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Tuesday, October 13, 2020 | History

3 edition of Final state interactions and inclusive nuclear collisions found in the catalog.

Final state interactions and inclusive nuclear collisions

Final state interactions and inclusive nuclear collisions

  • 47 Want to read
  • 9 Currently reading

Published by National Aeronautics and Space Administration, Office of Management, Scientific and Technical Information Program, National Technical Information Service, distributor] in [Washington, DC], [Springfield, Va .
Written in English

    Subjects:
  • Multiple scattering (Physics),
  • Nuclear reactions.

  • Edition Notes

    StatementFrancis A. Cucinotta, Rajendra R. Dubey.
    SeriesNASA technical paper -- 3353., NASA technical paper -- 3353.
    ContributionsDubey, Rajendra R., United States. National Aeronautics and Space Administration. Scientific and Technical Information Program.
    The Physical Object
    FormatMicroform
    Pagination1 v.
    ID Numbers
    Open LibraryOL14701163M

    The final chapters of the book are devoted to more specific topics that arise when nuclear collisions are considered as a tool for the experimental study of QCD thermodynamics. This second edition includes a new chapter on the hydrodynamic evolution of the medium produced in nuclear by: Abstract. We compute the Oσ 2 σ 2 s perturbative corrections to inclusive jet production in electron-nucleon collisions. This process is of particular interest to the physics program of a future Electron Ion Collider (EIC). We include all relevant partonic processes, including deep-inelastic scattering contributions, photon-initiated corrections, and parton-parton scattering terms that first.

    The model has then been extended to finite nuclei, taking into account nuclear effects such as Fermi motion, Pauli blocking (both within the local density approximation), nuclear binding and final-state interactions. The in-medium modification of the Δ resonance because of Pauli blocking and collisional broadening have also been included.   The construction of a Monte Carlo generator for high energy hadronic and nuclear collisions is discussed in detail. Interactions are treated in the framework of the Reggeon Field Theory, taking into consideration enhanced Pomeron diagrams which are resummed to all orders in the triple-Pomeron coupling. Soft and “semihard” contributions to the underlying parton dynamics are Cited by:

      The types of cross sections required for transport involve total yields and absorption cross sections and multiplicities and inclusive double-differential cross sections that depend on a single-particle angle and energy (3, 8). The multiplicity refers to the number of particles of a given type that may be produced in a nuclear by:   The BABAR collaboration at SLAC has observed the radiative decay of an excited state of bottomonium (the bound state of a bottom quark and its antiparticle) to its ground state ηb. Observing this long-sought ground state should enable better tests of quantum chromodynamic calculations of quark interactions and the computational approach called lattice quantum : Stephen Godfrey.


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Final state interactions and inclusive nuclear collisions Download PDF EPUB FB2

As a result of nucleon final-state interaction, the peak intensities are reduced by %; about half of the (e, e') reaction is found to correspond to multinucleon removal. paper we also focus on the final state interaction (FSI) between knocked-out target nucleons and the target recoil.

A treatment of the FSI in inclusive scattering is important for understanding scaling phenomena (refs. ) and transparency (refs. 7 9) in high-energy collisions as well as in the intranuclear cascade.

Get this from a library. Final state interactions and inclusive nuclear collisions. [Francis A Cucinotta; Rajendra R Dubey; United States. National Aeronautics and Space Administration.

Scientific and Technical Information Program.]. The presentation of bulk equilibrium thermodynamics is completed by studying the properties of the quark-gluon plasma as new state of strongly interacting final chapters of the book are devoted to more specific topics which arise when nuclear collisions are considered as a tool for the experimental study of QCD : Paperback.

CiteSeerX - Document Details (Isaac Councill, Lee Giles, Pradeep Teregowda): A scattering formalism is developed in a multiple scattering model to describe inclusive momentum distributions for high-energy projectiles. The e ects of nal state interactions on response functions and momentum distributions are investigated.

Calculations for high-energy protons that include shell model response. A scattering formalism is developed in a multiple scattering model to describe inclusive momentum distributions for high-energy projectiles. The e ects of nal state interactions on response functions and momentum distributions are investigated.

A big difficulty is represented by the scarce knowledge of the nuclear systems in their final states. In order to circumvent the obstacle represented by the continuum states, Lorentz integral transform method (LITM) was proposed, a method which allows the calculation of inclusive cross sections using bound state techniques.

