Old Wavelength, New Performance: Hectowatt 200-μJ-Level Femtosecond Fiber CPA System at 1064 Nm
The Yb:fiber based high-power and high-energy ultrafast lasers usually feature central wavelength of 1030 nm instead of the more common one of 1064 nm, thus limiting some potential wavelength-dependent applications. In this work, a hectowatt 1064-nm femtosecond chirped pulse amplification (CPA) syst...
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description | The Yb:fiber based high-power and high-energy ultrafast lasers usually feature central wavelength of 1030 nm instead of the more common one of 1064 nm, thus limiting some potential wavelength-dependent applications. In this work, a hectowatt 1064-nm femtosecond chirped pulse amplification (CPA) system based on double-stage rod-type photonic crystal fiber (PCF) amplifier was demonstrated, with a pulse energy of 212-μJ and a repetition rate of 0.5 MHz. Compared with our previous work [Opt. Express 30(6), 3611, 2022], two key measures were employed. Firstly, a Yb:YAG crystal was intentionally introduced as a spectral filter for avoiding 1030-nm amplified spontaneous emission (ASE) oscillation, which hence improved the signal-to-noise ratio (SNR) by 15 dB. Secondly, an additional stage of rod-type PCF amplifier was adopted for further power scaling, achieving an average power of 127 W. Finally, the pulse was compressed to ∼460 fs, with an average power of 106 W and a compression efficiency of ∼83%. The beam quality factors (M 2 ) were measured to be M2 X = 1.12 and M2 Y = 1.09. To the best of our knowledge, this is the highest pulse energy among 1064-nm hectowatt-level femtosecond lasers, thus providing a high-quality source for wavelength-dependent applications. For example, it can be used as a driver for high-repetition-rate vacuum ultraviolet (VUV) sources about 10.5 eV, with an expected conversion efficiency of up to 1%. |
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In this work, a hectowatt 1064-nm femtosecond chirped pulse amplification (CPA) system based on double-stage rod-type photonic crystal fiber (PCF) amplifier was demonstrated, with a pulse energy of 212-μJ and a repetition rate of 0.5 MHz. Compared with our previous work [Opt. Express 30(6), 3611, 2022], two key measures were employed. Firstly, a Yb:YAG crystal was intentionally introduced as a spectral filter for avoiding 1030-nm amplified spontaneous emission (ASE) oscillation, which hence improved the signal-to-noise ratio (SNR) by 15 dB. Secondly, an additional stage of rod-type PCF amplifier was adopted for further power scaling, achieving an average power of 127 W. Finally, the pulse was compressed to ∼460 fs, with an average power of 106 W and a compression efficiency of ∼83%. The beam quality factors (M 2 ) were measured to be M2 X = 1.12 and M2 Y = 1.09. To the best of our knowledge, this is the highest pulse energy among 1064-nm hectowatt-level femtosecond lasers, thus providing a high-quality source for wavelength-dependent applications. For example, it can be used as a driver for high-repetition-rate vacuum ultraviolet (VUV) sources about 10.5 eV, with an expected conversion efficiency of up to 1%.</description><identifier>ISSN: 0733-8724</identifier><identifier>EISSN: 1558-2213</identifier><identifier>DOI: 10.1109/JLT.2023.3326072</identifier><identifier>CODEN: JLTEDG</identifier><language>eng</language><publisher>New York: IEEE</publisher><subject>Amplifiers ; Chirped pulse amplification ; Crystal fibers ; Crystals ; Femtosecond pulsed lasers ; fiber amplifiers ; Fiber lasers ; Laser theory ; Mirrors ; Optical fiber amplifiers ; Optical fiber polarization ; Oscillators ; photonic crystal fiber ; Photonic crystals ; Repetition ; Signal to noise ratio ; Spontaneous emission ; Ultrafast lasers</subject><ispartof>Journal of lightwave technology, 2024-03, Vol.42 (5), p.1659-1666</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) 2024</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c245t-78712e466cc81a1c3beb40b82a258c6b1c2ccc67781f599749c254354684e75c3</cites><orcidid>0000-0003-2695-6687 ; 0000-0002-6707-0914 ; 0000-0002-7675-5501 ; 0000-0003-4439-3689 ; 0000-0003-3502-9666</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/10288051$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,796,27924,27925,54758</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/10288051$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc></links><search><creatorcontrib>Wang, Shang</creatorcontrib><creatorcontrib>Zhao, Qikai</creatorcontrib><creatorcontrib>Gao, Guanguang</creatorcontrib><creatorcontrib>Cong, Zhenhua</creatorcontrib><creatorcontrib>Liu, Zhaojun</creatorcontrib><creatorcontrib>Zhao, Zhigang</creatorcontrib><title>Old