Influence of grooves misaligned reflection grism stretcher on femtosecond pulse in chirped pulse amplification system

The misalignment of the compressor or stretcher based on the grisms is unavoidable in a chirped pulse amplification laser system. In this paper, analytical expressions for the dispersion of misaligned grooves in reflection grism stretcher are presented. The residual dispersion in a chirped pulse amp...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Su, Juan [verfasserIn] Wang, Jun [verfasserIn] Zheng, Suzhen [verfasserIn] Liu, Zhonghua [verfasserIn] Li, Jüfen [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2019

Schlagwörter:	Grism Grating groove Misalign Residual dispersion

Übergeordnetes Werk:	Enthalten in: Optik - München : Elsevier, 2001, 203
Übergeordnetes Werk:	volume:203

DOI / URN:	10.1016/j.ijleo.2019.163145

Katalog-ID:	ELV004168747

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520			\|a The misalignment of the compressor or stretcher based on the grisms is unavoidable in a chirped pulse amplification laser system. In this paper, analytical expressions for the dispersion of misaligned grooves in reflection grism stretcher are presented. The residual dispersion in a chirped pulse amplification system due to the misaligned grism stretcher is analyzed. Furthermore, we evaluate the effects of the residual dispersion on the femtosecond pulse. Results show that when the grism grooves are misaligned, the rotation angle of grooves and incidence angle have great effects on the dispersion of grism pair, especially on the third-order dispersion. The rotation direction of grism grooves has no influence on the dispersions. Residual dispersions resulted from the misaligned grism stretcher have arisen in the CPA system. Therefore, the residual dispersions lead to an increase in the recompressed pulse duration. Meanwhile, the pulse waveform tilts backward and exhibits a severe wing on the trailing edge of the pulse.
650		4	\|a Grism
650		4	\|a Grating groove
650		4	\|a Misalign
650		4	\|a Residual dispersion
700	1		\|a Wang, Jun \|e verfasserin \|4 aut
700	1		\|a Zheng, Suzhen \|e verfasserin \|4 aut
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700	1		\|a Li, Jüfen \|e verfasserin \|4 aut
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author_variant	j s js j w jw s z sz z l zl j l jl
matchkey_str	article:16181336:2019----::nlecogovsiaindelcinrssrthrnetscnplenh
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publishDate	2019
allfields	10.1016/j.ijleo.2019.163145 doi (DE-627)ELV004168747 (ELSEVIER)S0030-4026(19)31035-6 DE-627 ger DE-627 rda eng 620 DE-600 33.18 bkl 33.38 bkl 50.37 bkl 53.54 bkl 53.75 bkl 42.03 bkl Su, Juan verfasserin aut Influence of grooves misaligned reflection grism stretcher on femtosecond pulse in chirped pulse amplification system 2019 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The misalignment of the compressor or stretcher based on the grisms is unavoidable in a chirped pulse amplification laser system. In this paper, analytical expressions for the dispersion of misaligned grooves in reflection grism stretcher are presented. The residual dispersion in a chirped pulse amplification system due to the misaligned grism stretcher is analyzed. Furthermore, we evaluate the effects of the residual dispersion on the femtosecond pulse. Results show that when the grism grooves are misaligned, the rotation angle of grooves and incidence angle have great effects on the dispersion of grism pair, especially on the third-order dispersion. The rotation direction of grism grooves has no influence on the dispersions. Residual dispersions resulted from the misaligned grism stretcher have arisen in the CPA system. Therefore, the residual dispersions lead to an increase in the recompressed pulse duration. Meanwhile, the pulse waveform tilts backward and exhibits a severe wing on the trailing edge of the pulse. Grism Grating groove Misalign Residual dispersion Wang, Jun verfasserin aut Zheng, Suzhen verfasserin aut Liu, Zhonghua verfasserin aut Li, Jüfen verfasserin aut Enthalten in Optik München : Elsevier, 2001 203 Online-Ressource (DE-627)325791988 (DE-600)2040037-8 (DE-576)094480680 1618-1336 nnns volume:203 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2153 GBV_ILN_2336 GBV_ILN_2522 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 33.18 Optik 33.38 Quantenoptik nichtlineare Optik 50.37 Technische Optik 53.54 Optoelektronik 53.75 Optische Nachrichtentechnik 42.03 Methoden und Techniken der Biologie AR 203
