32 research outputs found

    Indigenous-driven tropical ethnobotany

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    Indigenous knowledge is recognised globally for its potential value in contemporary biodiversity conservation, management and research (Convention on Biological Diversity 2010; NRMMC 2010). In tropical Australia, Indigenous peoples' strong and diverse presence on country presents an important opportunity to support Indigenous knowledge and management systems. In November 20 I 0, we held a workshop in Cairns to consider whether a tropical Indigenous ethnobotany centre would be a good way of supporting Indigenous peoples' knowledge about the cultural values of plants

    Observation of proton-tagged, central (semi)exclusive production of high-mass lepton pairs in pp collisions at 13 TeV with the CMS-TOTEM precision proton spectrometer

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    Nonresonant central exclusive production of charged-hadron pairs in proton-proton collisions at s\sqrt{s} = 13 TeV

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    The central exclusive production of charged-hadron pairs in pp collisions at a centre-of-mass energy of 13\TeV is examined, based on data collected in a special high-β\beta^* run of the LHC. The nonresonant continuum processes are studied with the invariant mass of the centrally produced two-pion system in the resonance-free region, mπ+πm_{\pi^+\pi^-}<\lt 0.7 GeV or mπ+πm_{\pi^+\pi^-}>\gt 1.8 GeV. Differential cross sections as functions of the azimuthal angle between the surviving protons, squared exchanged four-momenta, and mπ+πm_{\pi^+\pi^-} are measured in a wide region of scattered proton transverse momenta, between 0.2 and 0.8 GeV, and for pion rapidities y\lvert y\rvert<\lt 2. A rich structure of interactions related to double-pomeron exchange is observed. A parabolic minimum in the distribution of the two-proton azimuthal angle is observed for the first time. It can be interpreted as an effect of additional pomeron exchanges between the protons from the interference between the bare and the rescattered amplitudes. After model tuning, various physical quantities are determined that are related to the pomeron cross section, proton-pomeron and meson-pomeron form factors, pomeron trajectory and intercept, and coefficients of diffractive eigenstates of the proton

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

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    A search is presented for high-mass exclusive diphoton production via photon-photon fusion in proton-proton collisions at s= \sqrt{s} = 13 TeV in events where both protons survive the interaction. The analysis utilizes data corresponding to an integrated luminosity of 103 fb1 ^{-1} collected in 2016--2018 with the central CMS detector and the CMS and TOTEM precision proton spectrometer (PPS). Events that have two photons with high transverse momenta (pTγ> p_{\mathrm{T}}^{\gamma} > 100 GeV), back-to-back in azimuth, and with a large diphoton invariant mass (mγγ> m_{\gamma\gamma} > 350 GeV) are selected. To remove the dominant inclusive diphoton backgrounds, the kinematic properties of the protons detected in PPS are required to match those of the central diphoton system. Only events having opposite-side forward protons detected with a fractional momentum loss between 0.035 and 0.15 (0.18) for the detectors on the negative (positive) side of CMS are considered. One exclusive diphoton candidate is observed for an expected background of 1.1 events. Limits at 95% confidence level are derived for the four-photon anomalous coupling parameters ζ1 |\zeta_1| 100 GeV), back-to-back in azimuth, and with a large diphoton invariant mass (mγγ>m_{\gamma\gamma} \gt 350 GeV) are selected. To remove the dominant inclusive diphoton backgrounds, the kinematic properties of the protons detected in PPS are required to match those of the central diphoton system. Only events having opposite-side forward protons detected with a fractional momentum loss between 0.035 and 0.15 (0.18) for the detectors on the negative (positive) side of CMS are considered. One exclusive diphoton candidate is observed for an expected background of 1.1 events. Limits at 95% confidence level are derived for the four-photon anomalous coupling parameters ζ1<\lvert\zeta_1\rvert \lt 0.073 TeV4^{-4} and ζ2<\lvert\zeta_2\rvert \lt 0.15 TeV4^{-4}, using an effective field theory. Additionally, upper limits are placed on the production of axion-like particles with coupling strength to photons f1f^{-1} that varies from 0.03 TeV1^{-1} to 1 TeV1^{-1} over the mass range from 500 to 2000 GeV

