CPM,Nd:YAG激光器脉宽计算公式的探讨

首次将Kumhlke脉宽计算公式应用于CPM,Nd:YAG激光器并对公式进行讨论,代入实验数据由计算机处理作出归一脉宽同小信号增益间的关系曲线,并同CPM染料激光器进行比较,最后提出脉宽公式应用于CPM,Nd:YAG激光器中的修正。     

激光二极管侧向泵浦的Nd:YAG激光器的热效应

分析了激光二极管侧向泵浦的Nd:YAG激光器的热效应、热分布及热焦距,采用传播圆的方法对等效三镜腔进行了分析,用稳腔法对热焦距进行了测量,分析了这种方法的优缺点.     

LD端面泵浦Nd:YAG激光器的热效应研究

对激光二极管端面泵浦Nd:YAG激光器的热效应进行了分析.由热传导方程得出YAG晶体内的温度分布,模拟出激光晶体的折射率分布,并得到了激光束腰和YAG的热焦距随泵浦功率的变化曲线.     

激光二极管泵浦1319nm单频可调谐激光器技术研究

采用激光二极管泵浦单块非平面环形腔Nd：YAG激光器，获得了1319nm的单频可调谐激光输出。输出功率为99mW。斜效率为29％。用扫描F—P法和狭缝扫描法分别测量了激光器的纵模、横模特性。激光器为单纵模、基横模运转．用温度调谐方法研究了激光器的频率调谐特性，结果是调谐范围为14GHz。连续温度调谐系数为2．1GHz／C。     

高功率LD侧面泵浦Nd:YAG激光器四镜折叠腔分析与设计

运用ABCD传输矩阵理论,把增益介质作为类透镜处理,对LD侧面泵浦地Nd:YAG激光器四镜折叠腔进行了分析,特别讨论了增益介质内部基模光斑半径和基模体积随泵浦功率变化的关系.在此基础上得到了一组腔的优化参数,能使激光器实现大基模体积热稳运转,并很好地补偿了像散.     

高功率热稳定基模运转激光谐振腔的设计

分析了设计基模运转的高功率连续固体激光器谐振腔的基本理论和原则,据此制定了设计内含热透镜的基模运转的热稳腔的基本步骤,并以Nd:YAG固体激光器为例,求出其最佳腔参数.     

热特性不匹配对固体激光器输出光束的影响

采用矩阵光学的方法对两级串接Nd:YAG激光器谐振腔进行了研究,分析了热焦距的差异对双棒串接固体激光器的输出光束基模模体积及光束质量的影响.结果表明:两支棒内模体积相等时,模式匹配较好,总的模体积较大.在匹配状态下,有效基模模体积及输出镜上光斑半径得到了较好的改善,输出光束的质量得到了较大的提高.     

Nd:YAG激光器的热透镜效应及其对激光输出的影响

对Nd：YAG激光器的热透镜效应进行了分析，给出了实验测量动态热效应的方法．利用矩阵光学的方法，分析了热透镜效应对激光输出功率和光束质量的影响，并计算了两种谐振腔参数下的束腰宽度ωo、远场发散角θo和模体积V随热焦距f的变化情况．     

端面研磨Nd:YAG晶体棒热透镜焦距测量

主要分析和测量端面研磨凹面的Nd:YAG激光晶体棒的热透镜焦距。实验通过He-Ne光测试法,分别测量了不同功率下的端面研磨和未研磨晶体棒的热透镜焦距,并通过作图比较二者的热透镜焦距随泵浦功率变化情况,得出随着泵浦功率的增大,热透镜焦距逐渐减小的结论。文中对未研磨晶体棒热透镜焦距进行了理论和实验值的比较,曲线情况基本相符,故根据理论计算出补偿热透镜效应所需要的晶体棒的研磨半径。由于通过理论计算得出的研磨半径在实验过程中出现了出光阈值高,输出功率降低等一些现象,不利于生产的需要,故在实际经验的指导下,增大了晶体棒的研磨半径。结论指出端面研磨晶体棒的方法在一定条件下能对激光晶体棒的热透镜效应进行补偿,对大功率固体激光器的研发有一定积极作用。     

低能耗YAG激光器的研究与实现

在研究小功率Nd:YAG激光电源的基础上,设计出RLC新型节能电路,经实验及各参数测试证明,应用了RLC节能电路的新型Nd:YAG激光电源待机电能耗散功率明显下降,且激光泵浦氪灯的使用寿命也相应延长。这一研究结果表明,新型RLC节能电路,在小功率Nd:YAG激光电源领域具有广泛的应用前景。     

泵浦功率变化对连续YAG激光器的影响

本文指出当连续YAG器件的泵浦功率变化时,不仅是器件增益发生变化,而且器件的损耗也同样发生变化。因而引起振荡模式的变化,腔的失稳,激光输出功率变化的复杂化。文中以大量的理论计算和实验证明:在多模运转时以平行平面腔为好。在单模运转时以平—凸或凹—凸腔为好。     

波导CO_2激光器的非匹配光腔

本文报道了波导CO_2激光器的一种选择横模的方法,该器件采用了大孔径波导和近场非匹配凹面镜,可得较高输出功率的基模激光.     