spelling	10.1016/j.ijleo.2019.163145 doi (DE-627)ELV004168747 (ELSEVIER)S0030-4026(19)31035-6 DE-627 ger DE-627 rda eng 620 DE-600 33.18 bkl 33.38 bkl 50.37 bkl 53.54 bkl 53.75 bkl 42.03 bkl Su, Juan verfasserin aut Influence of grooves misaligned reflection grism stretcher on femtosecond pulse in chirped pulse amplification system 2019 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The misalignment of the compressor or stretcher based on the grisms is unavoidable in a chirped pulse amplification laser system. In this paper, analytical expressions for the dispersion of misaligned grooves in reflection grism stretcher are presented. The residual dispersion in a chirped pulse amplification system due to the misaligned grism stretcher is analyzed. Furthermore, we evaluate the effects of the residual dispersion on the femtosecond pulse. Results show that when the grism grooves are misaligned, the rotation angle of grooves and incidence angle have great effects on the dispersion of grism pair, especially on the third-order dispersion. The rotation direction of grism grooves has no influence on the dispersions. Residual dispersions resulted from the misaligned grism stretcher have arisen in the CPA system. Therefore, the residual dispersions lead to an increase in the recompressed pulse duration. Meanwhile, the pulse waveform tilts backward and exhibits a severe wing on the trailing edge of the pulse. Grism Grating groove Misalign Residual dispersion Wang, Jun verfasserin aut Zheng, Suzhen verfasserin aut Liu, Zhonghua verfasserin aut Li, Jüfen verfasserin aut Enthalten in Optik München : Elsevier, 2001 203 Online-Ressource (DE-627)325791988 (DE-600)2040037-8 (DE-576)094480680 1618-1336 nnns volume:203 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2153 GBV_ILN_2336 GBV_ILN_2522 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 33.18 Optik 33.38 Quantenoptik nichtlineare Optik 50.37 Technische Optik 53.54 Optoelektronik 53.75 Optische Nachrichtentechnik 42.03 Methoden und Techniken der Biologie AR 203
allfields_unstemmed	10.1016/j.ijleo.2019.163145 doi (DE-627)ELV004168747 (ELSEVIER)S0030-4026(19)31035-6 DE-627 ger DE-627 rda eng 620 DE-600 33.18 bkl 33.38 bkl 50.37 bkl 53.54 bkl 53.75 bkl 42.03 bkl Su, Juan verfasserin aut Influence of grooves misaligned reflection grism stretcher on femtosecond pulse in chirped pulse amplification system 2019 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The misalignment of the compressor or stretcher based on the grisms is unavoidable in a chirped pulse amplification laser system. In this paper, analytical expressions for the dispersion of misaligned grooves in reflection grism stretcher are presented. The residual dispersion in a chirped pulse amplification system due to the misaligned grism stretcher is analyzed. Furthermore, we evaluate the effects of the residual dispersion on the femtosecond pulse. Results show that when the grism grooves are misaligned, the rotation angle of grooves and incidence angle have great effects on the dispersion of grism pair, especially on the third-order dispersion. The rotation direction of grism grooves has no influence on the dispersions. Residual dispersions resulted from the misaligned grism stretcher have arisen in the CPA system. Therefore, the residual dispersions lead to an increase in the recompressed pulse duration. Meanwhile, the pulse waveform tilts backward and exhibits a severe wing on the trailing edge of the pulse. Grism Grating groove Misalign Residual dispersion Wang, Jun verfasserin aut Zheng, Suzhen verfasserin aut Liu, Zhonghua verfasserin aut Li, Jüfen verfasserin aut Enthalten in Optik München : Elsevier, 2001 203 Online-Ressource (DE-627)325791988 (DE-600)2040037-8 (DE-576)094480680 1618-1336 nnns volume:203 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2153 GBV_ILN_2336 GBV_ILN_2522 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 33.18 Optik 33.38 Quantenoptik nichtlineare Optik 50.37 Technische Optik 53.54 Optoelektronik 53.75 Optische Nachrichtentechnik 42.03 Methoden und Techniken der Biologie AR 203
allfieldsGer	10.1016/j.ijleo.2019.163145 doi (DE-627)ELV004168747 (ELSEVIER)S0030-4026(19)31035-6 DE-627 ger DE-627 rda eng 620 DE-600 33.18 bkl 33.38 bkl 50.37 bkl 53.54 bkl 53.75 bkl 42.03 bkl Su, Juan verfasserin aut Influence of grooves misaligned reflection grism stretcher on femtosecond pulse in chirped pulse amplification system 2019 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The misalignment of the compressor or stretcher based on the grisms is unavoidable in a chirped pulse amplification laser system. In this paper, analytical expressions for the dispersion of misaligned grooves in reflection grism stretcher are presented. The residual dispersion in a chirped pulse amplification system due to the misaligned grism stretcher is analyzed. Furthermore, we evaluate the effects of the residual dispersion on the femtosecond pulse. Results show that when the grism grooves are misaligned, the rotation angle of grooves and incidence angle have great effects on the dispersion of