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The absorbed laser energy was measured by subtracting the reflected laser energy from the incident energy. The absorbed fluence was then computed with knowledge of the laser intensity profile. This measurement takes into account the optical properties of bismuth for the particular incidence angle and laser polarization used. Only the incident fluence was stated in many of the cited references, and therefore the optical properties of bismuth must be taken into account before directly comparing the results
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The absorbed laser energy was measured by subtracting the reflected laser energy from the incident energy. The absorbed fluence was then computed with knowledge of the laser intensity profile. This measurement takes into account the optical properties of bismuth for the particular incidence angle and laser polarization used. Only the incident fluence was stated in many of the cited references, and therefore the optical properties of bismuth must be taken into account before directly comparing the results.
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18
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33846862281
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An experimental ambiguity regarding the room temperature equilibrium position exists: A measurement of 0.4668 was cited in (14) and 0.46814 was cited in 15, The chosen value of 0.46719, the equilibrium value determined by DFT, was used to best compare experimental results to DFT calculations
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An experimental ambiguity regarding the room temperature equilibrium position exists: A measurement of 0.4668 was cited in (14) and 0.46814 was cited in (15). The chosen value of 0.46719, the equilibrium value determined by DFT, was used to best compare experimental results to DFT calculations.
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19
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33846881385
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This phase transition is distinct from the Bi I-II transition that occurs at 25.3 kbar of hydrostatic pressure 26
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This phase transition is distinct from the Bi I-II transition that occurs at 25.3 kbar of hydrostatic pressure (26).
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24
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27
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33846892065
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Portions of this research were supported by the U.S. Department of Energy, Office of Basic Energy Science through direct support for the SPPS and individual investigators and through the Stanford Synchrotron Radiation Laboratory, a national user facility operated by Stanford University, and the University of California Lawrence Livermore National Laboratory. Additional support for the construction of SPPS was provided by Uppsala University through a grant from the Swedish Research Council. E.D.M. is supported by the Irish Research Council for Science, Engineering, and Technology, S.F. by Science Foundation Ireland, and J.K. by the Keck Foundation. M.N, K.S.T. and D.V.D.L. gratefully acknowledge support by the Deutsche Forschungsgemeinschaft and the European Union [Research Training Network (RTN) Free-electron Laser in Hamburg FLASH, R.K. acknowledges a fellowship of the Austrian Academy of Sciences. D.M.F. and D.A.R. were supported by the NSF FOCUS frontier center and Stanford PULS
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Portions of this research were supported by the U.S. Department of Energy, Office of Basic Energy Science through direct support for the SPPS and individual investigators and through the Stanford Synchrotron Radiation Laboratory, a national user facility operated by Stanford University, and the University of California Lawrence Livermore National Laboratory. Additional support for the construction of SPPS was provided by Uppsala University through a grant from the Swedish Research Council. E.D.M. is supported by the Irish Research Council for Science, Engineering, and Technology, S.F. by Science Foundation Ireland, and J.K. by the Keck Foundation. M.N., K.S.T. and D.V.D.L. gratefully acknowledge support by the Deutsche Forschungsgemeinschaft and the European Union [Research Training Network (RTN) Free-electron Laser in Hamburg (FLASH)]. R.K. acknowledges a fellowship of the Austrian Academy of Sciences. D.M.F. and D.A.R. were supported by the NSF FOCUS frontier center and Stanford PULSE center.
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