3 edition of Momentum loss in proton-nucleus and nucleus-nucleus collisions found in the catalog.
Momentum loss in proton-nucleus and nucleus-nucleus collisions
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
|Statement||Ferdous Khan, Lawrence W. Townsend.|
|Series||NASA technical paper -- 3405., NASA technical paper -- 3405.|
|Contributions||United States. National Aeronautics and Space Administration. Scientific and Technical Information Program.|
|The Physical Object|
Discuss two dimensional collisions as an extension of one dimensional analysis. Define point masses. Derive an expression for conservation of momentum along x-axis and y-axis. Describe elastic collisions of two objects with equal mass. Determine the magnitude and direction of the final velocity given initial velocity, and scattering angle. We study nuclear stopping in high energy nuclear collisions using the constituent quark model. It is assumed that wounded nucleons with a different number of interacted quarks hadronize in different ways. The probabilities of having such wounded nucleons are evaluated for proton-proton, proton-nucleus, and nucleus-nucleus collisions.
hadron production in proton–nucleus (or deuteron–nucleus) collisions provides a valuable reference for nucleus–nucleus collisions,asitprobesinitial-statenPDFmodiﬁcationsovera wide kinematic range and is expected to be largely free from the ﬁnal-state effects that accompany QGP production . Free Online Library: Observation of Gaussian Pseudorapidity Distributions for Produced Particles in Proton-Nucleus Collisions at Tevatron Energies.(Research Article, Report) by "Advances in High Energy Physics"; Collisions (Nuclear physics) Analysis Energy (Physics) Force and energy Gaussian distribution Usage Normal distribution Particle collisions.
energy-loss, not only in nucleus nucleus collisions, but proton nucleus and proton proton collisions as well. 2. Leading Order pQCD Calculations Using formulae derived from perturbative QCD (pQCD), we intend to calculate the inclusive spectra of charged hadron production from proton anti-proton and proton nucleus collisions. Production of Charged Kaons in Proton - Nucleus and Nucleus-Nucleus Collisions at GeV/Nucleon J. Bachler et al., (NA35 Collaboration), C 58 () Multiplicity Distributions in Small Phase Space Domains in Central Nucleus-Nucleus Collisions J. Bachler et al., (NA35 Collaboration.), C 57 ()
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Of longitudinal momentum loss in proton-nucleus and nucleus-nucleus collisions is presented. The crucial role of the imaginary component of the nucleon-nucleon transition matrix in accounting for longitudinal momentum transfer is demonstrated.
Results obtained with this model are compared with Intranuclear Cascade (INC) calculations, as well as. Get this from a library. Momentum loss in proton-nucleus and nucleus-nucleus collisions.
[Ferdous Khan; United States. National Aeronautics and Space Administration. Scientific and. An optical model description, based on multiple scattering theory, of longitudinal momentum loss in proton-nucleus and nucleus-nucleus collisions is presented. CiteSeerX - Document Details (Isaac Councill, Lee Giles, Pradeep Teregowda): An optical model description, based on multiple scattering theory, of longitudinal momentum loss in proton-nucleus and nucleus-nucleus collisions is presented.
proton-nucleus and nucleus-nucleus (AA) collisons we de-veloped a new Monte Carlo (MC) event generator HARD-PING (Hard Probe Interaction Generator). It is based on HIJING generator , an extension of PYTHIA  for hadron collisions on jet production in nuclear collisions. Multiple soft rescatterings and energy loss of quarks.
Advanced Search. Citation; Search; DOI/ISSN/ISBN. In the wounded nucleon model, a proton–nucleus (p + A) collision is a superposition of independent nucleon–nucleon collisions.
We use this model to calculate the average transverse momentum of pions, kaons and protons in high energy p + A collisions. Measurements of the fractional momentum loss (S-loss = delta p(T) / p(T)) of high-transverse-momentum-identified hadrons in heavy-ion collisions are presented. Using pi(0) in Au + Au and Cu + Cu collisions at root s(NN) = and GeV measured by the PHENIX experiment at the Relativistic Heavy Ion Collider and and charged hadrons in Pb + Pb collisions measured by the.
parton energy loss is the observed suppression of ener-getic particles in AA collisions. It is typically quanti ed FIG. (top) The number of binary collisions as a func-tion of participant nucleons in minimum bias nucleus-nucleus, proton-nucleus and centrality selected heavy-ion collisions.
