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3 edition of Observation of prompt muon production in proton-nucleus collisions found in the catalog.

Observation of prompt muon production in proton-nucleus collisions

David L. Bintinger

Observation of prompt muon production in proton-nucleus collisions

by David L. Bintinger

  • 32 Want to read
  • 13 Currently reading

Published .
Written in English


Classifications
LC ClassificationsMicrofilm 45613
The Physical Object
FormatMicroform
Paginationii, 87 l.
Number of Pages87
ID Numbers
Open LibraryOL1367765M
LC Control Number92895061

The neutron is also classified as a baryon, because it is composed of three valence quarks. The finite size of the neutron and its magnetic moment both indicate that the neutron is a composite particle, as opposed to being an elementary particle. A neutron contains two down quarks with charge − 1 ⁄ 3 e and one up quark with charge + 2 ⁄ 3 abcdfestivalgoa.comfication: Baryon. Abashian, A. proposal to measure anti-muon - neutrino and muon - neutrino elastic scattering, neutrino oscillations and decays of long - lived neutral particles at the Tevatron of Fermilab; Aitkenhead, W. a determination of the pion and kaon structure functions;.

Measurement of prompt ψ(2S) production cross sections in proton–lead and proton–proton collisions at √sNN = TeV. Observation of single top quark production in association with a Z Boson in proton-proton collisions at s =13 TeV. Observation of top quark production in proton-nucleus collisions. Resonant and Continuum Production of Massive Muon Pairs in GeV Proton - Nucleus Collisions - Kaplan Inclusive jet production in ultrarelativistic proton-nucleus collisions - Perepelitsa, Dennis CERN-THESIS Observation of Muon Neutrino Charged Current Events in an Off-Axis Horn-Focused Neutrino Beam Using the NOvA Prototype Cited by:

Publications of Nicola Semprini Cesari. Professor at Department of Physics and Astronomy — DIFA Measurement of the Upsilon Production Cross Section in Gev Fixed-Target Proton-Nucleus Collisions Search for Anomalous Production of Prompt Like-Sign Muon Pairs and Constraints on Physics Beyond the Standard Model with the Atlas Detector. We have studied the transverse-momentum (pT) dependence of the inclusive J/ψ production in p–Pb collisions at √sNN= TeV, in three center-of-mass rapidity (ycms) regions, down to zero pT. Results in the forward and backward rapidity ranges (


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Observation of prompt muon production in proton-nucleus collisions by David L. Bintinger Download PDF EPUB FB2

Observation of prompt neutrinos from Gev proton-nucleus collisions. These ratios are not in contradiction with prompt muon production experiments [4,5], where most muons are produced in pairs. Absolute event rates from tr, K, A, and E- decays have been calculated replacing the nuclear cascade in the beam dump by a decay path of one Cited by: A proton beam-dump experiment using the CHARM neutrino detector has been performed at the CERN SPS.

We report the observation of events induced by pro Cited by: Abstract: The first observation of top quark production in proton-nucleus collisions is reported using proton-lead data collected by the CMS experiment at the CERN LHC at a nucleon-nucleon center-of-mass energy of $\sqrt{s_\mathrm{NN}} =$ TeV.

The measurement is performed using events with exactly one isolated electron or muon and at least four jets. Abstract. A measurement is presented of the exclusive and semi-exclusive production of charged pion pairs in proton-proton collisions, pp to p(p*) + pi+pi- + p(p*) here the pi+pi- pair is emitted at central rapidities, and the scattered protons stay intact (p) or diffractively dissociate (p*) without detection.

NA60 is a fixed-target experiment at the CERN SPS which measured dimuon production in nucleus–nucleus and proton–nucleus collisions. The experiment collected muon pair samples of unprecedented. Abstract. An experimental search was performed to look for the direct production of neutrinos or neutrino-like particles, i.e., neutral particles which interact weakly with hadrons, in proton-nucleus interactions at GeV incident proton abcdfestivalgoa.com: J.P.

Dishaw. Dec 14,  · The top quark is the heaviest quark, weighing more than most atoms. It was first observed in coming out of proton-antiproton collisions at the Tevatron accelerator outside of Chicago, and it has been studied since at the Large Hadron Collider in proton-proton collisions.

This is a list of past and current experiments at the CERN Super Proton Synchrotron (SPS) facility since its commissioning in The SPS was used as the main particle collider for many experiments, and has been adapted to various purpose ever since its inception. Four locations were used for experiments, the North Area (NA experiments), West Area (WA experiments), Underground Area (UA.

