1,453 research outputs found

    Muon Production in Relativistic Cosmic-Ray Interactions

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    Cosmic-rays with energies up to 3×10203\times10^{20} eV have been observed. The nuclear composition of these cosmic rays is unknown but if the incident nuclei are protons then the corresponding center of mass energy is snn=700\sqrt{s_{nn}} = 700 TeV. High energy muons can be used to probe the composition of these incident nuclei. The energy spectra of high-energy (>> 1 TeV) cosmic ray induced muons have been measured with deep underground or under-ice detectors. These muons come from pion and kaon decays and from charm production in the atmosphere. Terrestrial experiments are most sensitive to far-forward muons so the production rates are sensitive to high-xx partons in the incident nucleus and low-xx partons in the nitrogen/oxygen targets. Muon measurements can complement the central-particle data collected at colliders. This paper will review muon production data and discuss some non-perturbative (soft) models that have been used to interpret the data. I will show measurements of TeV muon transverse momentum (pTp_T) spectra in cosmic-ray air showers from MACRO, and describe how the IceCube neutrino observatory and the proposed Km3Net detector will extend these measurements to a higher pTp_T region where perturbative QCD should apply. With a 1 km2^2 surface area, the full IceCube detector should observe hundreds of muons/year with pTp_T in the pQCD regime.Comment: 4 pages, 2 figures - To appear in the conference proceedings for Quark Matter 2009, March 30 - April 4, Knoxville, Tennessee. Tweaked formatting at organizers reques

    Robert-John in Memories

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    Extended Air Shower Simulations Based on EPOS

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    We discuss air shower simulations based on the EPOS hadronic interaction model. A remarkable feature is the fact that the number of produced muons is considerably larger compared to other interaction models. We show that this is due to an improved treatment of baryon-antibaryon production.Comment: Talk presented at EDS0

    Global properties of proton-proton collisions at s\sqrt{s} = 100 TeV

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    The global properties of the final states produced in hadronic interactions of protons at centre-of-mass energies of future hadron colliders (such as FCC-hh at CERN, and SppC in China), are studied. The predictions of various Monte Carlo (MC) event generators used in collider physics (PYTHIA 6, PYTHIA 8, and PHOJET) and in ultrahigh-energy cosmic-rays studies (EPOS, and QGSJET) are compared. Despite their different underlying modeling of hadronic interactions, their predictions for proton-proton (p-p) collisions at s\sqrt{s} = 100 TeV are quite similar. The average of all MC predictions (except PHOJET) for the different observables are: (i) p-p inelastic cross sections σinel\sigma_{\rm inel} = 105 ±\pm 2 mb; (ii) total charged multiplicity Nch\rm N_{_{\rm ch}} = 150 ±\pm 20; (iii) charged particle pseudorapidity density at midrapidity dNch/dηη=0=9.6±0.2\rm dN_{ch}/d\eta|_{\eta=0} = 9.6 \pm 0.2; (iv) energy density at midrapidity dE/dηη=0=13.6±1.5\rm dE/d\eta|_{\eta=0} = 13.6 \pm 1.5 GeV, and dE/dηη=5=670±70\rm dE/d\eta|_{\eta=5} = 670 \pm 70 GeV at the edge of the central region; and (v) average transverse momenta at midrapidities =0.76±0.07\rm = 0.76 \pm 0.07 GeV/c. At midrapidity, EPOS and QGSJET-II predict larger per-event multiplicity probabilities at very low (Nch100\rm N_{\rm ch}100) particle multiplicities, whereas PYTHIA 6 and 8 feature higher yields in the intermediate region Nch\rm N_{\rm ch}\approx 30--80. These results provide useful information for the estimation of the detector occupancies and energy deposits from pileup collisions at the expected large FCC-hh/SppC luminosities.Comment: 10 pages, 11 figures. Minor changes. Matches version published in JHE

    Impact of QCD jets and heavy-quark production in cosmic-ray proton atmospheric showers up to 1020^{20} eV

