Diffusion in Binary and Pseudo-Binary L12 Indides, Stannides, Gallides and Aluminides of Rare-Earth Elements as Studied Using Perturbed Angular Correlation of 111In/Cd

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Diffusional jumps can produce fluctuating electric field gradients at nuclei of jumping atoms. Using perturbed angular correlation of gamma rays (PAC), jumps of probe atoms cause nuclear quadrupole relaxation that can be fitted to obtain the mean jump frequency. An overview is given of the application of this approach to highly ordered intermetallic compounds having the L12 (Cu3Au) crystal structure. New results are then presented for jump frequencies of 111In/Cd probe atoms in pseudo-binary L12 compounds of the forms In3(La1-xPrx) and (In1-xSnx)3La. For the mixed rare-earth system, jump frequencies are found to scale with composition between jump frequencies of the end-member phases In3La and In3Pr. However, for the mixed sp-element system, a large decrease in jump frequency is observed as Sn atoms substitute for In-atoms. This difference in behavior appears to depend on whether atomic disorder is on the diffusion sublattice (In-Sn substitution), as opposed to a neighboring sublattice (La-Pr substitution), whether or not there is a difference in diffusion mechanism between end-member phases, and/or whether or not there is a valence difference between the mixing atoms. All three conditions apply for only (In1-xSnx)3La.

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Defect and Diffusion Forum (Volumes 323-325)

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447-452

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April 2012

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© 2012 Trans Tech Publications Ltd. All Rights Reserved

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[1] Matthew O. Zacate, Aurélie Favrot and Gary S. Collins, Phys. Rev. Lett. 92 (2004) p.225901.

Google Scholar

[2] Gary S. Collins et al., Hyperfine Interact. 159 (2005) p.1.

Google Scholar

[3] G.S. Collins et al., Defect and Diffusion Forum 237-240 (2005) p.195.

Google Scholar

[4] Gary S. Collins et al., Phys. Rev. Lett. 102 (2009) p.155901.

Google Scholar

[5] Megan Lockwood et al., Defect and Diffusion Forum 311 (2011) p.159.

Google Scholar

[6] X. Jiang, M.O. Zacate and G.S. Collins, Defect and Diffusion Forum 289-292 (2009) p.725.

Google Scholar

[7] Gary S. Collins, J. Materials Science 42 (2007) p. (1915).

Google Scholar

[8] John. P. Bevington, PhD dissertation, Washington State University, May 2011 (unpublished).

Google Scholar

[9] Matthew O. Zacate and Gary S. Collins, Phys. Rev. B69 (2004) p.174202; Günter Schatz and Alois Weidinger, Nuclear Condensed Matter Physics, (John Wiley, New York, 1996).

Google Scholar

[10] Tyler Park et al., Hyperfine Interact., DOI 10. 1007/s10751-011-0332-6 (online 15 Apr 2011).

Google Scholar

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[1] 4 Qn(x) for In3(La1-xPrx) Q4 Q [eV] x Q0 La Pr.

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0 0. 2 0. 4 0. 6 0. 8 1. 0.

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[2] 0 Q0 Qn(x) for (In1-xSnx)3La Q[eV] x In Sn Q12 Fig. 4. Composition dependences of jump-frequency activation enthalpies modeled for probe atoms on In or (In, Sn) sublattices to jump into a vacancy on the same sublattice. Lines correspond to different local configurations of atoms. Left: In3(La1-xPrx), with jumps into vacancies having 04 Pr-neighbors. Right: (In1-xSnx)3La, with jumps into vacancies having 0-12 Sn-neighbors. Dark lines show the mean activation enthalpy as a function of composition.

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