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  1. Probing bottom-associated production of a TeV scale scalar decaying to a top quark and dark matter at the LHC (in EN)

    Abstract A minimal non-thermal dark matter model that can explain both the existence of dark matter and the baryon asymmetry in the universe is studied. It requires two color-triplet, iso-singlet scalars with$$$$ \mathcal{O}\left(\textrm{TeV}\right) $$$$ O TeV masses and a singlet Majorana fermion with a mass of$$$$ \mathcal{O}\left(\textrm{GeV}\right) $$$$ O GeV . The fermion becomes stable and can play the role of the dark matter candidate. We consider the fermion to interact with a top quark via the exchange of QCD-charged scalar fields coupled dominantly to third generation fermions. The signature of a single topmore » quark production associated with a bottom quark and large missing transverse momentum opens up the possibility to search for this type of model at the LHC in a way complementary to existing monotop searches.« less
  2. First measurement of the forward rapidity gap distribution in pPb collisions at $$\sqrt{s_{NN}}$$ = 8.16 TeV

    For the first time at LHC energies, the forward rapidity gap spectra from proton-lead collisions for both proton and lead dissociation processes are presented. The analysis is performed over 10.4 units of pseudorapidity at a center-of-mass energy per nucleon pair of $$\sqrt{s_{NN}}$$ = 8.16 TeV , almost 300 times higher than in previous measurements of diffractive production in proton-nucleus collisions. For lead dissociation processes, which correspond to the pomeron-lead event topology, the EPOS-LHC generator predictions are a factor of 2 below the data, but the model gives a reasonable description of the rapidity gap spectrum shape. For the pomeron-proton topology,more » the EPOS-LHC, QGSJET II, and HIJING predictions are all at least a factor of 5 lower than the data. The latter effect might be explained by a significant contribution of ultraperipheral photoproduction events mimicking the signature of diffractive processes. These data may be of significant help in understanding the high energy limit of quantum chromodynamics and for modeling cosmic ray air showers.« less
  3. Measurement of differential cross sections for the production of a Z boson in association with jets in proton-proton collisions at s = 13 TeV

    A measurement is presented of the production of Z bosons that decay into two electrons or muons in association with jets, in proton-proton collisions at a centre-of-mass energy of 13 TeV. The data were recorded by the CMS Collaboration at the LHC with an integrated luminosity of 35.9 fb$$^{-1}$$. The differential cross sections are measured as a function of the transverse momentum ($$p_\mathrm{T}$$) of the Z boson and the transverse momentum and rapidities of the five jets with largest $$p_\mathrm{T}$$. The jet multiplicity distribution is measured for up to eight jets. The hadronic activity in the events is estimated usingmore » the scalar sum of the $$p_\mathrm{T}$$ of all the jets. All measurements are unfolded to the stable particle-level and compared with predictions from various Monte Carlo event generators, as well as with expectations at leading and next-to-leading orders in perturbative quantum chromodynamics.« less
  4. Measurements of jet multiplicity and jet transverse momentum in multijet events in proton–proton collisions at $${\sqrt{s}=13\, \text {TeV}}$$

    Multijet events at large transverse momentum ($$p$$T) are measured at $$\sqrt{s}$$ = 13 TeV using data recorded with the CMS detector at the LHC, corresponding to an integrated luminosity of 36.3 fb-1. The multiplicity of jets with $$p$$T > 50 GeV that are produced in association with a high-$$p$$T dijet system is measured in various ranges of the $$p$$T of the jet with the highest transverse momentum and as a function of the azimuthal angle difference Δ$$\phi$$1,2 between the two highest $$p$$T jets in the dijet system. The differential production cross sections are measured as a function of the transversemore » momenta of the four highest $$p$$T jets. The measurements are compared with leading and next-to-leading order matrix element calculations supplemented with simula tions of parton shower, hadronization, and multiparton interactions. In addition, the measurements are compared with next-to-leading order matrix element calculations combined with transverse-momentum dependent parton densities and transverse-momentum dependent parton shower.« less
  5. Constraints on anomalous Higgs boson couplings to vector bosons and fermions from the production of Higgs bosons using the 𝜏⁢𝜏 final state

    A study of anomalous couplings of the Higgs boson to vector bosons and fermions is presented. The data were recorded by the CMS experiment at a center-of-mass energy of pp collisions at the LHC of 13 TeV and correspond to an integrated luminosity of 138 fb−1. The study uses Higgs boson candidates produced mainly in gluon fusion or electroweak vector boson fusion at the LHC that subsequently decay to a pair of 𝜏 leptons. Matrix-element and machine-learning techniques were employed in a search for anomalous interactions. The results are combined with those from the four-lepton and two-photon decay channels tomore » yield the most stringent constraints on anomalous Higgs boson couplings to date. The pure 𝐶⁢𝑃-odd scenario of the Higgs boson coupling to gluons is excluded at 2.4 standard deviations. The results are consistent with the standard model predictions.« less
  6. Azimuthal correlations in Z +jets events in proton–proton collisions at $$\sqrt{s} = 13\,\text {Te}\text {V} $$

