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层状晶体的光声光谱:光声信号的增强及其从热产生角度的分析。

Photoacoustic spectroscopy of layered crystals: An enhancement of the photoacoustic signal and its analysis from the perspective of heat generation.

作者信息

Misztal Kamil, Kopaczek Jan, Kudrawiec Robert

机构信息

Department of Semiconductor Materials Engineering, Wrocław University of Science and Technology, Wybrzeże Stanisława Wyspiańskiego 27, Wrocław 50-370, Poland.

出版信息

Photoacoustics. 2024 Nov 13;41:100668. doi: 10.1016/j.pacs.2024.100668. eCollection 2025 Feb.

DOI:10.1016/j.pacs.2024.100668
PMID:39640434
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11617410/
Abstract

Photoacoustic spectroscopy is a powerful tool for investigating semiconductors and determining some of their basic properties. However, generating a signal that is large enough for the investigated samples is still challenging. To address this, the focus is on enhancing photoacoustic (PA) signal intensity in a non-complex way, which does not require changing any part of an experimental setup. The PA signal intensity enhancement is mainly achieved by manipulating the sample volume and its surroundings. MoS, a layered material that belongs to the van der Waals crystals was selected due to ease of exfoliation to the proper thickness. A reduction in MoS thickness from 112 to 7 µm, resulted in enhancement of the PA signal by a factor of ∼50. A simple model has been proposed to describe the results based on thermal processes. Additionally, a method to determine the energy gap in transition metal dichalcogenides from PA measurements is presented.

摘要

光声光谱法是研究半导体及其某些基本性质的有力工具。然而,为被研究样品生成足够大的信号仍然具有挑战性。为了解决这个问题,重点是以一种不复杂的方式增强光声(PA)信号强度,这不需要改变实验装置的任何部分。PA信号强度的增强主要通过控制样品体积及其周围环境来实现。由于易于剥离到合适的厚度,选择了属于范德华晶体的层状材料二硫化钼(MoS)。二硫化钼厚度从112微米减小到7微米,导致PA信号增强了约50倍。已经提出了一个基于热过程的简单模型来描述这些结果。此外,还提出了一种从PA测量中确定过渡金属二硫属化物能隙的方法。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4945/11617410/e62ae0e039b5/gr9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4945/11617410/72f94fe8a153/gr1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4945/11617410/1b87ffe658a9/gr2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4945/11617410/ca09377e3ffa/gr3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4945/11617410/e60f8274f36d/gr4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4945/11617410/c0dbbbd4b9a0/gr5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4945/11617410/2b71944bae27/gr6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4945/11617410/2829119b5481/gr7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4945/11617410/62c482e8bea5/gr8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4945/11617410/e62ae0e039b5/gr9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4945/11617410/72f94fe8a153/gr1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4945/11617410/1b87ffe658a9/gr2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4945/11617410/ca09377e3ffa/gr3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4945/11617410/e60f8274f36d/gr4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4945/11617410/c0dbbbd4b9a0/gr5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4945/11617410/2b71944bae27/gr6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4945/11617410/2829119b5481/gr7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4945/11617410/62c482e8bea5/gr8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4945/11617410/e62ae0e039b5/gr9.jpg

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