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Response of plastic scintillator detectors to heavy ions, Z E <= 170 MeV

dc.contributor.authorBecchetti, Fredrick D.en_US
dc.contributor.authorThorn, C. E.en_US
dc.contributor.authorLevine, M. J.en_US
dc.date.accessioned2006-04-07T16:25:27Z
dc.date.available2006-04-07T16:25:27Z
dc.date.issued1976-10-01en_US
dc.identifier.citationBecchetti, F. D., Thorn, C. E., Levine, M. J. (1976/10/01)."Response of plastic scintillator detectors to heavy ions, Z E &lt;= 170 MeV." Nuclear Instruments and Methods 138(1): 93-104. <http://hdl.handle.net/2027.42/21662>en_US
dc.identifier.urihttp://www.sciencedirect.com/science/article/B73DN-471XS73-1C7/2/fd4fb8ec62564998c8367c179536687aen_US
dc.identifier.urihttps://hdl.handle.net/2027.42/21662
dc.description.abstractThe fluorescent response, L, of plastic scintillators such as NE102 has been measured for a variety of heavy ions, Z = 1-35, at near-normal incidence with energies ranging from a few MeV to over a hundred MeV. The response in general is non-linear with L [is proportial to] f(Z, A)E1.6 in the region E/A R, with L [is proportial to] Z1.22 (R-0.04 Z), where R is in mg/cm2. Such an expression also appears to describe the response of other scintillators, such as NaI(Tl), for heavy ions. Scintillation efficiency, dL/dE, and specific fluorescence, dL/dx, have been deduced from the plastic scintillator data. These quantities do not appear to be simple functions of the ion energy loss, dE/dx. The results can be described using simple models which include the effects of secondary electrons, however.en_US
dc.format.extent978990 bytes
dc.format.extent3118 bytes
dc.format.mimetypeapplication/pdf
dc.format.mimetypetext/plain
dc.language.isoen_US
dc.publisherElsevieren_US
dc.titleResponse of plastic scintillator detectors to heavy ions, Z E &#60;= 170 MeVen_US
dc.typeArticleen_US
dc.rights.robotsIndexNoFollowen_US
dc.subject.hlbsecondlevelNuclear Engineering and Radiological Sciencesen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelEngineeringen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumPhysics Department, The University of Michigan, Ann Arbor, Michigan 48109, U.S.A.; Physics Department, Brookhaven National Laboratory, Upton, New York 11973, U.S.A.en_US
dc.contributor.affiliationumPhysics Department, The University of Michigan, Ann Arbor, Michigan 48109, U.S.A.en_US
dc.contributor.affiliationumPhysics Department, The University of Michigan, Ann Arbor, Michigan 48109, U.S.A.en_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/21662/1/0000049.pdfen_US
dc.identifier.doihttp://dx.doi.org/10.1016/0029-554X(76)90154-3en_US
dc.identifier.sourceNuclear Instruments and Methodsen_US
dc.owningcollnameInterdisciplinary and Peer-Reviewed


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