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
Autor*in: |
Su, Juan [verfasserIn] Wang, Jun [verfasserIn] Zheng, Suzhen [verfasserIn] Liu, Zhonghua [verfasserIn] Li, Jüfen [verfasserIn] |
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Format: |
E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2019 |
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Schlagwörter: |
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Übergeordnetes Werk: |
Enthalten in: Optik - München : Elsevier, 2001, 203 |
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Übergeordnetes Werk: |
volume:203 |
DOI / URN: |
10.1016/j.ijleo.2019.163145 |
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Katalog-ID: |
ELV004168747 |
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245 | 1 | 0 | |a Influence of grooves misaligned reflection grism stretcher on femtosecond pulse in chirped pulse amplification system |
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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. | ||
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700 | 1 | |a Li, Jüfen |e verfasserin |4 aut | |
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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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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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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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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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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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Influence of grooves misaligned reflection grism stretcher on femtosecond pulse in chirped pulse amplification system |
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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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