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 共查询到18条相似文献,搜索用时 109 毫秒
1.
Cr^4+:YAG被动调Q五激光发态吸收饱和   总被引:1,自引:1,他引:0  
万小珂  林礼煌 《光学学报》1997,17(11):567-1570
运用速率方程计算了R^4+:YAG晶体的基态吸收,激发态吸收与入射脉冲的能量密度和强度的关系。在测量晶体透过率的实验中,发现Cr^4+;YAG晶体的激发态吸收趋于饱和。理论计算与实验数据拟合给出了包括基态吸收截面,激发态吸收截面和寿命等参数。  相似文献   

2.
Cr^4+:YAG的可饱和吸收特性与被动Q开关性能研究   总被引:22,自引:6,他引:16  
欧阳斌  丁彦华 《光学学报》1996,16(12):665-1670
运用速率方程计算了Cr^4+:YAG晶体的可饱和吸收特性参数,包括初始吸收系数,饱和吸收系数,饱和光强和损耗调制度,用Cr^4+:YAG对脉冲和连续Nd:YAG激光器进行了被动调Q,在脉冲Nd:YAG激光器上得到了8ns的调Q激光脉冲,在连续Nd:YAG激光器的调Q中得到了间隔和幅度抖动小于5%的输出脉冲充列。  相似文献   

3.
测量了Cr4+YAG材料的可饱和吸收特性,用多种数据分析方法处理了实验结果,Cr4+YAG的基态吸收截面σgs=11×10-19cm2,激发态吸收截面σes=1.2×10-19cm2。  相似文献   

4.
Cr^4+:YAG调Q特性的理论和实验研究   总被引:22,自引:1,他引:21  
张行愚  孙连科 《光学学报》1998,18(9):180-1185
从理论和实验两个方面研究Cr^4+:YAG的调Q特性,测量了Cr^4+:YAG调QNd^3+:YAG激光器在不同条件下脉冲能量和脉冲宽度,并与理论结果进行比较,结果显示脉冲能量的理论结果与实验结果能较发地符合,脉冲工的理论结果与实验结果变化趋势大致相一致,文中还对Cr^4+:YAG调QNd^3+:YAG激光器的其它实验现象给出定性解释。  相似文献   

5.
氟磷酸锶晶体Cr4+:YAG被动调Q激光特性研究   总被引:1,自引:0,他引:1  
采用氙灯泵浦,实现了掺钕氟磷酸锶晶体以Cr^4+:YAG作为被动调Q元件的1.059μm激光运转,测量了Cr^4+:YAG 同小爱过率及不同泵浦能量上激光单脉冲的输出能量、脉冲宽度、重复率,给出了Nd:S-FAP晶体Cr^4+:YAG调Q工作原理的方程组,数值求解该方程组得的理论结果与实验值相符。  相似文献   

6.
王加贤  王清月 《光学学报》1998,18(8):83-987
在理论上提出了Cr^4+:YAG作为可饱和吸收体在Nd:YAG激光器中实现被动锁模的可能性,运用速率方程组导出在强激光脉冲作用下Cr^4+:YAG激发态吸收的恢复时间和饱和光强。实验上在带有抗共振环结构的接近于介稳腔的脉冲式Nd:YAG激光器中用Cr^4+:YAG作为可饱和吸收体实现被动锁模运转,得到能量13.5mJ、平均脉宽180ps的锁模脉冲序列。  相似文献   

7.
YAG晶体中Cr4+和Yb3+的光谱和荧光特性研究   总被引:1,自引:0,他引:1  
董俊  邓佩珍  徐军 《光学学报》1999,19(11):576-1580
报道了(Cr^4+,Yb^3+):YAG晶体的吸收光谱和荧光光谱特性。在室温下,(Cr^4+,Yb^3+):YAG晶体在937nm和968nm处存在两个吸收带,能与InGaAs激光二级管有效耦合:而且在1030nm处有一Cr^4+吸收峰,可以实现对Yb^3+的自调Q激光输出。(Cr^+,Yb^3+):YAG 荧光光谱与Yb^3+:YAG晶体一样,发光中心也是位于1029nm,但其强度比Yb^3+:  相似文献   

8.
吴涛  邓佩珍 《光学学报》1997,17(7):66-869
测量了Cr^4+,YAG、Cr^4+,Mg2SiO4晶体在室温和液氮温度下的荧光光谱,吸收光谱和激发态寿命,讨论了温度变化时,两种晶体中Cr^4+近红外辐射积分强度变化与激光发态寿命变化的关系,得出结论:在77K ̄300K范围内,Cr^4+的^3T2能级荧光辐射截面本身受温度影响不大,Cr^4+辐射荧光的变化,主要是由无辐射弛豫速率随温度变化而引起的。  相似文献   

9.
Passive Q-switching of Pulsed and CW Nd: YAG Lasers with Cr~(4 ): YAG   总被引:1,自引:1,他引:0  
Passive Q-switching of Pulsed and CW Nd:YAG Lasers with Cr ̄(4+):YAGPassiveQ-switchingofPulsedandCWNd:YAGLaserswithCr ̄(4+):YAG...  相似文献   

10.
通过对Cr∶YAG、Tm∶YAG和Cr,Tm∶YAG晶体吸收光谱和发射光谱的比较,研究了Cr,Tm∶YAG晶体中的能量转移过程.指出Cr3+→Tm3+能量转移过程中,无辐射能量转移占绝对优势.  相似文献   