多量子阱InGaAsP实现Nd:YAG激光器被动锁模

采用InGaAsP多量子阱作为可饱和吸收体,以及Nd∶YAG激光器的耦合输出镜,实现1.06μm激光的被动锁模运转.当激光器腔长为115 cm时,在平凹腔结构中获得平均脉宽23 ps、能量7 mJ的单脉冲序列;在平凸腔结构获得平均脉宽21 ps、能量10.5 mJ的单脉冲序列.比较平凹腔和平凸腔结构的Nd∶YAG激光器的锁模效果,并根据样品结构和可饱和吸收体被动锁模理论,分析半导体多量子阱材料InGaAsP实现被动锁模的机理.     

提高CWAO锁模倍频Nd:YAG激光器输出绿光功率的一种有效方法

介绍一种能有效提高CWAO(连续声光)锁模腔内倍频Nd■YAG激光器输出绿光功率的方法,使倍频转换效率比一般不采取任何措施的情况提高了8％,从而获得了1.5W的基模0.5μm■光输出,大大超出了一般飞秒染料激光器的泵浦阈值.     

Orthogonal linear polarized lasers (II)--Study on the physical phenomena

The physical phenomena and corresponding theoretical analysis of orthogonal polarized laser are reviewed. Four lasers (or systems) with orthogonal polarized beams are involved. For the birefringence dual frequency laser, its physical phenomena discussed include the alternation between strong mode competition and medium mode competition in cavity tuning; the range of frequency difference of strong mode competition (about 0?40 MHz); four polarization statuses (o-light oscillating but e-light extinguishing, both o-light and e-light oscillating, e-light oscillating but o-light extinguishing, both o-light and e-light extinguishing) in cavity tuning; the tuning curves of frequency difference; the influence of optical activity of quartz crystal on polarization direction; and the aberrance of frequency splitting. For the Birefringence-Zeeman dual frequency laser, we focus on its intensity tuning and frequency difference tuning. For the feedback system of orthogonally polarized laser, we discuss the mutual suppression between two orthogonal frequencies, intensity exchange between two orthogonal frequencies and double of intensity fringe frequency. For orthogonally polarized LD-pumped Nd: YAG microchip laser, its property of the dependence of intensity sensitivity on frequency difference is described.     

LD端面泵浦Nd∶YAG/LBO蓝光激光器热效应分析

采用平凹腔,实现LD端面泵浦Nd∶YAG/LBO全固态蓝光激光器.在泵光功率为7.33W时,得到最大蓝光输出87.6mW,倍频光转换效率为1.2%,斜效率为2.6%.通过求解Possion热传导方程,得出了Nd∶YAG内部温度场分布.     

Orthogonal linear polarized lasers (Ⅱ)--Study on the physical phenomena

The physical phenomena and corresponding theoretical analysis of orthogonal polarized laser are reviewed. Four lasers (or systems) with orthogonal polarized beams are involved. For the birefringence dual frequency laser, its physical phenomena discussed include the alternation between strong mode competition and medium mode competition in cavity tuning; the range of frequency difference of strong mode competition (about 0-40 MHz); four polarization statuses (o-light oscillating but e-light extinguishing, both o-light and elight oscillating, e-light oscillating but o-light extinguishing, both o-light and e-light extinguishing) in cavity tuning; the tuning curves of frequency difference; the influence of optical activity of quartz crystal on polarization direction; and the aberrance of frequency splitting.For the Birefringence-Zeeman dual frequency laser, we focus on its intensity tuning and frequency difference tuning. For the feedback system of orthogonally polarized laser, we discuss the mutual suppression between two orthogonal frequencies, intensity exchange between two orthogonal frequencies and double of intensity fringe frequency. For orthogonally polarized LD-pumped Nd: YAG microchip laser, its property of the dependence of intensity sensitivity on frequency difference is described.     

基于Nd:YAG/V:YAG键合晶体的1338 nm微片激光器研究

基于Nd:YAG/V:YAG键合晶体,在连续和准连续LD端面泵浦条件下,研究了输出波长1 338 nm的被动调Q微片激光器的输出特性。在连续泵浦条件下,最大的输出功率为0.73 W,此时得到稳定的调Q脉冲输出,脉冲宽度为139 ns。在准连续泵浦下,获得了被动锁模调Q激光输出,输出的最大功率为1.01 W,对应的脉冲宽度为80 ns,其中的锁模系列单脉冲宽度约为70 ps。实验结果表明,Nd:YAG/V:YAG键合晶体有利于获得高功率紧凑的1 338 nm脉冲激光输出,同时准连续泵浦能有效地降低激光晶体的热效应从而获得更高功率的激光输出。