4 LHCb is the only detector fully instrumented in the forward region Some measurements currently only possible with LHCb (excellent particle ID) Good vertexing, possibility to separate prompt and from-b production Particle detection down to very low p T Burkhard Schmidt Workshop on Proton- and Photon-induced nuclear collisions at the LHC ATLAS & CMS: central detectorsAuthor: Burkhard Schmidt.

Abstract. Direct muon yields (μ ±) in the transverse momentum range from to GeV/c on Cu and Be nuclei at proton energies of 70, 50 and 35 GeV have been measured. The yield of direct muons to pions is shown to decrease considerably when the proton energy varies from 70 to 35 abcdfestivalgoa.com by: 5.

Meson Production in Proton-Nucleus and Nucleus-Nucleus Collisions* W. Cassingf Institut fur Theoretische Physik, Universitat Giessen, Germany Received August 28, accepted November 11, Abstract The production of K+ or q mesons in proton-nucleus reactions is analysed with respect to primary nucleon-nucleon (NN + NhK+ or NNq) and sec.

The NA60 experiment has studied low-mass muon pair production in proton–nucleus collisions with a system of Be, Cu, In, W, Pb and U targets, using a GeV proton beam at the CERN SPS. in proton-proton and proton-nucleus collisions, di rac-tive DIS and the initial state for hydrodynamical model-ing of heavy ion collisions.

This framework has thus a broad range of applications. The modification of J= production cross section in proton-nucleus compared to proton-proton collisions has been previously studied in the CGC.

Abstract. Given the large parton luminosities, sizable rate of events, with several pairs of b-quarks produced contemporarily by multiple parton interactions, are foreseen in hadronic and nuclear collisions at very high abcdfestivalgoa.com compare the different contributions to \(b\bar bb\bar b \) production, due to single and double parton scatterings, in pp and in p A collisions at the CERN LHC Author: A.

Del Fabbro, D. Treleani. in both proton-nucleus and nucleus-nucleus collisions over a wide range of energies. Introduction Propagation of a particle in the nuclear medium is characterized by its mean free path (refs.

1, 2, and 3). At incident energies of 50 MeV, the experimental mean free path for protons is known (refs. 4, 5, and 6) to be approximately 5 6 fin.

characteristics of muon pair production in p-p collisions at very high energies as a probe of proton constituents by joseph alan paradiso b.s.e.e.

tufts university submitted to the department of physics in partial fulfillment of the requirements for the degree of doctor of philosophy at the massachusetts institute of technology april the hard photon production in proton-nucleus collisions became available, ' which show that the earlier data of Ref.

9 is off by a factor ofTherefore, in the present work we analyze these new data. The formalism we use to calculate the nucleon-nucleus bremsstrahlung is the same as in Ref. We express the photon emission probability per.

ALICE is optimized to study heavy-ion (Pb-Pb nuclei) collisions at a centre of mass energy of TeV per nucleon abcdfestivalgoa.com resulting temperature and energy density are expected to be high enough to produce quark–gluon plasma, a state of matter wherein quarks and gluons are freed.

Similar conditions are believed to have existed a fraction of the second after the Big Bang before quarks and Headquarters: Geneva, Switzerland.

Using the ATLAS detector, observations have been made of a centrality-dependent dijet asymmetry in the collisions of lead ions at the Large Hadron Collider.

In a sample of lead-lead events with a per-nucleon center of mass energy of TeV, selected with a minimum bias trigger, jets are reconstructed in fine-grained, longitudinally-segmented electromagnetic and hadronic calorimeters.

Measurement of the bb production cross section in proton-nucleus collisions at HERA-B P. Kreuzer (for the HERA-B Collaboration) Observation of double cc production in e + e - annihilation H. Palka Isolated prompt photon production in photon-photon collisions at √ s ee = GeV T.

Schörner-Sadenius (for the OPAL Collaboration)Price: $. Proton-nucleus collisions at high luminosity have been implemented and exploited in the LHC, the first upgrade beyond its baseline design.

At 4TeVZ per beam, the luminosity is already close to the projection and request for V7 Te Z [2,3,4]. With the coming energy upgrade and lifting of the artificial.Emphasis is given to the lessons learnt from LHC Run 1 results, which are reviewed in a global picture with the results from SPS and RHIC at lower energies, as well as to the questions to be addressed in the future.

The report covers heavy flavour and quarkonium production in proton–proton, proton–nucleus and nucleus– nucleus abcdfestivalgoa.com by: 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.

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