    Proton reconstruction with the CMS-TOTEM Precision Proton Spectrometer

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    International audienceThe Precision Proton Spectrometer (PPS) of the CMS and TOTEM experiments collected 107.7 fb1^{-1} in proton-proton (pp) collisions at the LHC at 13 TeV (Run 2). This paper describes the key features of the PPS alignment and optics calibrations, the proton reconstruction procedure, as well as the detector efficiency and the performance of the PPS simulation. The reconstruction and simulation are validated using a sample of (semi)exclusive dilepton events. The performance of PPS has proven the feasibility of continuously operating a near-beam proton spectrometer at a high luminosity hadron collider

    A search for new physics in central exclusive production using the missing mass technique with the CMS detector and the CMS-TOTEM precision proton spectrometer

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    A generic search is presented for the associated production of a Z boson or a photon with an additional unspecified massive particle X, pppp+Z/γ+X \mathrm{p}\mathrm{p}\to \mathrm{p}\mathrm{p} +\mathrm{Z}/\gamma+\mathrm{X} , in proton-tagged events from proton-proton collisions at s= \sqrt{s}= 13 TeV, recorded in 2017 with the CMS detector and the CMS-TOTEM precision proton spectrometer. The missing mass spectrum is analysed in the 600-1600 GeV range and a fit is performed to search for possible deviations from the background expectation. No significant excess in data with respect to the background predictions has been observed. Model-independent upper limits on the visible production cross section of pppp+Z/γ+X \mathrm{p}\mathrm{p}\to \mathrm{p}\mathrm{p} +\mathrm{Z}/\gamma+\mathrm{X} are set.A generic search is presented for the associated production of a Z boson or a photon with an additional unspecified massive particle X, pp \to pp + Z/γ\gamma + X, in proton-tagged events from proton-proton collisions at s\sqrt{s} = 13 TeV, recorded in 2017 with the CMS detector and the CMS-TOTEM precision proton spectrometer. The missing mass spectrum is analysed in the 600-1600 GeV range and a fit is performed to search for possible deviations from the background expectation. No significant excess in data with respect to the background predictions has been observed. Model-independent upper limits on the visible production cross section of pp \to pp + Z/γ\gamma + X are set

    Search for central exclusive production of top quark pairs in proton-proton collisions at s= \sqrt{s} = 13 TeV with tagged protons

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    A search for the central exclusive production of top quark-antiquark pairs (ttˉ \mathrm{t} \bar{\mathrm{t}} ) is performed for the first time using proton-tagged events in proton-proton collisions at the LHC at a centre-of-mass energy of 13 TeV. The data correspond to an integrated luminosity of 29.4 fb1 ^{-1} . The ttˉ \mathrm{t} \bar{\mathrm{t}} decay products are reconstructed using the central CMS detector, while forward protons are measured in the CMS-TOTEM precision proton spectrometer. An observed (expected) upper bound on the production cross section of 0.59 (1.14) pb is set at 95% confidence level, for collisions of protons with fractional momentum losses between 2 and 20%.A search for the central exclusive production of top quark-antiquark pairs (ttˉ\mathrm{t\bar{t}}) is performed for the first time using proton-tagged events in proton-proton collisions at the LHC at a centre-of-mass energy of 13 TeV. The data correspond to an integrated luminosity of 29.4 fb1^{-1}. The ttˉ\mathrm{t\bar{t}} decay products are reconstructed using the central CMS detector, while forward protons are measured in the CMS-TOTEM precision proton spectrometer. An observed (expected) upper bound on the production cross section of 0.59 (1.14) pb is set at 95% confidence level, for collisions of protons with fractional momentum losses between 2 and 20%
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