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    The PYTHIA 6 Monte Carlo (MC) event generator, commonly used in collider physics, is interfaced for the first time with a fast transport simulation of a hydrogen atmosphere, with the same density as air, in order to study the properties of extended atmospheric showers (EAS) produced by cosmic ray protons with energies ECR1014_{CR}\approx 10^{14}--102010^{20} eV. At variance with the hadronic MC generators (EPOS-LHC, QGSJET, and SIBYLL) commonly used in cosmic-rays physics, PYTHIA includes the generation of harder hadronic jets and heavy (charm and bottom) quarks, thereby producing higher transverse momentum final particles, that could explain several anomalies observed in the data. The electromagnetic, hadronic, and muonic properties of EAS generated with various settings of PYTHIA 6, tuned to proton-proton data measured at the LHC, are compared to those from EPOS-LHC, QGSJET 01, QGSJET II, and SIBYLL 2.1. Despite their different underlying parton dynamics, the characteristics of the EAS generated with PYTHIA 6 are in between those predicted by the rest of MC generators. The only exceptions are the muonic components at large transverse distances from the shower axis, where PYTHIA predicts more activity than the rest of the models. Heavy-quark production, as implemented in this study for a hydrogen atmosphere, does not seem to play a key role in the EAS muon properties, pointing to nuclear effects as responsible of the muon anomalies observed in the air-shower data.Comment: 13 pages, 20 figure

    Proton-proton and deuteron-gold collisions at RHIC

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    We try to understand recent data on proton-proton and deuteron-gold collisions at RHIC, employing a modified parton model approach.Comment: Invited talk, given at the XXth Winter Workshop on Nuclear Dynamics, Trelawny Beach, Jamaica, March 200

    Particle Production in Proton-Proton and Deuteron-Gold Collisions at RHIC

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    We try to understand recent data on proton-proton and deuteron-gold collisions at RHIC, employing a parton model approach called EPOS.Comment: Invited talk, given at SQM2004, Cape Town, South Africa, 15-20 September, 200

    New results for hadronic collisions in the framework of the Parton-Based Gribov-Regge Theory

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    We recently proposed a new approach to high energy nuclear scattering, which treats hadronic collisions in a sophisticated way. Demanding theoretical consistency as a minimal requirement for a realistic model, we provide a solution for the energy conservation, screening problems and identical elementary interactions, the so-called "Parton-Based Gribov-Regge Theory" including enhanced diagrams. We can now present some of our results for SPS and RHIC energies.Comment: 4 pages, 3 figures, To appear in the proceedings of Quark Matter 2002 (QM 2002), Nantes, France, 18-24 Jul 200

    Ridges and Soft Jet Components in Untriggered Di-hadron Correlations in Pb+Pb Collisions at 2.76 TeV

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    We study untriggered di-hadron correlations in Pb+Pb at 2.76 TeV, based on an event-by-event simulation of a hydrodynamic expansion starting from flux tube initial conditions. The correlation function shows interesting structures as a function of the pseudorapidity difference Δη\Delta\eta and the azimuthal angle difference Δϕ\Delta\phi, in particular comparing different centralities. We can clearly identify a peak-like nearside structure associated with very low momentum components of jets for peripheral collisions, which disappears towards central collisions. On the other hand, a very broad ridge structure from asymmetric flow seen at central collisions, gets smaller and finally disappears towards peripheral collisions

    New Developments of EPOS 2

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    Since 2006, EPOS hadronic interaction model is being used for very high energy cosmic ray analysis. Designed for minimum bias particle physics and used for having a precise description of SPS and RHIC heavy ion collisions, EPOS brought more detailed description of hadronic interactions in air shower development. Thanks to this model it was possible to understand why there were less muons in air shower simulations than observed in real data. With the start of the LHC era, a better description of hard processes and collective effects is needed to deeply understand the incoming data. We will describe the basic physics in EPOS and the new developments and constraints which are taken into account in EPOS 2.Comment: Contributed presentation to the XVI International Symposium on Very High Energy Cosmic Ray Interactions (ISVHECRI 2010), Batavia, IL, USA (28 June 2 July 2010). 4 pages, 6 figure
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