J. Šulc, M. Jelínek, M. Němec, H. Jelínková, K. Nejezchleb, S. Uxa
{"title":"Influence of crystal orientation on Ho:YAP microchip laser generation","authors":"J. Šulc, M. Jelínek, M. Němec, H. Jelínková, K. Nejezchleb, S. Uxa","doi":"10.1117/12.2665634","DOIUrl":null,"url":null,"abstract":"The goal of this work was an investigation of Ho:YAP (Ho:YAlO3) crystal as an active medium of resonantly longitudinally pumped multi-watt microchip laser operating at 2.1 ¹m spectral region. Three Ho:YAP crystals,a\"-cut, b\"-cut, and c\"-cut Pbnm, with the same dimensions (7mm long, 3mm in diameter) and Ho-doping concentration (1.06 at.% Ho/Y) were compared. Resonator mirrors were deposited directly on the crystals faces. The output coupler transmission for desired laser emission wavelength range 2.1 µm was 11% and T = 3% @ 1.94 µm. The pumping mirror was highly reflecting at 2.1 µm and T = 89% @ 1.94 µm. Samples were fixed in air-cooled Cu-heatsink and longitudinally pumped by a CW Tm-fibre laser with the maximum output power amplitude of 12W @ 1939.2nm behind a focusing lens (f = 200 mm). The laser output power, emission wavelength, and output beam profile were measured in respect to incident pumping power. All three lasers had similar input-output power characteristics with the laser threshold close to 1.5W and slope efficiencies reaching quantum limit in respect to the incident pumping power. The best result (slope efficiency 79 %, laser threshold 1.54W, max output power 8.2W in an almost diffraction-limited, linearly polarized beam) was reached for microchip laser using b\"-cut Ho:YAP crystal. Laser emission wavelength was 2119nm for a\"-cut and b\"-cut Ho:YAP and 2132nm for c\"-cut Ho:YAP-based microchip laser. The designed lasers can serve as compact wavelength converters for laser radiation and could be used to expand capabilities of current Tm-fibre lasers used in medicine and industry preserving the overall system efficiency.","PeriodicalId":376481,"journal":{"name":"Optics + Optoelectronics","volume":"43 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2023-06-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Optics + Optoelectronics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1117/12.2665634","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
The goal of this work was an investigation of Ho:YAP (Ho:YAlO3) crystal as an active medium of resonantly longitudinally pumped multi-watt microchip laser operating at 2.1 ¹m spectral region. Three Ho:YAP crystals,a"-cut, b"-cut, and c"-cut Pbnm, with the same dimensions (7mm long, 3mm in diameter) and Ho-doping concentration (1.06 at.% Ho/Y) were compared. Resonator mirrors were deposited directly on the crystals faces. The output coupler transmission for desired laser emission wavelength range 2.1 µm was 11% and T = 3% @ 1.94 µm. The pumping mirror was highly reflecting at 2.1 µm and T = 89% @ 1.94 µm. Samples were fixed in air-cooled Cu-heatsink and longitudinally pumped by a CW Tm-fibre laser with the maximum output power amplitude of 12W @ 1939.2nm behind a focusing lens (f = 200 mm). The laser output power, emission wavelength, and output beam profile were measured in respect to incident pumping power. All three lasers had similar input-output power characteristics with the laser threshold close to 1.5W and slope efficiencies reaching quantum limit in respect to the incident pumping power. The best result (slope efficiency 79 %, laser threshold 1.54W, max output power 8.2W in an almost diffraction-limited, linearly polarized beam) was reached for microchip laser using b"-cut Ho:YAP crystal. Laser emission wavelength was 2119nm for a"-cut and b"-cut Ho:YAP and 2132nm for c"-cut Ho:YAP-based microchip laser. The designed lasers can serve as compact wavelength converters for laser radiation and could be used to expand capabilities of current Tm-fibre lasers used in medicine and industry preserving the overall system efficiency.