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High Pressure Research
An International Journal
Volume 38, 2018 - Issue 3
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Articles

Volume collapse phase transitions in cerium-praseodymium alloys under high pressure

, , , &
Pages 270-280 | Received 25 Apr 2018, Accepted 01 Jun 2018, Published online: 08 Jun 2018
 

ABSTRACT

Cerium-12at%Praseodymium(Ce0.88Pr0.12) and Ce-50at%Praseodymium(Ce0.50Pr0.50) alloy samples that contain a random solid-solution of Ce (4f1 (J = 5/2)) and Pr (4f2 (J = 4)) localized f-states have been studied by angle dispersive x-ray diffraction in a diamond anvil cell to a pressure of 65 GPa and 150 GPa respectively using a synchrotron source. Ce0.88Pr0.12 alloy crystallizes in a face-centered cubic (γ-phase) structure at ambient conditions, while Ce0.50Pr0.50 alloy crystallizes in the double hexagonal close packed (dhcp) structure at ambient conditions. Two distinct volume collapse transitions are observed in Ce0.88Pr0.12 alloy at 1.5 GPa and 18 GPa with volume change of 8.5% and 3% respectively. In contrast, Ce0.50Pr0.50 alloy shows only a single volume collapse of 5.6% at 20 GPa on phase transformation to α-Uranium structure under high pressure. Electrical transport measurements under high pressure show anomalies in electrical resistance at phase transitions for both compositions of this alloy.

Acknowledgements

This material is based upon work supported by the Department of Energy-National Nuclear Security Administration under Award Number DE-NA0002928. Los Alamos National Laboratory (LANL) is operated by LANS, LLC for the DOE-NNSA under Contract No. DE-AC52-06NA25396. NV acknowledge funding support from LANL Science Programs 1 and 2. Portions of this work were performed at HPCAT (Sector 16), Advanced Photon Source (APS), Argonne National Laboratory. HPCAT operations are supported by DOE-NNSA under Award No. DE-NA0001974 and DOE-BES under Award No. DE-FG02-99ER45775, with partial instrumentation funding by NSF. APS is supported by DOE-BES, under Contract No. DE-AC02-06CH11357.

Disclosure statement

No potential conflict of interest was reported by the authors.

Additional information

Funding

This material is based upon work supported by the Department of Energy-National Nuclear Security Administration under Award Number DE-NA0002928. Los Alamos National Laboratory (LANL) is operated by LANS, LLC for the DOE-NNSA under Contract No. DE-AC52-06NA25396. NV acknowledge funding support from LANL Science Programs 1 and 2. Portions of this work were performed at HPCAT (Sector 16), Advanced Photon Source (APS), Argonne National Laboratory. HPCAT operations are supported by DOE-NNSA under Award No. DE-NA0001974 and DOE-BES under Award No. DE-FG02-99ER45775, with partial instrumentation funding by NSF. APS is supported by DOE-BES, under Contract No. DE-AC02-06CH11357.

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