Micro-Structure Changes Caused by Thermal Evolution in Chalcogenide Ge<sub>x</sub>As<sub>y</sub>Se<sub>1−x−y</sub> Thin Films by In Situ Measurements
To understand the effects of thermal annealing on the structure of Ge<sub>x</sub>As<sub>y</sub>Se<sub>1−x−y</sub> thin films, the thermal evolution of these films was measured by the in situ X-ray diffraction (XRD) at different temperature (773 K or 1073 K) in a v...
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doaj-426105ec08eb496b868985e5e655bbc72021-06-01T00:07:49ZengMDPI AGMaterials1996-19442021-05-01142572257210.3390/ma14102572Micro-Structure Changes Caused by Thermal Evolution in Chalcogenide Ge<sub>x</sub>As<sub>y</sub>Se<sub>1−x−y</sub> Thin Films by In Situ MeasurementsXueqiong Su0Yong Pan1Dongwen Gao2Shufeng Li3Jin Wang4Rongping Wang5Li Wang6College of Applied Sciences, Beijing University of Technology, Beijing 100124, ChinaCollege of Applied Sciences, Beijing University of Technology, Beijing 100124, ChinaCollege of Applied Sciences, Beijing University of Technology, Beijing 100124, ChinaCollege of Applied Sciences, Beijing University of Technology, Beijing 100124, ChinaCollege of Applied Sciences, Beijing University of Technology, Beijing 100124, ChinaCentre for Ultra-High Bandwidth Devices for Optical Systems, Laser Physics Centre, Australian National University, ACT, 2600 Canberra, AustraliaCollege of Applied Sciences, Beijing University of Technology, Beijing 100124, ChinaTo understand the effects of thermal annealing on the structure of Ge<sub>x</sub>As<sub>y</sub>Se<sub>1−x−y</sub> thin films, the thermal evolution of these films was measured by the in situ X-ray diffraction (XRD) at different temperature (773 K or 1073 K) in a vacuum (10<sup>−1</sup> Pa) environment. The entire process of crystallization can be observed by using in situ XRD, which is from the appearance of a crystal structure to melting liquid-state and ultimately to the disappearance of the amorphous structure. In the crystallized process, the corresponding state-transition temperatures T<sub>x</sub> (the onset crystallization temperature), T<sub>l</sub> (the transition temperature from glassy-state to liquid-state), T<sub>p</sub> (peak crystallization temperature) are linear with MCN (Mean Coordination Number). In order to obtain information about changes in the amorphous structural origin of the anneal-induced material, the samples were analyzed by in situ Raman spectroscopy. Analysis of the results through decomposing the Raman spectra into different structural units showed that the Ge−Ge, As−As, or Se−Se homopolar bonds as the nonequilibrium minority carriers could be found in films. It suggests that the formation of these bonds cannot be completely suppressed in any case, as one falls and another rises.https://www.mdpi.com/1996-1944/14/10/2572chalcogenide glassesGe<sub>x</sub>As<sub>y</sub>Se<sub>1−x−y</sub>conduction mechanismselectrical conductivity |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Xueqiong Su Yong Pan Dongwen Gao Shufeng Li Jin Wang Rongping Wang Li Wang |
spellingShingle |
Xueqiong Su Yong Pan Dongwen Gao Shufeng Li Jin Wang Rongping Wang Li Wang Micro-Structure Changes Caused by Thermal Evolution in Chalcogenide Ge<sub>x</sub>As<sub>y</sub>Se<sub>1−x−y</sub> Thin Films by In Situ Measurements Materials chalcogenide glasses Ge<sub>x</sub>As<sub>y</sub>Se<sub>1−x−y</sub> conduction mechanisms electrical conductivity |
author_facet |
Xueqiong Su Yong Pan Dongwen Gao Shufeng Li Jin Wang Rongping Wang Li Wang |
author_sort |
Xueqiong Su |
title |
Micro-Structure Changes Caused by Thermal Evolution in Chalcogenide Ge<sub>x</sub>As<sub>y</sub>Se<sub>1−x−y</sub> Thin Films by In Situ Measurements |
title_short |
Micro-Structure Changes Caused by Thermal Evolution in Chalcogenide Ge<sub>x</sub>As<sub>y</sub>Se<sub>1−x−y</sub> Thin Films by In Situ Measurements |
title_full |
Micro-Structure Changes Caused by Thermal Evolution in Chalcogenide Ge<sub>x</sub>As<sub>y</sub>Se<sub>1−x−y</sub> Thin Films by In Situ Measurements |
title_fullStr |
Micro-Structure Changes Caused by Thermal Evolution in Chalcogenide Ge<sub>x</sub>As<sub>y</sub>Se<sub>1−x−y</sub> Thin Films by In Situ Measurements |
title_full_unstemmed |
Micro-Structure Changes Caused by Thermal Evolution in Chalcogenide Ge<sub>x</sub>As<sub>y</sub>Se<sub>1−x−y</sub> Thin Films by In Situ Measurements |
title_sort |
micro-structure changes caused by thermal evolution in chalcogenide ge<sub>x</sub>as<sub>y</sub>se<sub>1−x−y</sub> thin films by in situ measurements |
publisher |
MDPI AG |
series |
Materials |
issn |
1996-1944 |
publishDate |
2021-05-01 |
description |
To understand the effects of thermal annealing on the structure of Ge<sub>x</sub>As<sub>y</sub>Se<sub>1−x−y</sub> thin films, the thermal evolution of these films was measured by the in situ X-ray diffraction (XRD) at different temperature (773 K or 1073 K) in a vacuum (10<sup>−1</sup> Pa) environment. The entire process of crystallization can be observed by using in situ XRD, which is from the appearance of a crystal structure to melting liquid-state and ultimately to the disappearance of the amorphous structure. In the crystallized process, the corresponding state-transition temperatures T<sub>x</sub> (the onset crystallization temperature), T<sub>l</sub> (the transition temperature from glassy-state to liquid-state), T<sub>p</sub> (peak crystallization temperature) are linear with MCN (Mean Coordination Number). In order to obtain information about changes in the amorphous structural origin of the anneal-induced material, the samples were analyzed by in situ Raman spectroscopy. Analysis of the results through decomposing the Raman spectra into different structural units showed that the Ge−Ge, As−As, or Se−Se homopolar bonds as the nonequilibrium minority carriers could be found in films. It suggests that the formation of these bonds cannot be completely suppressed in any case, as one falls and another rises. |
topic |
chalcogenide glasses Ge<sub>x</sub>As<sub>y</sub>Se<sub>1−x−y</sub> conduction mechanisms electrical conductivity |
url |
https://www.mdpi.com/1996-1944/14/10/2572 |
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