Wavelength, New Performance: Hectowatt 200-μJ-Level Femtosecond Fiber CPA System at 1064 Nm</title><title>Journal of lightwave technology</title><addtitle>JLT</addtitle><description>The Yb:fiber based high-power and high-energy ultrafast lasers usually feature central wavelength of 1030 nm instead of the more common one of 1064 nm, thus limiting some potential wavelength-dependent applications. In this work, a hectowatt 1064-nm femtosecond chirped pulse amplification (CPA) system based on double-stage rod-type photonic crystal fiber (PCF) amplifier was demonstrated, with a pulse energy of 212-μJ and a repetition rate of 0.5 MHz. Compared with our previous work [Opt. Express 30(6), 3611, 2022], two key measures were employed. Firstly, a Yb:YAG crystal was intentionally introduced as a spectral filter for avoiding 1030-nm amplified spontaneous emission (ASE) oscillation, which hence improved the signal-to-noise ratio (SNR) by 15 dB. Secondly, an additional stage of rod-type PCF amplifier was adopted for further power scaling, achieving an average power of 127 W. Finally, the pulse was compressed to ∼460 fs, with an average power of 106 W and a compression efficiency of ∼83%. The beam quality factors (M 2 ) were measured to be M2 X = 1.12 and M2 Y = 1.09. To the best of our knowledge, this is the highest pulse energy among 1064-nm hectowatt-level femtosecond lasers, thus providing a high-quality source for wavelength-dependent applications. For example, it can be used as a driver for high-repetition-rate vacuum ultraviolet (VUV) sources about 10.5 eV, with an expected conversion efficiency of up to 1%.</description><subject>Amplifiers</subject><subject>Chirped pulse amplification</subject><subject>Crystal fibers</subject><subject>Crystals</subject><subject>Femtosecond pulsed lasers</subject><subject>fiber amplifiers</subject><subject>Fiber lasers</subject><subject>Laser theory</subject><subject>Mirrors</subject><subject>Optical fiber amplifiers</subject><subject>Optical fiber polarization</subject><subject>Oscillators</subject><subject>photonic crystal fiber</subject><subject>Photonic crystals</subject><subject>Repetition</subject><subject>Signal to noise ratio</subject><subject>Spontaneous emission</subject><subject>Ultrafast lasers</subject><issn>0733-8724</issn><issn>1558-2213</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNpNkMFOAjEURRujiYjuXbho4tbB9rWddtwRIiKZAIkYl-NMeaMQhsG2SPg3v8FvcggsXN3Nufcmh5Brzjqcs-R-mE47wEB0hICYaTghLa6UiQC4OCUtpoWIjAZ5Ti68XzDGpTS6Rd7Hyxl9y79xiauP8HlHR7ilE3Rl7ap8ZfGBDtCGepuHQIGx6PdnGKXY4LSPVag92no1o_15gY72Jl36svMBK5oHylks6ai6JGdlvvR4dcw2ee0_TnuDKB0_Pfe6aWRBqhBpozmgjGNrDc-5FQUWkhUGclDGxgW3YK2NtTa8VEmiZWJBSaFkbCRqZUWb3B52167-2qAP2aLeuFVzmUEiQMXNjmoodqCsq713WGZrN69yt8s4y_Yes8ZjtveYHT02lZtDZY6I_3Awhiku_gDX8Gu0</recordid><startdate>20240301</startdate><enddate>20240301</enddate><creator>Wang, Shang</creator><creator>Zhao, Qikai</creator><creator>Gao, Guanguang</creator><creator>Cong, Zhenhua</creator><creator>Liu, Zhaojun</creator><creator>Zhao, Zhigang</creator><general>IEEE</general><general>The Institute of Electrical and Electronics Engineers, Inc. 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To the best of our knowledge, this is the highest pulse energy among 1064-nm hectowatt-level femtosecond lasers, thus providing a high-quality source for wavelength-dependent applications. For example, it can be used as a driver for high-repetition-rate vacuum ultraviolet (VUV) sources about 10.5 eV, with an expected conversion efficiency of up to 1%.</abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/JLT.2023.3326072</doi><tpages>8</tpages><orcidid>https://orcid.org/0000-0003-2695-6687</orcidid><orcidid>https://orcid.org/0000-0002-6707-0914</orcidid><orcidid>https://orcid.org/0000-0002-7675-5501</orcidid><orcidid>https://orcid.org/0000-0003-4439-3689</orcidid><orcidid>https://orcid.org/0000-0003-3502-9666</orcidid></addata></record> |
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subjects | Amplifiers Chirped pulse amplification Crystal fibers Crystals Femtosecond pulsed lasers fiber amplifiers Fiber lasers Laser theory Mirrors Optical fiber amplifiers Optical fiber polarization Oscillators photonic crystal fiber Photonic crystals Repetition Signal to noise ratio Spontaneous emission Ultrafast lasers |
title | Old Wavelength, New Performance: Hectowatt 200-μJ-Level Femtosecond Fiber CPA System at 1064 Nm |
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