grism pair, especially on the third-order dispersion. The rotation direction of grism grooves has no influence on the dispersions. Residual dispersions resulted from the misaligned grism stretcher have arisen in the CPA system. Therefore, the residual dispersions lead to an increase in the recompressed pulse duration. Meanwhile, the pulse waveform tilts backward and exhibits a severe wing on the trailing edge of the pulse. Grism Grating groove Misalign Residual dispersion Wang, Jun verfasserin aut Zheng, Suzhen verfasserin aut Liu, Zhonghua verfasserin aut Li, Jüfen verfasserin aut Enthalten in Optik München : Elsevier, 2001 203 Online-Ressource (DE-627)325791988 (DE-600)2040037-8 (DE-576)094480680 1618-1336 nnns volume:203 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2153 GBV_ILN_2336 GBV_ILN_2522 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 33.18 Optik 33.38 Quantenoptik nichtlineare Optik 50.37 Technische Optik 53.54 Optoelektronik 53.75 Optische Nachrichtentechnik 42.03 Methoden und Techniken der Biologie AR 203
allfieldsSound	10.1016/j.ijleo.2019.163145 doi (DE-627)ELV004168747 (ELSEVIER)S0030-4026(19)31035-6 DE-627 ger DE-627 rda eng 620 DE-600 33.18 bkl 33.38 bkl 50.37 bkl 53.54 bkl 53.75 bkl 42.03 bkl Su, Juan verfasserin aut Influence of grooves misaligned reflection grism stretcher on femtosecond pulse in chirped pulse amplification system 2019 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The misalignment of the compressor or stretcher based on the grisms is unavoidable in a chirped pulse amplification laser system. In this paper, analytical expressions for the dispersion of misaligned grooves in reflection grism stretcher are presented. The residual dispersion in a chirped pulse amplification system due to the misaligned grism stretcher is analyzed. Furthermore, we evaluate the effects of the residual dispersion on the femtosecond pulse. Results show that when the grism grooves are misaligned, the rotation angle of grooves and incidence angle have great effects on the dispersion of grism pair, especially on the third-order dispersion. The rotation direction of grism grooves has no influence on the dispersions. Residual dispersions resulted from the misaligned grism stretcher have arisen in the CPA system. Therefore, the residual dispersions lead to an increase in the recompressed pulse duration. Meanwhile, the pulse waveform tilts backward and exhibits a severe wing on the trailing edge of the pulse. Grism Grating groove Misalign Residual dispersion Wang, Jun verfasserin aut Zheng, Suzhen verfasserin aut Liu, Zhonghua verfasserin aut Li, Jüfen verfasserin aut Enthalten in Optik München : Elsevier, 2001 203 Online-Ressource (DE-627)325791988 (DE-600)2040037-8 (DE-576)094480680 1618-1336 nnns volume:203 GBV_USEFLAG_U SYSFLAG_U GBV_ELV GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2153 GBV_ILN_2336 GBV_ILN_2522 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 33.18 Optik 33.38 Quantenoptik nichtlineare Optik 50.37 Technische Optik 53.54 Optoelektronik 53.75 Optische Nachrichtentechnik 42.03 Methoden und Techniken der Biologie AR 203
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topic_facet	Grism Grating groove Misalign Residual dispersion
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authorswithroles_txt_mv	Su, Juan @@aut@@ Wang, Jun @@aut@@ Zheng, Suzhen @@aut@@ Liu, Zhonghua @@aut@@ Li, Jüfen @@aut@@
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author	Su, Juan
spellingShingle	Su, Juan ddc 620 bkl 33.18 bkl 33.38 bkl 50.37 bkl 53.54 bkl 53.75 bkl 42.03 misc Grism misc Grating groove misc Misalign misc Residual dispersion Influence of grooves misaligned reflection grism stretcher on femtosecond pulse in chirped pulse amplification system
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topic_title	620 DE-600 33.18 bkl 33.38 bkl 50.37 bkl 53.54 bkl 53.75 bkl 42.03 bkl Influence of grooves misaligned reflection grism stretcher on femtosecond pulse in chirped pulse amplification system Grism Grating groove Misalign Residual dispersion
topic	ddc 620 bkl 33.18 bkl 33.38 bkl 50.37 bkl 53.54 bkl 53.75 bkl 42.03 misc Grism misc Grating groove misc Misalign misc Residual dispersion
topic_unstemmed	ddc 620 bkl 33.18 bkl 33.38 bkl 50.37 bkl 53.54 bkl 53.75 bkl 42.03 misc Grism misc Grating groove misc Misalign misc Residual dispersion
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title	Influence of grooves misaligned reflection grism stretcher on femtosecond pulse in chirped pulse amplification system
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title_full	Influence of grooves misaligned reflection grism stretcher on femtosecond pulse in chirped pulse amplification system
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title_sort	influence of grooves misaligned reflection grism stretcher on femtosecond pulse in chirped pulse amplification system