The Few Body Problem covers the proceedings of the Ninth International Conference on the Few Body Problem, held in Eugene, Oregon, USA on AugustThe book focuses on relativistic and particle physics, intermediate energy physics, nuclear, atomic, and molecular physics, and chemistry.

outline the extension of the framework to inclusive DIS, including a polarized deuteron target as well as its application to the tagged DIS reactions for future experiments at fixed target and collider energies.

Keywords: Nuclear deep inelastic scattering; final-state interactions; deuteron. PACS Number(s): −m, −r, Ni 1. The inclusive yield is enhanced in d+Au collisions relative to binary-scaled p+p collisions, while the two-particle azimuthal distributions are very similar to those observed in p+p by:   These results are consistent with a scenario where high-p_T eta production in nuclear collisions at RHIC is largely unaffected by initial-state effects, but where light-quark mesons (pi^0;eta) are equally suppressed due to final-state interactions of the parent partons in the dense medium produced in Au+Au by:   The implications of the ωN final state interactions are studied for ω production in 12 C + 12 C, 40 Ca + 40 Ca and 58 Ni + 58 Ni reactions at about 2 A GeV within the HSD transport approach; the drastic changes of the transverse mass spectra relative to a general m T-scaling (for π 0 and η mesons) might be controlled experimentally by Cited by: Final-state interactions in semi-inclusive and inclusive deep-inelastic scattering off the deuteron Wim Cosyn, M.

Sargsian, W. Melnitchouk Florida International University Ghent University, Belgium Exploring Hadron Structure with Tagged Structure Functions Jefferson Lab phenomena that have been observed at high-pT in Au+Au collisions are due to initial-state effects in the Au nuclei, final-state energy loss, or a combination of the two.

STAR recorded over 30 million minimum-bias d+Au collisions during the run, together with over 1 million events triggered on the I We predict the dynamical shadowing from final state interactions in ν+A reactions for sea and valence quarks in the structure functions F A 2 (x,Q2) and xF A 3 (x,Q2), respectively.

In p+A collisions we calculate the centrality and rapidity dependent nuclear suppression of single and double inclusive hadron production at moderate transverse. It contains the Section ‘ Color Deconfinement and Charmonium Production in Nuclear Collisions’ of the Chapter ‘6 Selective Tracer Signals of the QCD Plasma State’ with the content: Novel High Transverse Momentum Phenomena in Hadronic and Nuclear Collisions Stanley J.

Brodsky† SLAC National Accelerator Laboratory, Stanford University, Stanford, California E-mail:[email protected] The presence of direct higher-twist processes, where a proton is produced directly in the hard.

i,degli Atti, i,ni FINAL STATE INTERACTION IN INCLUSIVE AND EXCLUSIVE QUASI-ELASTIC PROCESSES World Scientific - nucl-th/; M. Alvioli, C. Ciofi degli Atti, H. Morita, L.P. Kaptari REALISTIC CALCULATIONS OF ONE- AND TWO-HADRON EMISSION PROCESSES OFF FEW- AND MANY-BODY NUCLEI.

The nuclear suppression factor R AA of single inclusive hadrons measured in ultrarelativistic heavy-ion collisions was the first observable to study jet quenching, i.e., the final state interaction of hard parton showers with the surrounding bulk matter.

While its transverse momentum (P T) dependence of R AA observed at RHIC was weak and hence never decisive in constraining Cited by: Events belong to very central collisions of protons with heavy emulsion nuclei with probability of realization of less than % and with multiplicity of shower particles exceeding (times) the average multiplicity in proton-nucleus collisions in emulsion.

Bjorken’s energy Author: Abdurakhmanov Ulugbek, Gulamov Kadyr, Lugovoi Vladimir, Navotny Vadim. CMS Collaboration: Observation of electroweak production of same-sign W boson pairs in the two jet and two same-sign lepton final state in proton-proton collisions at 13 TeV (arXiv, Phys.

Rev. Lett. () ).W_N is represented by its elastic and lowest-energy inelastic parts, while W_{\NA} is computed from its asymptotic limit, supplemented by final state interactions due to binary collisions between the knocked-out and core nucleons. (q/M)W_{\NA} per nucleon appears to be practically independent of mass number A and momentum transfer : A S Rinat and M F Taragin.In A+A collisions, the strong final-state interactions probably alter the momentum distribution to be more isotropic at low momenta; the hard tail is modified by parton energy loss.

Although these effects may in part be included in the glasma, the additional contributions at later stages are by: