Continuous-wave Nd:KGd(WO 4 ) 2 single-longitudinal-mode laser
A continuous-wave Nd:KGd(WO 4 ) 2 single-longitudinal-mode laser is demonstrated with Fabry–Perot etalons in a simple linear cavity. The thermal lens effect is dramatically lowered by propagating the laser beam along the ‘athermal’ direction inside the laser crystal, which is very beneficial to remo...
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Published in | Chinese physics B Vol. 30; no. 8; pp. 84201 - 406 |
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Main Authors | , , , , , , , , |
Format | Journal Article |
Language | English |
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School of Opto-electronic Information Science and Technology,Yantai University,Yantai 264005,China%National Key Laboratory of Tunable Laser Technology,Harbin Institute of Technology,Harbin 150001,China%Física i Cristal·lografia de Materials i Nanomaterials (FiCMA-FiCNA),Universitat Rovira i Virgili (URV),Campus Sescelades,c/Marcel·lí Domingo,s/n.,Tarragona 43007,Spain
01.07.2021
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Abstract | A continuous-wave Nd:KGd(WO
4
)
2
single-longitudinal-mode laser is demonstrated with Fabry–Perot etalons in a simple linear cavity. The thermal lens effect is dramatically lowered by propagating the laser beam along the ‘athermal’ direction inside the laser crystal, which is very beneficial to removing the heat generated in the mode selection process. The maximum single-longitudinal-mode output power obtained is 64.8 mW at incident pump power of 4.7 W, corresponding to an optical conversion efficiency of 1.3% and a slope efficiency of 1.7%. |
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AbstractList | A continuous-wave Nd:KGd(WO
4
)
2
single-longitudinal-mode laser is demonstrated with Fabry–Perot etalons in a simple linear cavity. The thermal lens effect is dramatically lowered by propagating the laser beam along the ‘athermal’ direction inside the laser crystal, which is very beneficial to removing the heat generated in the mode selection process. The maximum single-longitudinal-mode output power obtained is 64.8 mW at incident pump power of 4.7 W, corresponding to an optical conversion efficiency of 1.3% and a slope efficiency of 1.7%. A continuous-wave Nd∶KGd(WO4)2 single-longitudinal-mode laser is demonstrated with Fabry-Perot etalons in a simple linear cavity.The thermal lens effect is dramatically lowered by propagating the laser beam along the 'athermal'direction inside the laser crystal,which is very beneficial to removing the heat generated in the mode selection process.The maximum single-longitudinal-mode output power obtained is 64.8 mW at incident pump power of 4.7 W,corresponding to an optical conversion efficiency of 1.3% and a slope efficiency of 1.7%. |
Author | Lan, Rui-Jun Cao, De-Zhong Dai, Tong-Yu Mateos, Xavier Mu, Peng-Hua Min, Huan-Huan Shen, Ying-Jie Liu, Guang-Hua Ren, Cheng |
AuthorAffiliation | School of Opto-electronic Information Science and Technology,Yantai University,Yantai 264005,China%National Key Laboratory of Tunable Laser Technology,Harbin Institute of Technology,Harbin 150001,China%Física i Cristal·lografia de Materials i Nanomaterials (FiCMA-FiCNA),Universitat Rovira i Virgili (URV),Campus Sescelades,c/Marcel·lí Domingo,s/n.,Tarragona 43007,Spain |
AuthorAffiliation_xml | – name: School of Opto-electronic Information Science and Technology,Yantai University,Yantai 264005,China%National Key Laboratory of Tunable Laser Technology,Harbin Institute of Technology,Harbin 150001,China%Física i Cristal·lografia de Materials i Nanomaterials (FiCMA-FiCNA),Universitat Rovira i Virgili (URV),Campus Sescelades,c/Marcel·lí Domingo,s/n.,Tarragona 43007,Spain |
Author_xml | – sequence: 1 givenname: Rui-Jun surname: Lan fullname: Lan, Rui-Jun – sequence: 2 givenname: Guang-Hua surname: Liu fullname: Liu, Guang-Hua – sequence: 3 givenname: Huan-Huan surname: Min fullname: Min, Huan-Huan – sequence: 4 givenname: Tong-Yu surname: Dai fullname: Dai, Tong-Yu – sequence: 5 givenname: Ying-Jie surname: Shen fullname: Shen, Ying-Jie – sequence: 6 givenname: Peng-Hua surname: Mu fullname: Mu, Peng-Hua – sequence: 7 givenname: Cheng surname: Ren fullname: Ren, Cheng – sequence: 8 givenname: De-Zhong surname: Cao fullname: Cao, De-Zhong – sequence: 9 givenname: Xavier surname: Mateos fullname: Mateos, Xavier |
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Cites_doi | 10.1007/s00340-007-2666-y 10.1364/AO.51.001616 10.1038/nature13634 10.1117/1.601185 10.1007/s00340-007-2732-5 10.1364/OE.19.006797 10.1364/AO.44.003093 10.1088/1674-1056/ab9441 10.1364/OL.14.000024 10.1364/OL.30.000421 10.1364/AO.54.005143 10.1007/s00340-011-4777-8 10.3788/COL 10.7498/aps.68.20182018 10.1016/j.optlastec.2015.05.005 10.1038/nphys2083 10.1364/OE.17.012057 10.1364/OE.25.027671 10.1364/OE.27.026080 10.1103/PhysRevLett.117.240503 10.1007/s00340-002-1004-7 10.1364/OE.18.012161 10.1364/OL.27.001478 10.1016/S0925-3467(03)00151-4 10.1364/OE.18.002753 10.1007/s003400050467 |
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Keywords | continuous wave single-longitudinal mode Fabry-Perot etalon |
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Snippet | A continuous-wave Nd:KGd(WO
4
)
2
single-longitudinal-mode laser is demonstrated with Fabry–Perot etalons in a simple linear cavity. The thermal lens effect is... A continuous-wave Nd∶KGd(WO4)2 single-longitudinal-mode laser is demonstrated with Fabry-Perot etalons in a simple linear cavity.The thermal lens effect is... |
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Title | Continuous-wave Nd:KGd(WO 4 ) 2 single-longitudinal-mode laser |
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