title_auth	Influence of grooves misaligned reflection grism stretcher on femtosecond pulse in chirped pulse amplification system
abstract	The misalignment of the compressor or stretcher based on the grisms is unavoidable in a chirped pulse amplification laser system. In this paper, analytical expressions for the dispersion of misaligned grooves in reflection grism stretcher are presented. The residual dispersion in a chirped pulse amplification system due to the misaligned grism stretcher is analyzed. Furthermore, we evaluate the effects of the residual dispersion on the femtosecond pulse. Results show that when the grism grooves are misaligned, the rotation angle of grooves and incidence angle have great effects on the dispersion of grism pair, especially on the third-order dispersion. The rotation direction of grism grooves has no influence on the dispersions. Residual dispersions resulted from the misaligned grism stretcher have arisen in the CPA system. Therefore, the residual dispersions lead to an increase in the recompressed pulse duration. Meanwhile, the pulse waveform tilts backward and exhibits a severe wing on the trailing edge of the pulse.
abstractGer	The misalignment of the compressor or stretcher based on the grisms is unavoidable in a chirped pulse amplification laser system. In this paper, analytical expressions for the dispersion of misaligned grooves in reflection grism stretcher are presented. The residual dispersion in a chirped pulse amplification system due to the misaligned grism stretcher is analyzed. Furthermore, we evaluate the effects of the residual dispersion on the femtosecond pulse. Results show that when the grism grooves are misaligned, the rotation angle of grooves and incidence angle have great effects on the dispersion of grism pair, especially on the third-order dispersion. The rotation direction of grism grooves has no influence on the dispersions. Residual dispersions resulted from the misaligned grism stretcher have arisen in the CPA system. Therefore, the residual dispersions lead to an increase in the recompressed pulse duration. Meanwhile, the pulse waveform tilts backward and exhibits a severe wing on the trailing edge of the pulse.
abstract_unstemmed	The misalignment of the compressor or stretcher based on the grisms is unavoidable in a chirped pulse amplification laser system. In this paper, analytical expressions for the dispersion of misaligned grooves in reflection grism stretcher are presented. The residual dispersion in a chirped pulse amplification system due to the misaligned grism stretcher is analyzed. Furthermore, we evaluate the effects of the residual dispersion on the femtosecond pulse. Results show that when the grism grooves are misaligned, the rotation angle of grooves and incidence angle have great effects on the dispersion of grism pair, especially on the third-order dispersion. The rotation direction of grism grooves has no influence on the dispersions. Residual dispersions resulted from the misaligned grism stretcher have arisen in the CPA system. Therefore, the residual dispersions lead to an increase in the recompressed pulse duration. Meanwhile, the pulse waveform tilts backward and exhibits a severe wing on the trailing edge of the pulse.
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title_short	Influence of grooves misaligned reflection grism stretcher on femtosecond pulse in chirped pulse amplification system
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author2	Wang, Jun Zheng, Suzhen Liu, Zhonghua Li, Jüfen
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doi_str	10.1016/j.ijleo.2019.163145
up_date	2024-07-06T22:04:55.933Z
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In this paper, analytical expressions for the dispersion of misaligned grooves in reflection grism stretcher are presented. The residual dispersion in a chirped pulse amplification system due to the misaligned grism stretcher is analyzed. Furthermore, we evaluate the effects of the residual dispersion on the femtosecond pulse. Results show that when the grism grooves are misaligned, the rotation angle of grooves and incidence angle have great effects on the dispersion of grism pair, especially on the third-order dispersion. The rotation direction of grism grooves has no influence on the dispersions. Residual dispersions resulted from the misaligned grism stretcher have arisen in the CPA system. Therefore, the residual dispersions lead to an increase in the recompressed pulse duration. 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Influence of grooves misaligned reflection grism stretcher on femtosecond pulse in chirped pulse amplification system

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