Does backscattering of 4He ions by nuclei obey the Rutherford cross-section formula?
- 1 April 1974
- journal article
- research article
- Published by AIP Publishing in Journal of Applied Physics
- Vol. 45 (4) , 1888-1890
- https://doi.org/10.1063/1.1663510
Abstract
Implicit in the use of nuclear backscattering as a quantitative analytic tool is the accuracy of calculating cross sections using a classical Coulombic scattering formula (Rutherford cross section) which includes recoil effects, but ignores spin, nuclear size, electron screening, hard‐sphere scattering, and any nuclear‐force effects. The Rutherford cross section has not previously been verified experimentally for ions of 4He (1–2.5 MeV) for targets of 16O, 27Al, and 28Si. For 14N, agreement has been found with an accuracy of about 5%. Our experimental results show that 27Al and 28Si have the Rutherford formula value (±1%), and 16O is Rutherford from 1.4 to 2.4 MeV. 14N appears to deviate by about 2% at energies from 1.2 to 2.2 MeV and by more beyond this energy band.This publication has 8 references indexed in Scilit:
- Stopping cross sections and backscattering factors for 4He ions in matter Z = 1–92, E(4He) = 400–4000 keVAtomic Data and Nuclear Data Tables, 1974
- Tables for reaction gamma-ray spectroscopy part I. A = 6 to A = 20Atomic Data and Nuclear Data Tables, 1974
- ELECTRON CAPTURE AND LOSS BY FAST IONS IN ATOMIC COLLISIONSSoviet Physics Uspekhi, 1965
- + and + Differential Cross SectionsPhysical Review B, 1961
- and Differential Cross SectionsPhysical Review B, 1958
- Passage of Heavy Particles through MatterReviews of Modern Physics, 1953
- Elastic Scattering of Alpha-Particles by OxygenPhysical Review B, 1953
- LVIII. Collision of α particles with light atomsJournal of Computers in Education, 1914