130 research outputs found

    Performance studies of the final prototype for the CASTOR forward calorimeter at the CMS experiment

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    We present performance results of the final prototype for the CASTOR quartz-tungsten sampling calorimeter, to be installed in the very forward region of the CMS experiment at the LHC. The energy linearity and resolution, the uniformity, as well as the spatial resolution of the prototype to electromagnetic and hadronic showers are studied with E=E= 10--200 GeV electrons, E=E= 20--350 GeV pions, and E=E= 50, 150 GeV muons in beam tests carried out at CERN/SPS in 2007

    Bose-Einstein correlations of charged hadrons in proton-proton collisions at s\sqrt s = 13 TeV

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    Bose-Einstein correlations of charged hadrons are measured over a broad multiplicity range, from a few particles up to about 250 reconstructed charged hadrons in proton-proton collisions at s \sqrt{s} = 13 TeV. The results are based on data collected using the CMS detector at the LHC during runs with a special low-pileup configuration. Three analysis techniques with different degrees of dependence on simulations are used to remove the non-Bose-Einstein background from the correlation functions. All three methods give consistent results. The measured lengths of homogeneity are studied as functions of particle multiplicity as well as average pair transverse momentum and mass. The results are compared with data from both CMS and ATLAS at s \sqrt{s} = 7 TeV, as well as with theoretical predictions.[graphic not available: see fulltext]Bose-Einstein correlations of charged hadrons are measured over a broad multiplicity range, from a few particles up to about 250 reconstructed charged hadrons in proton-proton collisions at s=\sqrt{s} = 13 TeV. The results are based on data collected using the CMS detector at the LHC during runs with a special low-pileup configuration. Three analysis techniques with different degrees of dependence on simulations are used to remove the non-Bose-Einstein background from the correlation functions. All three methods give consistent results. The measured lengths of homogeneity are studied as functions of particle multiplicity as well as average pair transverse momentum and mass. The results are compared with data from both CMS and ATLAS at s=\sqrt{s} = 7 TeV, as well as with theoretical predictions

    HERA Results on Small x and Forward Jets

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    Results on measurements at small x at HERA performed by H1 and ZEUS collaborations are reviewed. Parton dynamics, i.e. DGLAP vs BFKL evolution, is studied with use of data on inclusive forward jet and forward jet accompanied by a dijet system via comparison with fixed order QCD calculations and leading-order parton-shower Monte Carlo models. Signatures of saturation at HERA are discussed

    Production of quartz plates for CMS-CASTOR Experiment

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    Light transmission rate performance of 102102 irradiated quartz samples was measured to select the best quartz plates for CMS-CASTOR calorimeter. All the produced quartz plates were originally used in a previous CERN experiment, DELPHI. Three different doses of 60^{60}Co source were used with the collaboration of PSI (Paul Scherrer Institute, Villigen PSI, Switzerland.) to study the transmission rate performance of the quartz samples after irradiation for different incident light, ranging from 250250 to 700700 nm in 55 nm increasing steps. All samples show different decrease in the rate with wavelength for different doses. Three different steps were followed before irradiation to find out the best way of cleaning the original DELPHI Cu/Cr tracks on the samples. Results of these measurements presented here correspond to the quartz plates that will be used in one hadronic sector of CASTOR calorimeter until end of 2008. For the full calorimeter new quartz plates will be installed. We also present the light transmission rate of new quartz samples (fused silica) for 1010, 5050 and 100100 MRad dose levels. This activity was performed at CERN during the period from February to May of 20082008

    Measurement of charged particle spectra in minimum-bias events from proton-proton collisions at root s =13 TeV

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    Pseudorapidity, transverse momentum, and multiplicity distributions are measured in the pseudorapidity range vertical bar eta vertical bar 0.5 GeV in proton-proton collisions at a center-of-mass energy of root s = 13 TeV. Measurements are presented in three different event categories. The most inclusive of the categories corresponds to an inelastic pp data set, while the other two categories are exclusive subsets of the inelastic sample that are either enhanced or depleted in single diffractive dissociation events. The measurements are compared to predictions from Monte Carlo event generators used to describe high-energy hadronic interactions in collider and cosmic-ray physics.Peer reviewe

    Measurement of the underlying event activity using charged-particle jets in proton-proton collisions at s\sqrt{s} = 2.76 TeV

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    A measurement of the underlying event (UE) activity in proton-proton collisions is performed using events with charged-particle jets produced in the central pseudorapidity region (∣ηjet∣ |{\eta^{\text{jet}}} | < 2) and with transverse momentum 1 ≀pTjet<\le p_{\mathrm{T}}^\text{jet} \lt 100 GeV. The analysis uses a data sample collected at a centre-of-mass energy of 2.76 TeV with the CMS experiment at the LHC. The UE activity is measured as a function of pTjetp_{\mathrm{T}}^\text{jet} in terms of the average multiplicity and scalar sum of transverse momenta (pTp_{\mathrm{T}}) of charged particles, with ∣η∣<2|{\eta}| \lt 2 and pT>0.5p_{\mathrm{T}} \gt 0.5 GeV, in the azimuthal region transverse to the highest pTp_{\mathrm{T}} jet direction. By further dividing the transverse region into two regions of smaller and larger activity, various components of the UE activity are separated. The measurements are compared to previous results at 0.9 and 7 TeV, and to predictions of several Monte Carlo event generators, providing constraints on the modelling of the UE dynamics

    The very forward CASTOR calorimeter of the CMS experiment

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