Role of Focusing Distance in Picosecond Laser-Induced Cu Plasma Spectra

To study the effects of focusing distance on the characteristics of copper plasma, a picosecond laser is utilized to ablate a pure copper plate to generate a plasma spectrum. Following numerous experiments on the subject, three significant factors are determined: lens focal length, pulse energy, and...

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Main Authors: Linyu Chen, Hu Deng, Zhixiang Wu, Zhonggang Xiong, Jin Guo, Quancheng Liu, Akwasi Danso Samuel, Liping Shang
Format: Article
Language:English
Published: Wiley 2022-01-01
Series:Advances in High Energy Physics
Online Access:http://dx.doi.org/10.1155/2022/4885924
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author Linyu Chen
Hu Deng
Zhixiang Wu
Zhonggang Xiong
Jin Guo
Quancheng Liu
Akwasi Danso Samuel
Liping Shang
author_facet Linyu Chen
Hu Deng
Zhixiang Wu
Zhonggang Xiong
Jin Guo
Quancheng Liu
Akwasi Danso Samuel
Liping Shang
author_sort Linyu Chen
collection DOAJ
description To study the effects of focusing distance on the characteristics of copper plasma, a picosecond laser is utilized to ablate a pure copper plate to generate a plasma spectrum. Following numerous experiments on the subject, three significant factors are determined: lens focal length, pulse energy, and the lens-to-sample distance. These factors are employed to analyze the spectral intensity, plasma temperature, and electron density in the local thermodynamic equilibrium (LTE) and optically thin condition. Due to the shielding effects of mixed plasma, the strongest spectral intensity is achieved in the prefocused case, no matter how much beam irradiance is employed. The more intensive the beam irradiance is, the more the optimal position is distant from the focal point. The variation of plasma temperature and electron density showed a peak in the prefocused case, which is consistent with the trend of spectral intensity. For the case of extremely high irradiance (on the focus), the shielding effects become seriously, and the resultant above three factors decreased sharply. When a longer-focal-length lens is employed, the spectral intensity exhibited an obvious bimodal trend. In the prefocused case, a longer-focal-length lens is helpful to eliminate the effects of the roughness of the target surface compared with a shorter one. Finally, the assumed LTE is validated by McWhirter relation, plasma relaxation time, and diffusion length, and the optically thin condition was also validated by spectral intensity ratio. We hope that this work could be an important reference for the future design of highly optimized experiments for Calibration-Free Laser-Induced Breakdown Spectroscopy (CF-LIBS).
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spelling doaj-art-3882b93442e7488db231a0d6f28fffa22025-02-03T05:53:08ZengWileyAdvances in High Energy Physics1687-73652022-01-01202210.1155/2022/4885924Role of Focusing Distance in Picosecond Laser-Induced Cu Plasma SpectraLinyu Chen0Hu Deng1Zhixiang Wu2Zhonggang Xiong3Jin Guo4Quancheng Liu5Akwasi Danso Samuel6Liping Shang7School of Information EngineeringSchool of Information EngineeringSchool of Information EngineeringSchool of Information EngineeringSchool of Information EngineeringSchool of Information EngineeringSchool of Information EngineeringSchool of Information EngineeringTo study the effects of focusing distance on the characteristics of copper plasma, a picosecond laser is utilized to ablate a pure copper plate to generate a plasma spectrum. Following numerous experiments on the subject, three significant factors are determined: lens focal length, pulse energy, and the lens-to-sample distance. These factors are employed to analyze the spectral intensity, plasma temperature, and electron density in the local thermodynamic equilibrium (LTE) and optically thin condition. Due to the shielding effects of mixed plasma, the strongest spectral intensity is achieved in the prefocused case, no matter how much beam irradiance is employed. The more intensive the beam irradiance is, the more the optimal position is distant from the focal point. The variation of plasma temperature and electron density showed a peak in the prefocused case, which is consistent with the trend of spectral intensity. For the case of extremely high irradiance (on the focus), the shielding effects become seriously, and the resultant above three factors decreased sharply. When a longer-focal-length lens is employed, the spectral intensity exhibited an obvious bimodal trend. In the prefocused case, a longer-focal-length lens is helpful to eliminate the effects of the roughness of the target surface compared with a shorter one. Finally, the assumed LTE is validated by McWhirter relation, plasma relaxation time, and diffusion length, and the optically thin condition was also validated by spectral intensity ratio. We hope that this work could be an important reference for the future design of highly optimized experiments for Calibration-Free Laser-Induced Breakdown Spectroscopy (CF-LIBS).http://dx.doi.org/10.1155/2022/4885924
spellingShingle Linyu Chen
Hu Deng
Zhixiang Wu
Zhonggang Xiong
Jin Guo
Quancheng Liu
Akwasi Danso Samuel
Liping Shang
Role of Focusing Distance in Picosecond Laser-Induced Cu Plasma Spectra
Advances in High Energy Physics
title Role of Focusing Distance in Picosecond Laser-Induced Cu Plasma Spectra
title_full Role of Focusing Distance in Picosecond Laser-Induced Cu Plasma Spectra
title_fullStr Role of Focusing Distance in Picosecond Laser-Induced Cu Plasma Spectra
title_full_unstemmed Role of Focusing Distance in Picosecond Laser-Induced Cu Plasma Spectra
title_short Role of Focusing Distance in Picosecond Laser-Induced Cu Plasma Spectra
title_sort role of focusing distance in picosecond laser induced cu plasma spectra
url http://dx.doi.org/10.1155/2022/4885924
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