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|a (TOE)ost6360518
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|a (TOE)6360518
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|a E 1.99:conf-900936-22
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|a E 1.99:conf-900936-22
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|a Ion-induced grain growth in multilayer and coevaporated metal alloy thin films
|h [electronic resource]
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| 260 |
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|a Washington, D.C :
|b United States. Dept. of Energy. Office of Energy Research ;
|a Oak Ridge, Tenn. :
|b distributed by the Office of Scientific and Technical Information, U.S. Dept. of Energy,
|c 1990.
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| 300 |
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|a Pages: (10 p) :
|b digital, PDF file.
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| 336 |
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|a text
|b txt
|2 rdacontent.
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| 337 |
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|a computer
|b c
|2 rdamedia.
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| 338 |
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|a online resource
|b cr
|2 rdacarrier.
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|a Published through the Information Bridge: DOE Scientific and Technical Information.
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|a 09/01/1990.
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|a "conf-900936-22"
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|a "DE91004489"
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|a ": DMR8603174"
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|a "DMR8903138"
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|a 7. international conference on ion beam modification of materials, Knoxville, TN (USA), 9-14 Sep 1990.
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|a Alexander, D.E.; Was, G.S. . Dept. of Nuclear Engineering; Rehn, L.E.
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|a Irradiation experiments were conducted on multilayer (ML) and coevaporated (CO) thin films in order to examine the role that the heat of mixing (ΔH{sub mix}) 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 ΔH{sub mix} 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 ΔH{sub mix} of the system (with 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, (F{sub D}²)/(ΔH{sub coh}³), where F{sub D} is the deposited damage energy and ΔH{sub coh} is the cohesive energy.
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| 536 |
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|b W-31109-ENG-38.
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| 650 |
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|a Rare Gases.
|2 local.
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|a Gases.
|2 local.
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|a Nonmetals.
|2 local.
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|a Crystal Growth.
|2 local.
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|a Xenon.
|2 local.
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|a Thin Films.
|2 local.
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|a Films.
|2 local.
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|a Radiation Effects.
|2 local.
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|a Physical Properties.
|2 local.
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| 650 |
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|a Physical Radiation Effects.
|2 local.
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|a Ion Beams.
|2 local.
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|a Fluids.
|2 local.
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|a Ion Implantation.
|2 local.
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|a Elements.
|2 local.
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| 650 |
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|a Alloys.
|2 local.
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|a Beams.
|2 local.
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| 650 |
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|a Mixing Heat.
|2 local.
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| 650 |
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|a Thermodynamic Properties.
|2 local.
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| 650 |
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|a Enthalpy.
|2 local.
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| 650 |
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|a Condensed Matter Physics, Superconductivity And Superfluidity.
|2 edbsc.
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| 710 |
2 |
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|a Argonne National Laboratory.
|4 res.
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| 710 |
1 |
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|a United States.
|b Department of Energy.
|b Office of Energy Research.
|4 spn.
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| 710 |
2 |
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|a National Renewable Energy Laboratory (U.S.).
|4 spn.
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| 710 |
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|a United States.
|b Department of Energy.
|b Office of Scientific and Technical Information.
|4 dst.
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| 856 |
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|u http://www.osti.gov/servlets/purl/6360518-xL6lws/
|z Online Access
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| 907 |
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|a .b59764326
|b 03-06-23
|c 05-26-10
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| 998 |
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|a web
|b 05-26-10
|c f
|d m
|e p
|f eng
|g dcu
|h 0
|i 1
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| 956 |
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|a Information bridge
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|i d828f54d-87d9-526a-8698-f1c6a34061fb
|s 247199c2-1802-542f-bd8a-5f6eb1f30b8c
|
| 952 |
f |
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|p Can circulate
|a University of Colorado Boulder
|b Online
|c Online
|d Online
|e E 1.99:conf-900936-22
|h Superintendent of Documents classification
|i web
|n 1
|
