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Ion-induced grain growth in multilayer and coevaporated metal alloy thin films

dc.contributor.authorAlexander, Dale E.en_US
dc.contributor.authorWas, Gary S.en_US
dc.contributor.authorRehn, L. E.en_US
dc.date.accessioned2006-04-10T14:40:31Z
dc.date.available2006-04-10T14:40:31Z
dc.date.issued1991-07-01en_US
dc.identifier.citationAlexander, D. E., Was, G. S., Rehn, L. E. (1991/07/01)."Ion-induced grain growth in multilayer and coevaporated metal alloy thin films." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 59-60(Part 1): 462-466. <http://hdl.handle.net/2027.42/29259>en_US
dc.identifier.urihttp://www.sciencedirect.com/science/article/B6TJN-4718N8V-129/2/84ed63982c7746a7d30f0b7833e6ba95en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/29259
dc.description.abstractIrradiation experiments were conducted on multilayer (ML) and coevaporated (CO) thin films in order to examine the role that the heat-of-mixing ([Delta]Hmix) has in ion-induced grain growth. Room-temperature irradiations using 1.7 MeV Xe were performed in the High Voltage Electron Microscope at Argonne National Laboratory. The alloys studied (Pt-Ti, Pt-V, Pt-Ni, Au-Co and Ni-Al) spanned a large range of [Delta]Hmix values. Comparison of grain growth rates between ML and CO films of a given alloy confirmed a heat of mixing effect. Differences in grain growth rates between ML and CO films scaled according to the sign and magnitude of [Delta]Hmix of the system (with the exception of the Pt-V system). Substantial variations in growth rates among CO alloy films experiencing similar irradiation damage demonstrated that a purely collisional approach is inadequate for describing ion-induced grain growth and consideration must also be given to material-specific properties. Results from CO alloy films were consistent with a thermal spike model of ion-induced grain growth. The grain boundary mobility was observed to be proportional to the thermal spike-related parameter, F2D/[Delta]H3coh, where FD is the energy deposited in nuclear interactions and [Delta]Hcoh is the cohesive energy.en_US
dc.format.extent470260 bytes
dc.format.extent3118 bytes
dc.format.mimetypeapplication/pdf
dc.format.mimetypetext/plain
dc.language.isoen_US
dc.publisherElsevieren_US
dc.titleIon-induced grain growth in multilayer and coevaporated metal alloy thin filmsen_US
dc.typeArticleen_US
dc.rights.robotsIndexNoFollowen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbsecondlevelNuclear Engineering and Radiological Sciencesen_US
dc.subject.hlbtoplevelScienceen_US
dc.subject.hlbtoplevelEngineeringen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumDepartment of Nuclear Engineering, University of Michigan, Ann Arbor, MI 48109, USAen_US
dc.contributor.affiliationumDepartment of Nuclear Engineering, University of Michigan, Ann Arbor, MI 48109, USAen_US
dc.contributor.affiliationotherArgonne National Laboratory, 9700 S. Cass Ave., Argonne, IL 60439, USAen_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/29259/1/0000316.pdfen_US
dc.identifier.doihttp://dx.doi.org/10.1016/0168-583X(91)95260-Ken_US
dc.identifier.sourceNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atomsen_US
dc.owningcollnameInterdisciplinary and Peer-Reviewed


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