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Brillouin Scattering With Simultaneous X-Ray Diffraction at GSECARS, Advanced Photon Source: Toward Determination of Absolute Pressure Scales Jay Bass 1 Stanislav Sinogeikin 1,2 Dmitry Lakshtanov 1 Carmen Sanchez-Valle 1 Vitali Prakapenka 2, Guoyin Shen 2,3 Jean-Philippe Perrillat 1 Jingyun Wang 1 Bin Chen 1 1 University of Illinois at UC, Geology Dept. 2 GSECARS, The University of Chicago 3 HPCAT, Advanced Photon Sourse, Argonne National Laboratory 4 Carnegie Institution of Washington, Geophysical Laboratory Fall AGU 2006
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Isothermal bulk modulus (volume measurements) Adiabatic elastic moduli (velocity measurements) Brillouin Scattering with synchrotron X-rays at the APS Elasticity Grand Challenge COMPRES Infrastructure Development Project Measure sound velocities and density simultaneously “ Absolute” or internally consistent Pressure Scales Zha et al., Brillouin on MgO (PNAS, 2000)
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Phase Transitions: Stishovite - CaCl 2
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Stishovite - CaCl 2 : Brillouin scattering velocities
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Brillouin scattering Acoustic waves present in a solid due to thermal motion of atoms Laser light interacts with phonons (or density / refractive index fluctuations) and is scattered with Doppler shifted frequency Brillouin shift is proportional to acoustic velocity V i = / 2n*sin ( /2) V i = / 2sin ( */2) Platelet (symmetric) geometry
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Schematic diagram of the Brillouin system installed at sector 13-BMD (GSECARS) at APS Sinogeikin et al.,Rev. Sci. Instr. 77, 2006
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Schematic diagram of the Brillouin system installed at sector 13-BMD at APS (Lower Tier) Motorized translation components (controllable from outside the hatch, blue boxes): HMTS - horizontal motorized translation stage; VMTS - vertical motorized translation stage; MLFA - motorized laser focusing assembly; MSCA - motorized signal collecting assembly; SPOA - sample positioning and orientation assembly; SL-LB - sample light / light block. Observation / feedback elements (red boxes): VC - video camera; BT - beam target. X-ray components: MAR - MAR Imaging plate; XBS - X-ray beam stop; CS - cleanup slit.
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Mobile focusing/collecting part of the Brillouin system at 13-BMD GSECARS
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X-ray image and integrated spectrum of single-crystal NaCl at ambient conditions
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Single crystal NaCl (B1) at ~30 GPa in DAC in Ne pressure medium Au+Pt+NaCl NaCl Single crystal Ruby 100 μm Au+Pt+NaCl Schematic view of simultaneous Brillouin scattering and X-ray diffraction in DAC
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X-ray image and spectrum of single-crystal NaCl in Ne at 30 GPa NaCl (B1) (200) Ne
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Single crystal Brillouin spectrum of NaCl (B1) and velocity distribution in (100) plane at 30.5 GPa
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Single crystal and aggregate elastic moduli of NaCl (B1) as a function of density
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Anisotropy of NaCl (B1) to 30 GPa
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Aggregate velocities of NaCl (B1) as a function of density
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“Absolute” equations of state / pressure scale Isothermal bulk modulus (volume measurements) Adiabatic elastic moduli (velocity measurements) We measure Ks as a function of volume directly. The problem is to convert K S to K T at high pressure, e.g. we need to know volume dependence of and . Possible models/assumptions:
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Conclusions We simultaneously measured single crystal (and aggregate) elastic moduli of NaCl (B1) with Brillouin spectroscopy and density with angle dispersive X-ray diffraction to 30.5 GPa. At high pressure NaCl exhibits extreme elastic anisotropy, which is >3 times higher than that at ambient conditions. Above ~17 GPa on approaching B1-B2 phase transition NaCl exhibits acoustic mode softening. Above ~17 GPa the density – velocity relations deviate from linearity and violate Birch’s law. Acoustic softening indicates that B1-B2 phase transition in NaCl may be multi-step and of more complicated nature than it was previously thought. Pressure calculated from measured bulk modulus and density is higher than that calculated from Decker EOS by ~ 3-5% at 30 GPa.
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Acknowledgments NSF: Elasticity Grand Challenge COMPRES: Infrastructure development project GSECARS: Sector 13, Advanced Photon Source
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