Phase transition lowering in dynamically compressed silicon
- Authors:
-
[1];
[2];
[3];
- Deutsches Elektronen-Synchrotron (DESY), Hamburg (Germany); SLAC National Accelerator Lab., Menlo Park, CA (United States); European XFEL GmbH, Hamburg (Germany)
- IMPMC, UPMC, MNHN, IRD, Paris (France)
- Deutsches Elektronen-Synchrotron (DESY), Hamburg (Germany)
- SLAC National Accelerator Lab., Menlo Park, CA (United States)
- Deutsches Elektronen-Synchrotron (DESY), Hamburg (Germany); European XFEL GmbH, Hamburg (Germany)
- Helmholtz-Zentrum Dresden-Rossendorf, Dresden (Germany)
- Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States)
- Rutherford Appleton Lab., Didcot (United Kingdom)
- European XFEL GmbH, Schenefeld (Germany)
- Univ. of Oxford, Oxford (United Kingdom)
- Univ. of York, York (United Kingdom)
- Publication Date:
- Research Org.:
- Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States); SLAC National Accelerator Lab., Menlo Park, CA (United States). Linac Coherent Light Source (LCLS)
- Sponsoring Org.:
- USDOE National Nuclear Security Administration (NNSA); Engineering and Physical Sciences Research Council (EPSRC); French Agence Nationale de la Recherche (ANR); USDOE Office of Science (SC), Fusion Energy Sciences (FES)
- OSTI Identifier:
- 1483786
- Alternate Identifier(s):
- OSTI ID: 1874865
- Report Number(s):
- LLNL-JRNL-830710
Journal ID: ISSN 1745-2473; PII: 290
- Grant/Contract Number:
- AC02-76SF00515; AC52-07NA27344; EP/J017256/1; ANR IRONFEL 12-PDOC-0011
- Resource Type:
- Accepted Manuscript
- Journal Name:
- Nature Physics
- Additional Journal Information:
- Journal Volume: 15; Journal ID: ISSN 1745-2473
- Publisher:
- Nature Publishing Group (NPG)
- Country of Publication:
- United States
- Language:
- English
- Subject:
- 36 MATERIALS SCIENCE
Citation Formats
McBride, E. E., Krygier, A., Ehnes, A., Galtier, E., Harmand, M., Konôpková, Z., Lee, H. J., Liermann, H. -P., Nagler, B., Pelka, A., Rödel, M., Schropp, A., Smith, R. F., Spindloe, C., Swift, D., Tavella, F., Toleikis, S., Tschentscher, T., Wark, J. S., and Higginbotham, A. Phase transition lowering in dynamically compressed silicon. United States: N. p., 2018.
Web. doi:10.1038/s41567-018-0290-x.
McBride, E. E., Krygier, A., Ehnes, A., Galtier, E., Harmand, M., Konôpková, Z., Lee, H. J., Liermann, H. -P., Nagler, B., Pelka, A., Rödel, M., Schropp, A., Smith, R. F., Spindloe, C., Swift, D., Tavella, F., Toleikis, S., Tschentscher, T., Wark, J. S., & Higginbotham, A. Phase transition lowering in dynamically compressed silicon. United States. https://doi.org/10.1038/s41567-018-0290-x
McBride, E. E., Krygier, A., Ehnes, A., Galtier, E., Harmand, M., Konôpková, Z., Lee, H. J., Liermann, H. -P., Nagler, B., Pelka, A., Rödel, M., Schropp, A., Smith, R. F., Spindloe, C., Swift, D., Tavella, F., Toleikis, S., Tschentscher, T., Wark, J. S., and Higginbotham, A. Mon .
"Phase transition lowering in dynamically compressed silicon". United States. https://doi.org/10.1038/s41567-018-0290-x. https://www.osti.gov/servlets/purl/1483786.
@article{osti_1483786,
title = {Phase transition lowering in dynamically compressed silicon},
author = {McBride, E. E. and Krygier, A. and Ehnes, A. and Galtier, E. and Harmand, M. and Konôpková, Z. and Lee, H. J. and Liermann, H. -P. and Nagler, B. and Pelka, A. and Rödel, M. and Schropp, A. and Smith, R. F. and Spindloe, C. and Swift, D. and Tavella, F. and Toleikis, S. and Tschentscher, T. and Wark, J. S. and Higginbotham, A.},
abstractNote = {},
doi = {10.1038/s41567-018-0290-x},
journal = {Nature Physics},
number = ,
volume = 15,
place = {United States},
year = {2018},
month = {9}
}
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Cited by: 7 works
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Figures / Tables:
FIG. 1: Experimental configuration and data examples: a the transverse configuration whereby the compression laser was perpendicular to the X-ray beam. b Velocimetry data (VISAR) lineouts showing free surface velocity (Umore »). Laser intensity increases to the right. Dashed lines indicate the onset of the 2nd and 3rd wave. c Azimuthally integrated 1D diffraction patterns as a function of increasing laser intensity and hence increasing pressure in both the transverse: (i), (ii), (iv), (v), (ix) and collinear (iii), (vi), (vii), (viii) configurations. Peaks marked with the * symbol belong to the compressed cubic diamond phase. Peaks marked with the † symbol cannot be described by the cubic diamond, $β$-tin, $I$$mma$, or simple hexagonal phases.
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