32 research outputs found
Cross sections for the production of fragments with Z greater than or equal to 8 by fragmentation of Z greater than or equal to 9 and less than or equal to 26 nuclei
Charge changing nuclear collisions in plastic nuclear track detectors were studied using a new experimental technique of automatic track measurement for etched tracks in plastic detectors. Partial cross sections for the production of fragments of charge Z approximately 8 were measured for projectile nuclei of charge 9 approximately Z approximately 26 in the detector material CR39 and in silver. for this purpose three independent experiments were performed using Bevalac beams. The first one was an exposure of a stack of CR39 plastic plates to 1.8 GeV/nucl. Ar-40 nuclei. The second one was an exposure of another CR39 stack of 1.7 GeV/nucl. Fe-56 projectiles. In the third experiment a mixed stack of CR39 plates and silver foils was irradiated with 1.7 GeV/nucl. Fe-56 nuclei. Thus the measurement of nuclear cross sections in a light target (CR39 = C12H18O7) and as well in a heavy target (silver) was possible
Photon-Photon Physics in Very Peripheral Collisions of Relativistic Heavy Ions
In central collisions at relativistic heavy ion colliders like the
Relativistic Heavy Ion Collider RHIC/Brookhaven and the Large Hadron Collider
LHC (in its heavy ion mode) at CERN/Geneva, one aims at detecting a new form of
hadronic matter - the Quark Gluon Plasma. It is the purpose of this review to
discuss a complementary aspect of these collisions, the very peripheral ones.
Due to coherence, there are strong electromagnetic fields of short duration in
such collisions. They give rise to photon-photon and photon-nucleus collisions
with high flux up to an invariant mass region hitherto unexplored
experimentally. After a general survey photon-photon luminosities in
relativistic heavy ion collisions are discussed. Special care is taken to
include the effects of strong interactions and nuclear size. Then photon-photon
physics at various gamma-gamma-invariant mass scales is discussed. The region
of several GeV, relevant for RHIC is dominated by QCD phenomena (meson and
vector meson pair production). Invariant masses of up to about 100 GeV can be
reached at LHC, and the potential for new physics is discussed. Photonuclear
reactions and other important background effects, especially diffractive
processes are also discussed. A special chapter is devoted to lepton-pair
production, especially electron-positron pair production; due to the strong
fields new phenomena, especially multiple e+-e- pair production, will occur
there.Comment: 40 pages, 19 figures, Topical Review, to appear in Journal of Physics
G, revised text, updated text/references, one figure replace
Fragmentation cross sections of S at 0.7, 1.2 and 200 GeV/nucleon
We used CR39 plastic nuclear track detectors (C12H18O7) in combination with automatic track measurement techniques to determine total charge changing and partial cross sections for the production of fragments of chargeZ F =6 toZ F =15 in collisions of32S beam nuclei at energies of 0.7, 1.2 and 200 GeV/nucleon in targets H, C, CR39, CH2, Al, Cu, Ag and Pb. By application of factorization rules measured partial cross sections are separated into pure nuclear and electromagnetic components. Total and partial cross sections for electromagnetic dissociation are compared with theoretical models. The energy dependence of pure nuclear cross sections is investigated
Fragmentation cross sections of O at 60 and 200 GeV/nucleon
We used CR39 plastic nuclear track detectors (C12H18O7) in combination with automatic track measurement to determine total charge changing and partial cross sections for the production of fragments of chargeZ=6 andZ=7 in collisions of16O beam nuclei at energies of 60 GeV/nucleon and 200 GeV/nucleon in targets H, C, CR39, CH2, Al, Cu, Ag and Pb. Total charge changing cross sections due to the process of electromagnetic dissociation are calculated based on a theoretical model and found to be consistent with total and partial electromagnetic dissociation cross sections derived from this experiment. The energy dependence of pure nuclear fragmentation is investigated