《Tab.1 Yb3+doped laser materials classified by molecular structure表1按分子结构分类的Yb3+掺杂激光材料》
![《Tab.1 Yb3+doped laser materials classified by molecular structure表1按分子结构分类的Yb3+掺杂激光材料》](http://bookimg.mtoou.info/tubiao/gif/ZGGA201901017_14800.gif)
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《基于SESAM被动调Q的激光二极管泵浦Yb∶CaYAlO_4脉冲激光器》
Existing research shows that Yb3+ion dopedlaser materials have the advantages of having a simple energy level structure,high quantum efficiency,wide emission spectrum,being unaffected by excited stateabsorption,up-conversion,concentration quenching,etc….These are each very suitable for generating high power,near-infrared short-pulse laser beams[28-29].Meanwhile,since a doped Yb3+laser medium has an absorption wavelength matching the emission wavelength of its high-intensity InGaAs laser diode,a compact laser-diode-pumped all-solidstate laser can be constructed.Doped Yb3+laser materials can be classified into glass,crystal,and ceramic,depending on the used process of preparation.They can also be classified by molecular structure,as shown in Tab.1.In recent years,as a new type of erbium-doped gain material,Yb∶CaYAlO4has been attracting the attention of academics and industrial professionals,its output characteristics in continuous lasers and mode-locked pulsed lasers has been studied with more frequency.In 2010,Dongzhen Li et al.used the Czochralski method to grow Yb∶CaYAlO4crystals then determined their lifetime of fluorescence to be 426μs and the full width at half maximum of their fluorescence spectrum to be at61 nm[30].In 2011,they further studied the continuous laser output of Yb∶CaYAlO4crystals.When the incident pump's power is set to 8 W,a continuous laser with a maximum output power of 2.48 W is achieved with a slope efficiency of 55.4%[31].Also in 2011,Tan et al.of Nanyang Technological University achieved a pulsed laser with a pulse width of156 fs,repetition rate of 91 MHz and a maximum average output power of 740 m W[32]using a SESAM mode-locked Yb∶CaYAlO4laser.In 2015,Gao et al.achieved Kerr lens mode-locking with Yb∶CaYAlO4and produced an ultrashort pulse laser of 33 fs with a repetition rate of 115 MHz[33].In 2016,Ma et al.of Nanyang Technological University used graphene as a saturable absorber to achieve mode-locking pulse output with a Yb∶CaYAlO4laser achieving a pulsed width of 30 fs,which is the shortest pulse generated by mode-locked Yb∶CaYAlO4lasers so far[34].It is worth noting that,while current research on Yb∶CaYAlO4pulsed lasers is related to mode-locked lasers with no report on passive Q-switched lasers,understanding the performance of Q-switched pulses from Yb∶CaYAlO4crystal lasers helps further understand the optical properties of Yb∶CaYAlO4crystals.Therefore,it is necessary to research and explore the performance of passive Q-switched Yb∶CaYAlO4crystal lasers.
图表编号 | XD0047198500 严禁用于非法目的 |
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绘制时间 | 2019.02.01 |
作者 | 唐睿、高子叶、吴正茂、夏光琼 |
绘制单位 | 西南大学物理科学与技术学院、西南大学物理科学与技术学院、西南大学物理科学与技术学院、西南大学物理科学与技术学院 |
更多格式 | 高清、无水印(增值服务) |