predict new massive charged gauge bosons ...[1–3]. The W 0 boson, for example, is a heavy partner of the SM W gauge boson that could manifest itself in ... See full document

42

Search for physics beyond the standard model in dilepton mass spectra in proton-proton collisions at $ \sqrt{s}=8 $ TeV

Search for physics beyond the standard model in dilepton mass spectra in proton-proton collisions at $ \sqrt{s}=8 $ TeV

... from proton- proton collisions at 8 TeV and recorded by the CMS experiment, are used to search for both narrow resonances and broad deviations from standard model ... See full document

47

Search for resonant $WZ$ production in the fully leptonic final state in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector

Search for resonant $WZ$ production in the fully leptonic final state in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector

... detector at the LHC has a cylindrical geometry with a near 4 π coverage in solid ...1 The inner detector (ID), con- sisting of silicon pixel, silicon microstrip and transition radiation ... See full document

21

Search for physics beyond the standard model in high-mass diphoton events from proton-proton collisions at $\sqrt{s} =$ 13 TeV

Search for physics beyond the standard model in high-mass diphoton events from proton-proton collisions at $\sqrt{s} =$ 13 TeV

... from the measurements of the photon energies and from the reso- lution of the measurement between the two ...If the z position of the vertex from which the photons ... See full document

26

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

... of physics beyond the standard model (SM) [1–3] predict strong pro- duction of particles decaying into high-multiplicity final states, ...nonperturbative physics phenomena. While the ... See full document

47

Search for electroweak production of charginos and neutralinos in multilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for electroweak production of charginos and neutralinos in multilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... describes the vast majority of particle physics ...for physics beyond the SM carried out by various experiments also have not revealed convincing evidence for the existence of such ... See full document

58

Search for heavy resonances decaying to tau lepton pairs in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Search for heavy resonances decaying to tau lepton pairs in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... from the Marie-Curie program and the European Research Council and EPLANET (European Union); the Leventis Foundation; the ...tion; the Alexander von Humboldt Foundation; the ... See full document

32

Search for bottom squark pair production in proton–proton collisions at $\sqrt{s}=13$  TeV with the ATLAS detector

Search for bottom squark pair production in proton–proton collisions at $\sqrt{s}=13$  TeV with the ATLAS detector

... Uncertainties in the modelling of the top-quark pair and single-top-quark (Wt) backgrounds are sub- dominant in SRA and dominant in ...as the difference between the ... See full document

37

Search for direct production of supersymmetric partners of the top quark in the all-jets final state in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Search for direct production of supersymmetric partners of the top quark in the all-jets final state in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... of the CMS apparatus is a superconducting solenoid of 6 m internal diame- ter, providing a magnetic field of ...Within the solenoid volume are an all-silicon pixel and strip tracker, a lead tungstate ... See full document

58

Search for new physics in events with two soft oppositely charged leptons and missing transverse momentum in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for new physics in events with two soft oppositely charged leptons and missing transverse momentum in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... arise in several SUSY models, in- cluding natural SUSY, ...solve the hierarchy problem with little fine tuning. It has been pointed out in sev- eral studies, for example in ...on ... See full document

28

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

... general search for the pair production of resonances, each decaying to two quarks, is ...reported. The search is conducted separately for heavier resonances (masses above 400 GeV), where each ... See full document

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Search for standard model production of four top quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV

Search for standard model production of four top quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV

... 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 top quark partners with charge 5/3 in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Search for top quark partners with charge 5/3 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 ... See full document

42

Combined search for electroweak production of charginos and neutralinos in proton-proton collisions at $\sqrt{s} =$ 13 TeV

Combined search for electroweak production of charginos and neutralinos in proton-proton collisions at $\sqrt{s} =$ 13 TeV

... on the particle-flow (PF) algorithm [61], which optimally com- bines information from the tracker, calorimeters, and muon systems to reconstruct and identify PF candidates, ...require at least one ... See full document

46

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

... appear in the acceptance A. Figure 3 also shows the expected limits on the cross section and their bands of ...uncertainty. The expected limits are estimated with pseudo-experiments ... See full document

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