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Cr Self-Diffusion Mundy 1981

dc.contributorMaterials Science Division, Argonne Rational Laboratoryen_US
dc.contributorAmes Laboratory, DOE, Iowa State University
dc.contributor.authorMundy, J. N.
dc.contributor.authorHoff, H. A.
dc.contributor.authorPelleg, J.
dc.contributor.authorRothman, S. J.
dc.contributor.authorNowicki, L. J.
dc.contributor.authorSchmidt, F. A.
dc.date.accessioned2013-07-03T17:01:45Z
dc.date.accessioned2015-06-10T20:13:03Z
dc.date.available2013-07-03T17:01:45Z
dc.date.available2015-06-10T20:13:03Z
dc.date.issued2013-07-03
dc.identifier.citationJ. N. Mundy, H. A. Hoff, J. Pelleg, S. J. Rothman, L. J. Nowicki, F. A. Schmidt, Self-diffusion in chromium, Phys. Rev. B 24, 658, 1981en_US
dc.identifier.urihttp://hdl.handle.net/11115/132
dc.description.abstractSelf-diffusion in chromium single crystals has been measured over the temperature range 1073 to 1446 K. These data, when combined with earlier measurements from this laboratory over the. range 1370—2090 K, yield a plot of lnD vs 1/T, which is straight over ten orders of magnitude in the diffusion coefficient D. The high values of the preexponential factor (1280+ 230 cm's ') and activation enthalpy (4.58+ 0.03 eV) are not readily interpreted in terms of a specific diffusion mechanism. They appear to be too high to be interpreted in terms of a monovacancy mechanism. The possible contribution of divacancies and self-interstitials are discussed.en_US
dc.relation.urihttp://dx.doi.org/10.1103/PhysRevB.24.658en_US
dc.rightsAttribution 3.0 United States*
dc.rights.urihttp://creativecommons.org/licenses/by/3.0/us/*
dc.subjectself-diffusionen_US
dc.subjectCr
dc.subjectDiffusion Mobilities
dc.titleCr Self-Diffusion Mundy 1981en_US
dc.typeDataseten_US


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