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Search for a heavy resonance decaying into a Z boson and a vector boson in the $\nu\overline{\nu}\mathrm{q}\mathrm{\bar{q}}$ final state / CMS Collaboration
A search is presented for a heavy resonance decaying into either a pair of Z bosons or a Z boson and a W boson (ZZ or WZ), with a Z boson decaying into a pair of neutrinos and the other boson decaying hadronically into two collimated quarks that are reconstructed as a highly energetic large-cone jet. The search is performed using the data collected with the CMS detector at the CERN LHC during 2016 in proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to a total integrated luminosity of 35.9 fb$^{-1}$. [...]
arXiv:1803.03838; CMS-B2G-17-005; CERN-EP-2018-023; CMS-B2G-17-005-003.- Geneva : CERN, 2018-07-11 - 34 p. - Published in : JHEP 07 (2018) 075 Article from SCOAP3: PDF; Fulltext: PDF; External links: Additional information for the analysis; CMS AuthorList

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Measurement of the $\Lambda_b$ polarization and angular parameters in $\Lambda_b\to J/\psi\, \Lambda$ decays from pp collisions at $\sqrt{s}=$ 7 and 8 TeV / CMS Collaboration
An analysis of the decay $\Lambda_b \to J/\psi(\to\mu^+\mu^-)\Lambda(\to p \pi^-)$ decay is performed to measure the $\Lambda_b$ polarization and three angular parameters in data from pp collisions at $\sqrt{s} =$ 7 and 8 TeV, collected by the CMS experiment at the LHC. The $\Lambda_b$ polarization is measured to be 0.00 $\pm$ 0.06 (stat) $\pm$ 0.06 (syst) and the parity-violating asymmetry parameter is determined to be 0.14 $\pm$ 0.14 (stat) $\pm$ 0.10 (syst). [...]
arXiv:1802.04867; CMS-BPH-15-002; CERN-EP-2017-331; CMS-BPH-15-002-003.- Geneva : CERN, 2018-04-18 - 20 p. - Published in : Phys. Rev. D 97 (2018) 072010 Article from SCOAP3: PDF; Fulltext: 1802.04867 - PDF; cms-bph-15-002-arxiv - PDF; External links: Additional information for the analysis; CMS AuthorList

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Search for dark matter in events with energetic, hadronically decaying top quarks and missing transverse momentum at $\sqrt{s}=$ 13 TeV / CMS Collaboration
A search for dark matter is conducted in events with large missing transverse momentum and a hadronically decaying, Lorentz-boosted top quark. This study is performed using proton-proton collisions at a center-of-mass energy of 13 TeV, in data recorded by the CMS detector in 2016 at the LHC, corresponding to an integrated luminosity of 36 fb$^{-1}$. [...]
arXiv:1801.08427; CMS-EXO-16-051; CERN-EP-2017-299; CMS-EXO-16-051-003.- Geneva : CERN, 2018-06-05 - 52 p. - Published in : JHEP 06 (2018) 027 Article from SCOAP3: PDF; Fulltext: PDF; External links: Additional information for the analysis; CMS AuthorList

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Combined search for electroweak production of charginos and neutralinos in proton-proton collisions at $\sqrt{s} =$ 13 TeV / CMS Collaboration
A statistical combination of several searches for the electroweak production of charginos and neutralinos is presented. All searches use proton-proton collision data at $\sqrt{s}=$ 13 TeV, recorded with the CMS detector at the LHC in 2016 and corresponding to an integrated luminosity of 35.9 fb$^{-1}$. [...]
arXiv:1801.03957; CMS-SUS-17-004; CERN-EP-2017-283; CMS-SUS-17-004-003.- Geneva : CERN, 2018-03-27 - 44 p. - Published in : JHEP 03 (2018) 160 Article from SCOAP3: PDF; Fulltext: PDF; External links: Additional information for the analysis; CMS AuthorList

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Measurement of the $\mathrm{Z}\gamma^{*} \to \tau\tau$ cross section in pp collisions at $\sqrt{s} = $ 13 TeV and validation of $\tau$ lepton analysis techniques / CMS Collaboration
A measurement is presented of the $\mathrm{Z}/\gamma^{*} \to \tau\tau$ cross section in pp collisions at $\sqrt{s} = $ 13 TeV, using data recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 2.3 fb$^{-1}$. The product of the inclusive cross section and branching fraction is measured to be $\sigma(\mathrm{pp} \to \mathrm{Z}/\gamma^{*}\text{+X}) \, \mathcal{B}(\mathrm{Z}/\gamma^{*} \to \tau\tau) = $ 1848 $\pm$ 12 (stat) $\pm$ 67 (syst+lumi) pb, in agreement with the standard model expectation, computed at next-to-next-to-leading order accuracy in perturbative quantum chromodynamics. [...]
arXiv:1801.03535; CMS-HIG-15-007; CERN-EP-2017-307; CMS-HIG-15-007-003.- Geneva : CERN, 2018-09-03 - 68 p. - Published in : Eur. Phys. J. C 78 (2018) 708 Article from SCOAP3: PDF; Fulltext: PDF; External links: Additional information for the analysis; CMS AuthorList

