Pressure-induced structural transformations in In sub(2-x)Y sub(x)(MoO sub(4)) sub(3) systems

In this work, we report results of high-pressure Raman experiments (P

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Veröffentlicht in:Journal of Raman spectroscopy 2016-03, Vol.47 (3), p.350-356
Hauptverfasser: Mendonca, R, Paraguassu, W, Mendes Filho, J, Marinkovic, BA, Souza Filho, AG, Maczka, M, Freire, PTC
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container_end_page 356
container_issue 3
container_start_page 350
container_title Journal of Raman spectroscopy
container_volume 47
creator Mendonca, R
Paraguassu, W
Mendes Filho, J
Marinkovic, BA
Souza Filho, AG
Maczka, M
Freire, PTC
description In this work, we report results of high-pressure Raman experiments (P
doi_str_mv 10.1002/jrs.4814
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A crystalline to crystalline structural phase transition and pressure-induced amorphization (PIA) have been identified. The structural phase transition takes place at 1.5 and 1.0GPa for In sub(2)(MoO sub(4)) sub(3 ) and In sub(1.5)Y sub(0.5)(MoO sub(4)) sub(3), respectively, resulting in the change of structure from monoclinic P2 sub(1)/a to a more denser structure. The PIA started at 5 and 3.4GPa for In sub(2)Mo sub(3)O sub(12) and In sub(1.5)Y sub(0.5)Mo sub(3)O sub(12), respectively. The amorphization process takes place in two stages in the case of In sub(1.5)Y sub(0.5)Mo sub(3)O sub(12) phase, while for In sub(2)Mo sub(3)O sub(12), it is not complete until the pressure is as high as 7GPa. Our results also suggest that with increase of ionic size of the A super(3+) ions, the octahedral distortion increases and consequently larger local structural disorder is introduced in the A sub(2)(MoO sub(4)) sub(3) system, where A is a trivalent ion (In, Y super(3+), Sc super(3+), Fe super(3+), etc.). High-pressure Raman experiments on In sub(2-x)Y sub(x)Mo sub(3 )O sub(12) reveal a crystalline to crystalline structural phase transition at low-pressure values and a pressure-induced amorphization at higher pressures. The first transformation leads the structure from monoclinic P2 sub(1)/a to a more denser structure. The amorphization process takes place in two stages for In sub(1.5)Y sub(0.5)Mo sub(3)O sub(12), while for In sub(2)Mo sub(3)O sub(12), it is not complete until the pressure is as high as 7GPa. 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A crystalline to crystalline structural phase transition and pressure-induced amorphization (PIA) have been identified. The structural phase transition takes place at 1.5 and 1.0GPa for In sub(2)(MoO sub(4)) sub(3 ) and In sub(1.5)Y sub(0.5)(MoO sub(4)) sub(3), respectively, resulting in the change of structure from monoclinic P2 sub(1)/a to a more denser structure. The PIA started at 5 and 3.4GPa for In sub(2)Mo sub(3)O sub(12) and In sub(1.5)Y sub(0.5)Mo sub(3)O sub(12), respectively. The amorphization process takes place in two stages in the case of In sub(1.5)Y sub(0.5)Mo sub(3)O sub(12) phase, while for In sub(2)Mo sub(3)O sub(12), it is not complete until the pressure is as high as 7GPa. Our results also suggest that with increase of ionic size of the A super(3+) ions, the octahedral distortion increases and consequently larger local structural disorder is introduced in the A sub(2)(MoO sub(4)) sub(3) system, where A is a trivalent ion (In, Y super(3+), Sc super(3+), Fe super(3+), etc.). High-pressure Raman experiments on In sub(2-x)Y sub(x)Mo sub(3 )O sub(12) reveal a crystalline to crystalline structural phase transition at low-pressure values and a pressure-induced amorphization at higher pressures. The first transformation leads the structure from monoclinic P2 sub(1)/a to a more denser structure. The amorphization process takes place in two stages for In sub(1.5)Y sub(0.5)Mo sub(3)O sub(12), while for In sub(2)Mo sub(3)O sub(12), it is not complete until the pressure is as high as 7GPa. 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A crystalline to crystalline structural phase transition and pressure-induced amorphization (PIA) have been identified. The structural phase transition takes place at 1.5 and 1.0GPa for In sub(2)(MoO sub(4)) sub(3 ) and In sub(1.5)Y sub(0.5)(MoO sub(4)) sub(3), respectively, resulting in the change of structure from monoclinic P2 sub(1)/a to a more denser structure. The PIA started at 5 and 3.4GPa for In sub(2)Mo sub(3)O sub(12) and In sub(1.5)Y sub(0.5)Mo sub(3)O sub(12), respectively. The amorphization process takes place in two stages in the case of In sub(1.5)Y sub(0.5)Mo sub(3)O sub(12) phase, while for In sub(2)Mo sub(3)O sub(12), it is not complete until the pressure is as high as 7GPa. Our results also suggest that with increase of ionic size of the A super(3+) ions, the octahedral distortion increases and consequently larger local structural disorder is introduced in the A sub(2)(MoO sub(4)) sub(3) system, where A is a trivalent ion (In, Y super(3+), Sc super(3+), Fe super(3+), etc.). High-pressure Raman experiments on In sub(2-x)Y sub(x)Mo sub(3 )O sub(12) reveal a crystalline to crystalline structural phase transition at low-pressure values and a pressure-induced amorphization at higher pressures. The first transformation leads the structure from monoclinic P2 sub(1)/a to a more denser structure. The amorphization process takes place in two stages for In sub(1.5)Y sub(0.5)Mo sub(3)O sub(12), while for In sub(2)Mo sub(3)O sub(12), it is not complete until the pressure is as high as 7GPa. With increase of ionic size of the trivalent cation, the octahedral distortion increases.</abstract><doi>10.1002/jrs.4814</doi></addata></record>
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subjects Amorphization
Cations
Crystal structure
Disorders
Distortion
Phase transformations
Raman spectroscopy
Transformations
title Pressure-induced structural transformations in In sub(2-x)Y sub(x)(MoO sub(4)) sub(3) systems
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