X-ray diffraction of solid tin to 1.2 TPa

Lazicki, A.; Rygg, J. R.; Coppari, F.; Smith, R.; Fratanduono, D.; Kraus, R. G.; Collins, G. W.; Briggs, R.; Braun, D. G.; Swift, D. C.; Eggert, J. H.

doi:10.1103/PhysRevLett.115.075502

Title: X-ray diffraction of solid tin to 1.2 TPa

Journal Article · Wed Aug 12 00:00:00 EDT 2015 · Physical Review Letters

DOI:https://doi.org/10.1103/PhysRevLett.115.075502· OSTI ID:1249158

Lazicki, A. ^[1]; Rygg, J. R. ^[1]; Coppari, F. ^[1]; Smith, R. ^[1]; Fratanduono, D. ^[1]; Kraus, R. G. ^[1]; Collins, G. W. ^[1]; Briggs, R. ^[2]; Braun, D. G. ^[1]; Swift, D. C. ^[1]; Eggert, J. H. ^[1]

Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States)
The Univ. of Edinburgh, Edinburgh (United Kingdom)

In this study, we report direct in situ measurements of the crystal structure of tin between 0.12 and 1.2 TPa, the highest stress at which a crystal structure has ever been observed. Using angle-dispersive powder x-ray diffraction, we find that dynamically compressed Sn transforms to the body-centered-cubic (bcc) structure previously identified by ambient-temperature quasistatic-compression studies and by zero-kelvin density-functional theory predictions between 0.06 and 0.16 TPa. However, we observe no evidence for the hexagonal close-packed (hcp) phase found by those studies to be stable above 0.16 TPa. Instead, our results are consistent with bcc up to 1.2 TPa. We conjecture that at high temperature bcc is stabilized relative to hcp due to differences in vibrational free energy.

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Research Organization:: Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States)

Sponsoring Organization:: USDOE

Grant/Contract Number:: AC52-07NA27344

OSTI ID:: 1249158

Alternate ID(s):: OSTI ID: 1210005

Report Number(s):: LLNL-JRNL-673348; PRLTAO

Journal Information:: Physical Review Letters, Vol. 115, Issue 7; ISSN 0031-9007

Publisher:: American Physical Society (APS)Copyright Statement

Country of Publication:: United States

Language:: English

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Cited by: 45 works

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