11.
在考虑Cr^4+:YAG晶体激发态吸收的情况下,给出了Cr^4+:YAG被动调Q的Nd:YAG激光器的速率方程组,从该速率方程组出发推导出了Nd:YAG被动调Q激光器的输出能量、脉冲宽度和效率的解析解,并分析了各参量之间的相互耦合关系。结果表明,在考虑了Cr^4+:YAG晶体激发态吸收的情况下,理论上能够正确地反应出Cr^4+:YAG晶体的吸收特性,对设计和优化Cr^4+:YAG被动调Q激光器有一定的指导意义。  相似文献   

12.
SaturableExcitedStateAbsorptionofCr4+YAGforQ┐switchingNdYAGLaserWANXiaokeLINLihuangOUYANGBinDINGYanhuaXUJunDENGPeizhen(Shang...  相似文献   

13.
Lai CC  Ke CP  Liu SK  Jheng DY  Wang DJ  Chen MY  Li YS  Yeh PS  Huang SL 《Optics letters》2011,36(6):784-786
A significant advancement of cw lasing in Cr4+:Y3Al5O12 (Cr4+:YAG) double-clad crystal fiber grown by the codrawing laser-heated pedestal growth technique was demonstrated at RT. The optical-to-optical slope efficiency of 33.9% is the highest, to the best of our knowledge, among all Cr4+:YAG lasers, whether they are in bulk or fiber forms. The low-threshold lasing of 78.2?mW and high efficiency are in good agreement with the simulation. The keys to the high laser efficiency are twofold: one is the improved Cr4+ emission cross section and fluorescence lifetime due to release of the strain on the distorted Cr4+ tetrahedron, which also mitigates photobleaching in Cr4+:YAG; the other is the improved core uniformity at long fiber lengths. In addition, because of the low threshold, the impact of excited state absorption of the pump light is significantly reduced. The effects of crystal-orientation, self-selected, and pump-dependent linear polarization states were also addressed.  相似文献   

14.
激光二极管抽运的被动调QNd3+:YAG微晶片激光器及其稳定性   总被引:8,自引:0,他引:8  
欧攀  闫平  巩马理  谢韬 《光学学报》2002,22(12):465-1469
从理论和实验两个方面研究了连续激光二极管抽运的Cr~(4+):YAG被动调QNd~(3+):YAG微晶片激光器。考虑Cr~(4+):YAG饱和吸收体激发态吸收,推导了连续抽运的被动调Q微晶片激光器的速率方程,分析了微晶片参量对调Q脉冲半峰全宽和峰值功率的影响;提出了实现稳定脉冲输出的微晶片激光器设计原则。在饱和吸收体初始透过率较低(T_0≈40%)的情况下,获得了脉冲峰值功率不稳定性小于±0.7%、脉冲宽度不稳定性小于±1.0%、峰值功率高达千瓦量级的高重复频率激光输出。  相似文献   

15.
The absorption and fluorescence spectra of Cr,Yb:YAG crystal were measured. There are two absorption bands at 940 nm and 968 nm although the absorption coefficient is lower than that of the absorption peak of Yb:YAG superimposed in Cr:YAG absorption peak. The emission peak intensity is 4 times lower than that of Yb:YAG, which may be caused by the existence of the ground state absorption of Cr4+ which quenches the Yb3+ emission intensity. Although the emission peak of Cr,Yb:YAG is lower than that of Yb:YAG, there is an advantage of this crystal which combines the saturable absorber and gain medium into one and can be a self-Q switching laser crystal if Cr,Yb:YAG crystal is pumped with high energy power.  相似文献   

16.
The absorption spectra characters of the (Cr,Yb):YAG,Cr:YAG and Yb:YAG crystals are reported. In the absorption spectra of the (Cr,Yb): YAG crystal,there are two absorption bands at 937 nm and 968 nm respectively,which are suitable for InGaAs diode laser pumping;and there is an absorption band of Cr4+ near 1030 nm,which is suitable for passive Q switch laser output at 1.03 μm. This Cr-Yb-codoped crystal may be a potential material for compact,diode laser pumped passive Q-switched solid-state laser with efficient,high-stable.  相似文献   

17.
1lntroductionThsaturableabsotherswhichhavebeensucceSSfullyusedforpassiveQswitched1asersincludedye['],Lffi:F2colDcenterCrytals['],Cr -doPedcrysds['~'],etc.Amngthem,Cr -doPedCryStalsdevtheedinrecentyearssuchasCr :YAG,Cr :GSGG,andCr :WeSnyandsoon,havetheadVanageSofgoodphoto-chedcalandthermalstabillty,largabsorptbocross-section,besaturableintensityandhighdaInaethreshod.Inaddition,Cr canbedoPedintOgainmediumtoformselfQ-switchedl..,['J.Cr -dopedcrystalsbecomethemostprotalsingsatIJrable…  相似文献   

18.
余先伦  杨伯君  于丽 《光子学报》2006,35(2):161-165
对Cr4+∶YAG固体激光器的吸收效率、量子效率、储存效率和提取效率等本征效率进行了分析.Cr4+∶YAG晶体的吸收截面、发射截面、上能级寿命和激活离子浓度等对激光器的本征效率有很大的影响.提高Cr4+∶YAG晶体的光学品质和激活离子的掺杂浓度,优化泵浦源的运转波长和激光腔的设计都能显著改善Cr4+∶YAG固体激光器的本征效率.  相似文献   

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