Design of Third-Order Dispersion Compensation for the SG PW Laser System Using a Birefringent Crystal
This study aims to update the existing SG PW laser system and improve the temporal contrast and shape fidelity of a compressed pulse with a 150 fs level for multi-PW (5–10 PW). The design of third-order dispersion (TOD) compensation via a birefringent crystal was studied through numerical simulation...
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MDPI AG
2022-04-01
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author | Dawei Li Tao Wang Xiaolei Yin Jiamei Li Hui Yu Li Wang Xingqiang Lu Guang Xu |
author_facet | Dawei Li Tao Wang Xiaolei Yin Jiamei Li Hui Yu Li Wang Xingqiang Lu Guang Xu |
author_sort | Dawei Li |
collection | DOAJ |
description | This study aims to update the existing SG PW laser system and improve the temporal contrast and shape fidelity of a compressed pulse with a 150 fs level for multi-PW (5–10 PW). The design of third-order dispersion (TOD) compensation via a birefringent crystal was studied through numerical simulations and experiments. The dispersions introduced by the birefringent crystal were calculated using the Jones matrix element by changing the in-plane rotation angle <i>ϕ</i>, thickness d, incident angle <i>θ</i>, and temperature T, while also considering the transmission spectral bandwidth. The group-velocity dispersion (GVD), TOD, and fourth-order dispersion (FOD) of the existing SG PW laser system and its influence on the compressed pulse with different pulse durations were analyzed. The results suggest that a TOD of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mn>1.3</mn><mo>×</mo><msup><mrow><mn>10</mn></mrow><mn>6</mn></msup></mrow></semantics></math></inline-formula> fs<sup>3</sup> needs to compensate for the multi-PW design. The compensation scheme is designed using a quartz crystal of <i>d</i> = 6.5 mm, <i>θ</i> = 90<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mo>°</mo></semantics></math></inline-formula>, <i>ϕ</i> = 17<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mo>°</mo></semantics></math></inline-formula>, and T = 21 °C, corresponding to the thickness, inclination angle, in-plane rotation angle, and temperature, respectively. Furthermore, we show a principle-proof experiment offline and measure the GVD and TOD by the Wizzler, which is based on theoretical simulations. These results can be applied to independently and continuously control the TOD of short-pulse laser systems. |
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spelling | doaj.art-6d44b2f21d77478a9df8a1a52be2698a2023-12-01T00:44:53ZengMDPI AGApplied Sciences2076-34172022-04-01128407810.3390/app12084078Design of Third-Order Dispersion Compensation for the SG PW Laser System Using a Birefringent CrystalDawei Li0Tao Wang1Xiaolei Yin2Jiamei Li3Hui Yu4Li Wang5Xingqiang Lu6Guang Xu7Key Laboratory of High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, ChinaShanghai Institute of Laser Plasma, Chinese Academy of Engineering Physics, Shanghai 201800, ChinaSchool of Sciences, Changzhou Institute of Technology, Changzhou 213032, ChinaKey Laboratory of High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, ChinaKey Laboratory of High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, ChinaKey Laboratory of High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, ChinaKey Laboratory of High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, ChinaKey Laboratory of High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, ChinaThis study aims to update the existing SG PW laser system and improve the temporal contrast and shape fidelity of a compressed pulse with a 150 fs level for multi-PW (5–10 PW). The design of third-order dispersion (TOD) compensation via a birefringent crystal was studied through numerical simulations and experiments. The dispersions introduced by the birefringent crystal were calculated using the Jones matrix element by changing the in-plane rotation angle <i>ϕ</i>, thickness d, incident angle <i>θ</i>, and temperature T, while also considering the transmission spectral bandwidth. The group-velocity dispersion (GVD), TOD, and fourth-order dispersion (FOD) of the existing SG PW laser system and its influence on the compressed pulse with different pulse durations were analyzed. The results suggest that a TOD of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mn>1.3</mn><mo>×</mo><msup><mrow><mn>10</mn></mrow><mn>6</mn></msup></mrow></semantics></math></inline-formula> fs<sup>3</sup> needs to compensate for the multi-PW design. The compensation scheme is designed using a quartz crystal of <i>d</i> = 6.5 mm, <i>θ</i> = 90<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mo>°</mo></semantics></math></inline-formula>, <i>ϕ</i> = 17<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mo>°</mo></semantics></math></inline-formula>, and T = 21 °C, corresponding to the thickness, inclination angle, in-plane rotation angle, and temperature, respectively. Furthermore, we show a principle-proof experiment offline and measure the GVD and TOD by the Wizzler, which is based on theoretical simulations. These results can be applied to independently and continuously control the TOD of short-pulse laser systems.https://www.mdpi.com/2076-3417/12/8/4078third-order dispersion compensationbirefringent crystalSG PW laser systemtemporal contrastshape fidelitymulti-PW laser |
spellingShingle | Dawei Li Tao Wang Xiaolei Yin Jiamei Li Hui Yu Li Wang Xingqiang Lu Guang Xu Design of Third-Order Dispersion Compensation for the SG PW Laser System Using a Birefringent Crystal Applied Sciences third-order dispersion compensation birefringent crystal SG PW laser system temporal contrast shape fidelity multi-PW laser |
title | Design of Third-Order Dispersion Compensation for the SG PW Laser System Using a Birefringent Crystal |
title_full | Design of Third-Order Dispersion Compensation for the SG PW Laser System Using a Birefringent Crystal |
title_fullStr | Design of Third-Order Dispersion Compensation for the SG PW Laser System Using a Birefringent Crystal |
title_full_unstemmed | Design of Third-Order Dispersion Compensation for the SG PW Laser System Using a Birefringent Crystal |
title_short | Design of Third-Order Dispersion Compensation for the SG PW Laser System Using a Birefringent Crystal |
title_sort | design of third order dispersion compensation for the sg pw laser system using a birefringent crystal |
topic | third-order dispersion compensation birefringent crystal SG PW laser system temporal contrast shape fidelity multi-PW laser |
url | https://www.mdpi.com/2076-3417/12/8/4078 |
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