8 research outputs found

    First search for exclusive diphoton production at high mass with tagged protons in proton-proton collisions at s=\sqrt{s} = 13 TeV

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    A search for exclusive two-photon production via photon exchange in proton-proton collisions, pp \to pγγ\gamma\gammap with intact protons, is presented. The data correspond to an integrated luminosity of 9.4 fb1^{-1} collected in 2016 using the CMS and TOTEM detectors at a center-of-mass energy of 13 TeV at the LHC. Events are selected with a diphoton invariant mass above 350 GeV and with both protons intact in the final state, to reduce backgrounds from strong interactions. The events of interest are those where the invariant mass and rapidity calculated from the momentum losses of the forward-moving protons matches the mass and rapidity of the central, two-photon system. No events are found that satisfy this condition. Interpreting this result in an effective dimension-8 extension of the standard model, the first limits are set on the two anomalous four-photon coupling parameters. If the other parameter is constrained to its standard model value, the limits at 95% CL are ζ1\lvert\zeta_1\rvert <\lt 2.9 ×\times 1013^{-13} GeV4^{-4} and ζ2\lvert\zeta_2\rvert <\lt 6.0 ×\times 1013^{-13} GeV4^{-4}

    Hard color-singlet exchange in dijet events in proton-proton collisions at s=\sqrt{s} = 13 TeV

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    International audienceEvents where the two leading jets are separated by a pseudorapidity interval devoid of particle activity, known as jet-gap-jet events, are studied in proton-proton collisions at s=\sqrt{s} = 13 TeV. The signature is expected from hard color-singlet exchange. Each of the highest transverse momentum (pTp_\mathrm{T}) jets must have pTjetp_\mathrm{T}^\text{jet}>\gt 40 GeV and pseudorapidity 1.4 <\ltηjet|\eta^\text{jet}|<\lt 4.7, with ηjet1ηjet2\eta^\text{jet1} \eta^\text{jet2}<\lt 0, where jet1\text{jet1} and jet2\text{jet2} are the leading and subleading jets in pTp_\mathrm{T}, respectively. The analysis is based on data collected by the CMS and TOTEM experiments during a low luminosity, high-β\beta^* run at the CERN LHC in 2015, with an integrated luminosity of 0.66 pb1^{-1}. Events with a low number of charged particles with pTp_\mathrm{T}>\gt 0.2 GeV in the interval η|\eta|<\lt 1 between the jets are observed in excess of calculations that assume only color-exchange. The fraction of events produced via color-singlet exchange, fCSEf_\text{CSE}, is measured as a function of pTjet2p_\mathrm{T}^\text{jet2}, the pseudorapidity difference between the two leading jets, and the azimuthal angular separation between the two leading jets. The fraction fCSEf_\text{CSE} has values of 0.4-1.0%. The results are compared with previous measurements and with predictions from perturbative quantum chromodynamics. In addition, the first study of jet-gap-jet events detected in association with an intact proton using a subsample of events with an integrated luminosity of 0.40 pb1^{-1} is presented. The intact protons are detected with the Roman pot detectors of the TOTEM experiment. The fCSEf_\text{CSE} in this sample is 2.91 ±\pm 0.70 (stat) 1.01+1.08^{+1.08}_{-1.01} (syst) times larger than that for inclusive dijet production in dijets with similar kinematics

    First search for exclusive diphoton production at high mass with tagged protons in proton-proton collisions at s=\sqrt{s} = 13 TeV

    No full text
    International audienceA search for exclusive two-photon production via photon exchange in proton-proton collisions, pp \to pγγ\gamma\gammap with intact protons, is presented. The data correspond to an integrated luminosity of 9.4 fb1^{-1} collected in 2016 using the CMS and TOTEM detectors at a center-of-mass energy of 13 TeV at the LHC. Events are selected with a diphoton invariant mass above 350 GeV and with both protons intact in the final state, to reduce backgrounds from strong interactions. The events of interest are those where the invariant mass and rapidity calculated from the momentum losses of the forward-moving protons matches the mass and rapidity of the central, two-photon system. No events are found that satisfy this condition. Interpreting this result in an effective dimension-8 extension of the standard model, the first limits are set on the two anomalous four-photon coupling parameters. If the other parameter is constrained to its standard model value, the limits at 95% CL are ζ1\lvert\zeta_1\rvert <\lt 2.9 ×\times 1013^{-13} GeV4^{-4} and ζ2\lvert\zeta_2\rvert <\lt 6.0 ×\times 1013^{-13} GeV4^{-4}

    First search for exclusive diphoton production at high mass with tagged protons in proton-proton collisions at s\sqrt{s} = 13 TeV

    No full text
    A search for exclusive two-photon production via photon exchange in proton-proton collisions, pp \to pγγ\gamma\gammap with intact protons, is presented. The data correspond to an integrated luminosity of 9.4 fb1^{-1} collected in 2016 using the CMS and TOTEM detectors at a center-of-mass energy of 13 TeV at the LHC. Events are selected with a diphoton invariant mass above 350 GeV and with both protons intact in the final state, to reduce backgrounds from strong interactions. The events of interest are those where the invariant mass and rapidity calculated from the momentum losses of the forward-moving protons matches the mass and rapidity of the central, two-photon system. No events are found that satisfy this condition. Interpreting this result in an effective dimension-8 extension of the standard model, the first limits are set on the two anomalous four-photon coupling parameters. If the other parameter is constrained to its standard model value, the limits at 95% CL are ζ1<\lvert\zeta_1\rvert\lt 2.88×\times1013^{-13} GeV4^{-4} and ζ2<\lvert\zeta_2\rvert\lt6.02×\times1013^{-13}GeV4^{-4}

    Search for high-mass exclusive γγ\gamma\gamma\to WW and γγ\gamma\gamma\to ZZ production in proton-proton collisions at s\sqrt{s} = 13 TeV

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    A search is performed for exclusive high-mass γγ\gamma\gamma\to WW and γγ\gamma\gamma\to ZZ production in proton-proton collisions using intact forward protons reconstructed in near-beam detectors, with both weak bosons decaying into boosted and merged jets. The analysis is based on a sample of proton-proton collisions collected by the CMS and TOTEM experiments at s \sqrt{s} = 13 TeV, corresponding to an integrated luminosity of 100 fb1^{−1}. No excess above the standard model background prediction is observed, and upper limits are set on the pp → pWWp and pp → pZZp cross sections in a fiducial region defined by the diboson invariant mass m(VV) > 1 TeV (with V = W, Z) and proton fractional momentum loss 0.04 < ξξ < 0.20. The results are interpreted as new limits on dimension-6 and dimension-8 anomalous quartic gauge couplings.[graphic not available: see fulltext
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