    The production of Z bosons associated with jets is measured in pp collisions at $$\sqrt{s}=13\,\text {TeV}$$ with data recorded with the CMS experiment at the LHC corresponding to an integrated luminosity of 36.3 fb-1. The multiplicity of jets with transverse momentum $$p$$T > 30 GeV is measured for different regions of the Z boson’s $$p$$T (Z ), from lower than 10 GeV to higher than 100 GeV. The azimuthal correlation $$Δ\phi$$ between the Z boson and the leading jet, as well as the correlations between the two leading jets are measured in three regions of $$p$$T(Z ). The measurements aremore » compared with several predictions at leading and next-to-leading orders, interfaced with parton showers. Predictions based on transverse-momentum dependent parton distributions and corresponding parton showers give a good description of the measurement in the regions where multiple parton interactions and higher jet multiplicities are not important. The effects of multiple parton interactions are shown to be important to correctly describe the measured spectra in the low $$p$$T(Z ) regions.« less
  7. Azimuthal Correlations within Exclusive Dijets with Large Momentum Transfer in Photon-Lead Collisions

    The structure of nucleons is multidimensional and depends on the transverse momenta, spatial geometry, and polarization of the constituent partons. Such a structure can be studied using high-energy photons produced in ultraperipheral heavy-ion collisions. The first measurement of the azimuthal angular correlations of exclusively produced events with two jets in photon-lead interactions at large momentum transfer is presented, a process that is considered to be sensitive to the underlying nuclear gluon polarization. This study uses a data sample of ultraperipheral lead-lead collisions at s NN = 5.02 more » TeV , corresponding to an integrated luminosity of 0.38 nb - 1 , collected with the CMS experiment at the LHC. The measured second harmonic of the correlation between the sum and difference of the two jet transverse momentum vectors is found to be positive, and rising, as the dijet transverse momentum increases. A well-tuned model that has been successful at describing a wide range of proton scattering data from the HERA experiments fails to describe the observed correlations, suggesting the presence of gluon polarization effects.« less
  8. Two-particle azimuthal correlations in γp interactions using pPb collisions at s NN =8.16TeV

    The first measurements of the Fourier coefficients ( V n Δ ) of the azimuthal distributions of charged hadrons emitted from photon-proton (γp) interactions are presented. The data are extracted from 68.8 nb−1 of ultra-peripheral proton-lead (pPb) collisions at s NN =8.16TeV using the CMS detector. The high energy lead ions produce a flux of photons that can interact with the oncoming proton. This γp system provides a set of uniquemore » initial conditions with multiplicity lower than in photon-lead collisions but comparable to recent electron-positron and electron-proton data. The V n Δ coefficients are presented in ranges of event multiplicity and transverse momentum ( p T ) and are compared to corresponding hadronic minimum bias pPb results. For a given multiplicity range, the mean p T of charged particles is smaller in γp than in pPb collisions. For both the γp and pPb samples, V 1 Δ is negative, V 2 Δ is positive, and V 3 Δ consistent with 0. For each multiplicity and p T range, V 2 Δ is larger for γp events. The γp data are consistent with model predictions that have no collective effects.« less
  9. Search for the exotic decay of the Higgs boson into two light pseudoscalars with four photons in the final state in proton-proton collisions at $$ \sqrt{s} $$ = 13 TeV

    A search for the exotic decay of the Higgs boson to a pair of light pseudoscalars, each of which subsequently decays into a pair of photons, is presented. The search uses data from proton-proton collisions at $$ \sqrt{s} $$ = 13 TeV recorded with the CMS detector at the LHC that corresponds to an integrated luminosity of 132 fb$$^{−1}$$. The analysis probes pseudoscalar bosons with masses in the range 15–62 GeV, coming from the Higgs boson decay, which leads to four well-isolated photons in the final state. No significant deviation from the background-only hypothesis is observed. Upper limits are setmore » on the product of the Higgs boson production cross section and branching fraction into four photons. The observed (expected) limits range from 0.80 (1.00) fb for a pseudoscalar boson mass of 15 GeV to 0.26 (0.24) fb for a mass of 62 GeV at 95% confidence level.[graphic not available: see fulltext]« less
  10. Search for direct pair production of supersymmetric partners of τ leptons in the final state with two hadronically decaying τ leptons and missing transverse momentum in proton-proton collisions at s = 13 TeV

    A search for the direct production of a pair of $$τ$$ sleptons, the supersymmetric partners of $$τ$$ leptons, is presented. Each $$τ$$ slepton is assumed to decay to a $$τ$$ lepton and the lightest supersymmetric particle (LSP), which is assumed to be stable and to not interact in the detector, leading to an imbalance in the total reconstructed transverse momentum. The search is carried out in events identified as containing two $$τ$$ leptons, each decaying to one or more hadrons and a neutrino, and significant transverse momentum imbalance. In addition to scenarios in which the $$τ$$ sleptons decay promptly, themore » search also addresses scenarios in which the $$τ$$ sleptons have sufficiently long lifetimes to give rise to nonprompt $$τ$$ leptons. The data were collected in proton-proton collisions at a center-of-mass energy of 13 TeV at the CERN LHC with the CMS detector in 2016–2018, and correspond to an integrated luminosity of 138 fb-1. No significant excess is seen with respect to standard model expectations. Upper limits on cross sections for the pair production of $$τ$$ sleptons are obtained in the framework of simplified models. In a scenario in which the $$τ$$ sleptons are superpartners of left-handed $$τ$$ leptons, and each undergoes a prompt decay to a $$τ$$ lepton and a nearly massless LSP, $$τ$$ slepton masses between 115 and 340 GeV are excluded. In a scenario in which the lifetime of the $$τ$$ sleptons corresponds to c$$τ$$0 = 0.1 mm, where $$τ_{0}$$ represents the mean proper lifetime of the $$τ$$ slepton, masses between 150 and 220 GeV are excluded.« less
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