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27至350K温度范围内α-SnS的介电函数和临界点的温度依赖性

Temperature dependence of the dielectric function and critical points of α-SnS from 27 to 350 K.

作者信息

Nguyen Hoang Tung, Le Van Long, Nguyen Thi Minh Hai, Kim Tae Jung, Nguyen Xuan Au, Kim Bogyu, Kim Kyujin, Lee Wonjun, Cho Sunglae, Kim Young Dong

机构信息

Department of Physics, Kyung Hee University, Seoul, 02447, Republic of Korea.

Institute of Materials Science, Vietnam Academy of Science and Technology, Hanoi, 100000, Vietnam.

出版信息

Sci Rep. 2020 Oct 27;10(1):18396. doi: 10.1038/s41598-020-75383-0.

DOI:10.1038/s41598-020-75383-0
PMID:33110190
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7591561/
Abstract

We report the temperature dependence of the dielectric function ε = ε + iε and critical point (CP) energies of biaxial α-SnS in the spectral energy region from 0.74 to 6.42 eV and temperatures from 27 to 350 K using spectroscopic ellipsometry. Bulk SnS was grown by temperature gradient method. Dielectric response functions were obtained using multilayer calculations to remove artifacts due to surface roughness. We observe sharpening and blue-shifting of CPs with decreasing temperature. A strong exciton effect is detected only in the armchair direction at low temperature. New CPs are observed at low temperature that cannot be detected at room temperature. The temperature dependences of the CP energies were determined by fitting the data to the phenomenological expression that contains the Bose-Einstein statistical factor and the temperature coefficient for describing the electron-phonon interaction.

摘要

我们使用光谱椭偏仪报告了双轴α-SnS在0.74至6.42电子伏特的光谱能量区域以及27至350开尔文温度下的介电函数ε = ε + iε和临界点(CP)能量的温度依赖性。通过温度梯度法生长块状SnS。使用多层计算获得介电响应函数,以消除由于表面粗糙度引起的伪影。我们观察到随着温度降低,CPs出现锐化和蓝移。仅在低温下的扶手椅方向检测到强烈的激子效应。在低温下观察到新的CPs,而在室温下无法检测到。通过将数据拟合到包含玻色-爱因斯坦统计因子和用于描述电子-声子相互作用的温度系数的唯象表达式中来确定CP能量的温度依赖性。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5aac/7591561/c0960f334260/41598_2020_75383_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5aac/7591561/d7a3eb2933b2/41598_2020_75383_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5aac/7591561/bc0673b6319e/41598_2020_75383_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5aac/7591561/eb9f17bfd3ba/41598_2020_75383_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5aac/7591561/43f768fb7c5c/41598_2020_75383_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5aac/7591561/c0960f334260/41598_2020_75383_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5aac/7591561/d7a3eb2933b2/41598_2020_75383_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5aac/7591561/bc0673b6319e/41598_2020_75383_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5aac/7591561/eb9f17bfd3ba/41598_2020_75383_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5aac/7591561/43f768fb7c5c/41598_2020_75383_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5aac/7591561/c0960f334260/41598_2020_75383_Fig5_HTML.jpg

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