1985
DOI: 10.1016/0012-821x(85)90064-0
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Shock behavior of zircon: phase transition to scheelite structure and decomposition

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Cited by 143 publications
(108 citation statements)
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“…The boundary found in this study is generally consistent with the large-volume press experiments using the heated method (Reid and Ringwood 1969;Tange and Takahashi 2002), and with the boundary estimated by Ono et al (2004), who used the laser-heated diamond anvil cell method combined with synchrotron X-rays. However, the boundary in this study disagrees with those determined by room-temperature compression (Knittle and Williams 1993;van Westrenen et al 2004) and shock compression studies (Kusaba et al 1985). These studies indicated much higher transition pressures than that indicated by our results, and there is also a large discrepancy among them.…”
contrasting
confidence: 99%
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“…The boundary found in this study is generally consistent with the large-volume press experiments using the heated method (Reid and Ringwood 1969;Tange and Takahashi 2002), and with the boundary estimated by Ono et al (2004), who used the laser-heated diamond anvil cell method combined with synchrotron X-rays. However, the boundary in this study disagrees with those determined by room-temperature compression (Knittle and Williams 1993;van Westrenen et al 2004) and shock compression studies (Kusaba et al 1985). These studies indicated much higher transition pressures than that indicated by our results, and there is also a large discrepancy among them.…”
contrasting
confidence: 99%
“…The pressure discrepancy between this study and room-temperature compression experiments (Knittle and Williams 1993;van Westrenen et al 2004) indicates that the high-temperature heating played a fundamental role in overcoming kinetic effects of the phase transition from zircon to reidite. In the case of the shock experiments (Kusaba et al 1985), the duration at high-pressure and high-temperature was much shorter than that of the static compression experiment. It is generally accepted that the shock experiments is not a suitable method for the determination of the phase boundary.…”
mentioning
confidence: 79%
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“…(ii) static experiments show that this transformation is observed at pressures in the range [10][11][12][13][14][15] GPa when temperature is increased up to 1000-1500 K [10][11][12], whereas at room temperature the transition is also possible if pressure is increased up to approximately 20-23 GPa [13,14], (iii) shock wave studies found this transformation to occur very fast (microsecond time scale), and at much higher pressures (30-50 GPa) [9,15,16], (iv) zircon → reidite transformation exhibits large hysteresis, zircon is not recoverable from reidite at zero pressure unless heated up to 1273 K [15], and (v) the thermodynamic boundary presents a positive Clapeyron slope [17].…”
Section: Thermodynamics and Thermal Barriers Of The Zircon-reidimentioning
confidence: 99%
“…Static-pressure 1,3,4,9,10 and shock-wave compression [11][12][13] experiments have identified reidite as the only high-pressure polymorph of ZrSiO 4 . At elevated temperature and pressure, ZrSiO 4 is observed to decompose into SiO 2 ͑stishovite͒ and ZrO 2 ͑cottunite͒.…”
Section: Introductionmentioning
confidence: 99%