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Measurement of prompt and nonprompt charmonium suppression in $\text {PbPb}$ collisions at 5.02 $\,\text {Te}\text {V}$ / CMS Collaboration
The nuclear modification factors of J/$\psi$ and $\psi$(2S) mesons are measured in PbPb collisions at a centre-of-mass energy per nucleon pair of $\sqrt{s_{\mathrm{NN}}} =$ 5.02 TeV. The analysis is based on PbPb and pp data samples collected by CMS at the LHC in 2015, corresponding to integrated luminosities of 464 $\mu$b$^{-1}$ and 28 pb$^{-1}$, respectively. [...]
arXiv:1712.08959; CMS-HIN-16-025; CERN-EP-2017-308; CMS-HIN-16-025; CERN-EP-2017-308; CMS-HIN-16-025-003.- Geneva : CERN, 2018-06-20 - 36 p. - Published in : Eur. Phys. J. C
Article from SCOAP3: PDF; Fulltext: arXiv:1712.08959 - PDF; 1712.08959 - PDF; External links: Additional information for the analysis; CMS AuthorList

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Bose-Einstein correlations in $pp, p\mathrm{Pb}$, and PbPb collisions at $\sqrt{{s}_{NN}}=0.9-7$ TeV / CMS Collaboration
Quantum statistical (Bose-Einstein) two-particle correlations are measured in pp collisions at $\sqrt{s}= $ 0.9, 2.76, and 7 TeV, as well as in pPb and peripheral PbPb collisions at nucleon-nucleon center-of-mass energies of 5.02 and 2.76 TeV, respectively, using the CMS detector at the LHC. Separate analyses are performed for same-sign unidentified charged particles as well as for same-sign pions and kaons identified via their energy loss in the silicon tracker. [...]
arXiv:1712.07198; CMS-FSQ-14-002; CERN-EP-2017-327; CMS-FSQ-14-002-003.- Geneva : CERN, 2018-06-15 - 42 p. - Published in : Phys. Rev. C 97 (2018) 064912 Article from SCOAP3: PDF; Fulltext: arXiv:1712.07198 - PDF; openaccess_PhysRevC.97.064912 - PDF; External links: Additional information for the analysis; CMS AuthorList

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Search for lepton flavour violating decays of the Higgs boson to $\mu\tau$ and e$\tau$ in proton-proton collisions at $\sqrt{s}=$ 13 TeV / CMS Collaboration
A search for lepton flavour violating decays of the Higgs boson in the $\mu\tau$ and e$\tau$ decay modes is presented. The search is based on a data set corresponding to an integrated luminosity of 35.9 fb$^{-1}$ of proton-proton collisions collected with the CMS detector in 2016, at a centre-of-mass energy of 13 TeV. [...]
arXiv:1712.07173; CMS-HIG-17-001; CERN-EP-2017-292; CMS-HIG-17-001-003.- Geneva : CERN, 2017 - 48 p. - Published in : JHEP 1806 (2018) 001 Article from SCOAP3: PDF; Fulltext: arXiv:1712.07173 - PDF; cms-hig-17-001-arxiv - PDF; External links: Additional information for the analysis; CMS AuthorList

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Identification of heavy-flavour jets with the CMS detector in pp collisions at 13 TeV / CMS Collaboration
Many measurements and searches for physics beyond the standard model at the LHC rely on the efficient identification of heavy-flavour jets, i.e. jets originating from bottom or charm quarks. [...]
arXiv:1712.07158; CMS-BTV-16-002; CERN-EP-2017-326; CMS-BTV-16-002-004.- Geneva : CERN, 2018-05-08 - 114 p. - Published in : JINST 13 (2018) P05011 Fulltext: arXiv:1712.07158 - PDF; cms-btv-16-002-arxiv - PDF; pdf - PDF; Fulltext from Publisher: PDF; External links: Additional information for the analysis; CMS AuthorList

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10.

Search for the X(5568) state decaying into $\mathrm{B}^{0}_{\mathrm{s}}\pi^{\pm}$ in proton-proton collisions at $\sqrt{s} = $ 8 TeV / CMS Collaboration
A search for resonance-like structures in the $\mathrm{B}^{0}_{\mathrm{s}}\pi^{\pm}$ invariant mass spectrum is performed using proton-proton collision data collected by the CMS experiment at the LHC at $\sqrt{s} = $ 8 TeV, corresponding to an integrated luminosity of 19.7 fb$^{-1}$. The $\mathrm{B}^{0}_{\mathrm{s}}$ mesons are reconstructed in the decay chain $\mathrm{B}^{0}_{\mathrm{s}} \rightarrow \mathrm{J}/\psi\,\phi$, with $\mathrm{J}/\psi \rightarrow \mu^+\mu^-$ and $\phi\rightarrow\mathrm{K^{+}}\mathrm{K^{-}}$. [...]
arXiv:1712.06144; CMS-BPH-16-002; CERN-EP-2017-287; CMS-BPH-16-002-003.- Geneva : CERN, 2018-05-19 - 17 p. - Published in : Phys. Rev. Lett. 120 (2018) 202005 Article from SCOAP3: PDF; Fulltext: PDF; Fulltext from Publisher: PDF; External links: Additional information for the analysis; CMS AuthorList

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4	Lapsien, T
6	Lapsien, T.

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