Poly-a-morphism is the amorphous analogue of polymorphism observed in crystals. It is the idea that there can exist multiple, structurally distinct amorphous forms of the same material, between which there is a first order-like phase transition. Polyamorphism and the related amorphous-amorphous transitions is a subject of much debate. Several liquid and glassy materials (including H2O) have been reported to exist in different density states under extremes of temperature and pressure. One such system that we have studied is Y2O3-Al2O3 glasses [1].
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Some important unanswered questions that surround polyamorphism and the corresponding liquid-liquid, or amorphous-amorphous phase transitions are:
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Top - samples produced by levitation. left to right Y2O3 content is 20, 24, 30, 37.5, 41 mol%. Two extreme samples are completetly crystalline the central sample is single phase glass. The 24 and 37.5 samples are both turbid. Bottom - phase contrast optical microscope images, AY37.5 contains inclusions (shown to be crystalline by X-ray diffraaction) whereas the AY24 sample does not contain inclusions. The intresting question is then what is causing the turbity, is it the beginnings of density driven phase separation (i.e. polyamorphism) or composiotnally driven separation, that has been arrested on cooling. |
With our work on Aluminate glasses, we aim to, learn about the structural and dynamical changes that accompany polyamorphism, allowing us to contribute towards answering some of these important questions.
[1] L.B. Skinner, A.C. Barnes, P.S. Salmon & W.A. Crichton, Phase separation, crystallisation and polyamorphism in the Y2O3-Al2O3 system. J. Phys.: Condens. Matter 20, 205103 (2008).