Heavy-ion partial beam lifetimes due to Coulomb induced processes
- 1 October 1996
- journal article
- Published by American Physical Society (APS) in Physical Review E
- Vol. 54 (4) , 4233-4239
- https://doi.org/10.1103/physreve.54.4233
Abstract
The magnitude of heavy-ion beam loss at the relativistic heavy ion collider (RHIC) and the large hadron collider (LHC) due to Coulomb induced bound-electron–positron production and to Coulomb dissociation of the nucleus is evaluated. With the nominal design parameters, the associated partial beam lifetime of RHIC (assuming four intersection regions) is calculated as 7.7 h and that of LHC (one intersection region) as 5.3 h. © 1996 The American Physical Society.Keywords
This publication has 23 references indexed in Scilit:
- Convergence of bound-electron–positron pair production calculations for relativistic heavy-ion collisionsPhysical Review A, 1994
- Calculation of the cross section fore+-e−(Korbit) pairs by very-high-energy fully stripped heavy ions at perturbational impact parametersPhysical Review A, 1993
- Bound-electron–positron pair production in relativistic heavy-ion collisionsPhysical Review A, 1993
- Energy dependence of bound-electron–positron pair production at very-high-energy ion-ion transitsPhysical Review A, 1991
- Electromagnetic processes in relativistic heavy ion collisionsPhysics Reports, 1988
- Total photonuclear absorption cross section for Pb and for heavy nuclei in the Δ-resonance regionNuclear Physics A, 1984
- Measurements of the total photonuclear cross sections from 30 MeV to 140 MeV for Sn, Ce, Ta, Pb and U nucleiNuclear Physics A, 1981
- The total photon deuteron hadronic cross section in the energy range 0.265–4.215 GeVNuclear Physics B, 1972
- Total Hadronic Cross Section ofRays in Hydrogen in the Energy Range 0.265-4.215 GeVPhysical Review D, 1972
- Photoneutron cross sections of 208Pb and 197AuNuclear Physics A, 1970