Integral measurements of plural and multiple scattering of electrons with energies between 10 and 100 keV for 6 ≤ Z ≤ 83: I. Thin and intermediate-thickness targets

dc.contributor.authorBarros, Suelen F.
dc.contributor.authorPetri, A.R.
dc.contributor.authorMalafronte, A.A.
dc.contributor.authorFernández Varea, José María
dc.contributor.authorMaidana, N.L.
dc.contributor.authorMartins, Marcos N.
dc.contributor.authorSilva, T.F.
dc.contributor.authorVanin, V.R.
dc.contributor.authorMangiarotti, A.
dc.date.accessioned2024-07-02T15:13:53Z
dc.date.available2024-12-31T06:10:10Z
dc.date.issued2023-01-01
dc.date.updated2024-07-02T15:13:58Z
dc.description.abstractAngle-integrated plural- and multiple-scattering distributions have been measured for electrons impinging with kinetic energies from 10 to 100 keV on targets with atomic numbers between those of C and Bi and mass thicknesses ranging from to 300 2. The thinnest targets, to 20 2, are not self-supporting and have been deposited on C backings with areal densities around 10 2. The intermediate-thickness ones are made of a single element and have mass thicknesses of to 300 2. The electrons scattered at frontal angles are collected with a Faraday cup covering the polar angles below 12.0°. In addition, to supplement this information, an aluminium ring spanning a polar angle interval of has been installed around the entrance of the Faraday cup and the charge deposited on it has also been recorded. The electrical current in the scattering chamber is measured as well so as to provide an accurate normalisation. Corrections for the fraction of impinging electrons backscattered by both the Faraday cup and the ring are applied to the data. The measurements are compared with the predictions of a Monte Carlo code that simulates each individual elastic collision. For targets made of a single element, the analytical Goudsmit–Saunderson and Lewis theories are tested as well. In all cases, the single-scattering angular differential cross sections, obtained by partial-wave solution of the Dirac equation in a self-consistent central potential, are taken from the ICRU Report 77. Good agreement is found within the uncertainties of the data. An analytical formula for the angular integration of the Goudsmit–Saunderson distribution is presented in an Appendix.
dc.format.extent17 p.
dc.format.mimetypeapplication/pdf
dc.identifier.idgrec729409
dc.identifier.issn0969-806X
dc.identifier.urihttps://hdl.handle.net/2445/214171
dc.language.isoeng
dc.publisherElsevier Ltd
dc.relation.isformatofVersió postprint del document publicat a: https://doi.org/10.1016/j.radphyschem.2022.110540
dc.relation.ispartofRadiation Physics and Chemistry, 2023, vol. 202, p. 110540-1-110540-17
dc.relation.urihttps://doi.org/10.1016/j.radphyschem.2022.110540
dc.rightscc-by-nc-nd (c) Elsevier Ltd, 2023
dc.rights.accessRightsinfo:eu-repo/semantics/openAccess
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/4.0/
dc.sourceArticles publicats en revistes (Física Quàntica i Astrofísica)
dc.subject.classificationTransport d'electrons
dc.subject.classificationMètode de Montecarlo
dc.subject.otherElectron transport
dc.subject.otherMonte Carlo method
dc.titleIntegral measurements of plural and multiple scattering of electrons with energies between 10 and 100 keV for 6 ≤ Z ≤ 83: I. Thin and intermediate-thickness targets
dc.typeinfo:eu-repo/semantics/article
dc.typeinfo:eu-repo/semantics/acceptedVersion

Fitxers

Paquet original

Mostrant 1 - 1 de 1
Carregant...
Miniatura
Nom:
256423.pdf
Mida:
2.18 MB
Format:
Adobe Portable Document Format