(bottom) Measured hadron and jet nuclear modi cation. Momentum is the most important quantity when it comes to handling collisions in physics. Momentum is a physical quantity defined as the product of mass multiplied by velocity.
Note the definition says velocity, not speed, so momentum is a vector quantity. This means that a 1,kg car moving north at 20 m/s has a different [ ]. Forward Physics in Proton-Nucleus and Nucleus-Nucleus Collisions Jan Nemchik IEP SAS, Kosice, Slovakia Czech Technical University, FNSPE, Praque, Czech Republic Sixth International Conference on Perspectives in Hadronic Physics Trieste - Italy, 12 - 16 May, Forward Physics in Proton-Nucleusand Nucleus-Nucleus Collisions – p.
1/ KK decays, in Pb-Pb and other collision systems. Keywords: Heavy ion collisions, proton-nucleus collisions,φmeson, dimuon PACS: q,Dw,Cs NA60 is a ﬁxed-target experiment devoted to the study of dimuon production in proton-nucleus (p-A) and nucleus-nucleus collisions at the CERN SPS.
Its apparatus is. The aim of this paper is to understand particle production for different collision systems, namely proton-proton (pp), proton-nucleus (pA), and nucleus-nucleus (AA) scattering at the LHC. This universal regime of high-energy QCD is described by non-linear evolution equations.
The program would address the theoretical and phenomenological progress in our understanding of gluon saturation in ep, eA, along with the proton-proton (pp), proton-nucleus (pA) and nucleus-nucleus (AA) collisions.
the collective effects in multiparticle production in nucleus-nucleus and proton-nucleus collisions just by consideration of energy needed to produce particles in all nucleon-nucleon collisions. The Modiﬁed Glauber Model of nucleon momentum loss done in the MGM (Fig. This means that caution should be taken in.
An optical model description, based on multiple scattering theory, of longitudinal momentum loss in proton-nucleus and nucleus-nucleus collisions is presented.
The crucial role of the imaginary component of the nucleon-nucleon transition matrix in accounting for longitudinal momentum transfer is. The Monte Carlo version of the Modified Glauber Model (MGM)  is updated and applied to the analysis of the total multiplicity yields of charged particles in mucleus-nucleus and proton-nucleus collisions in a broad energy range.
The MGM takes into account the energy conservation and momentum loss for particle production in each nucleon-nucleon inelastic collision. The production of antiprotons in proton-nucleus and nucleus-nucleus reactions is analyzed with respect to baryon-baryon production processes.
The dynamical evolution of the phase-space distributions is treated on the basis of the Vlasov-Uehling-Uhlenbeck transport theory including explicitly pion, Δ() and N ∗ () degrees of freedom and considering free on-shell production. In our framework, all the matter created in high-energy proton–proton, proton–nucleus, and nucleus–nucleus collisions originates from partons produced in the primary collisions.
Here we employ an event generator, P ythiafor the production of partons. pp collisions via Eq. () (n =2,3), once the corresponding SPS cross section is known. Proton-nucleus collisions The larger transverse parton density in nuclei compared to protons results in enhanced DPS cross sections, pA → ab, coming from interactions where the.
In high energy nucleus-nucleus collisions a novel state of nuclear matter, the Quark Gluon Plasma (QGP) is created. Hard partonic scatterings which happen inside the bulk of this nuclear matter serve as an important probe of QGP properties through their energy loss.We present a detailed phenomenological study of the associated production of a prompt photon and a heavy-quark jet (charm or bottom) in proton-nucleus (p-A) and nucleus-nucleus (A-A) collisions.
We show that future p-A data to be collected at the LHC should allow one to disentangle the various sets currently available. In A-A collisions, the photon transverse momentum can be used to gauge the.The transverse momentum and rapidity distributions of net protons and negatively charged hadrons have been measured for minimum bias proton–nucleus and deuteron–gold interactions, as well as central oxygen–gold and sulphur–nucleus collisions at GeV per nucleon.
The rapidity density of net protons at midrapidity in central nucleus–nucleus collisions increases both with target mass.