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• W1991394464 abstract "The equilibrium phase boundary between the $B1$ and $B2$ phases in NaCl was determined at temperatures between 1150 and 2000 K by in situ x-ray diffraction, using a Kawai-type apparatus in a beam line of SPring-8, Hyogo, Japan. The press was oscillated during data acquisition in order to reduce the effect of grain growth on the diffraction pattern of NaCl at high temperature, obtained by the energy-dispersive method with a fixed angle. Forward $(B1$ to $B2)$ and backward $(B2$ to $B1)$ transitions were observed independently at temperatures between 1150 and 1600 K; the $Pensuremath{-}T$ conditions where these transitions occur fall on a straight line, indicating that there is no kinetic effect between the forward and the backward transitions over this temperature range. The equilibrium phase boundary is represented by the linear equation $P$ $(mathrm{in}mathrm{}mathrm{GPa})=30.6(2)--0.0053(2)$ $T$ (in K). Liquid NaCl was observed at 20.1 GPa and 2100 K, consistent with the melting curve obtained in a previous study using a laser- heated diamond anvil cell. According to our experimental results, the triple point between $B1,$ $B2,$ and liquid NaCl would be located at $19.7ifmmodepmelsetextpmfi{}0.5mathrm{GPa}$ and $2050ifmmodepmelsetextpmfi{}50mathrm{K}.$" @default.
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• W1991394464 date "2003-10-17" @default.
• W1991394464 modified "2023-09-25" @default.
• W1991394464 title "Determination of the phase boundary between the<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mi>B</mml:mi><mml:mn>1</mml:mn><mml:mn /></mml:math>and<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mi>B</mml:mi><mml:mn>2</mml:mn><mml:mn /></mml:math>phases in NaCl by<i>in situ</i>x-ray diffraction" @default.
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• W1991394464 doi "https://doi.org/10.1103/physrevb.68.134109" @default.
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