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1.
提出并实验研究了一种2μm波段全光纤间隔可调双波长光纤激光器.该激光器采用传统的环形腔设计,以最大输出功率33dBm的1 565nm光纤激光器为泵浦源,4m单模掺铥光纤为增益介质,腔内为嵌入多模干涉滤波器的Sagnac环的复合滤波结构.该复合滤波器可实现间隔可调谐,高边模抑制比的双波长激光信号输出.通过泵浦功率的控制和对复合滤波器中偏振控制器的调节,实现双波长3nm到80nm间隔可调的激光输出,边模抑制比为60dB,线宽为0.2nm,功率稳定度为±1.5dB/h,双峰能量差小于4dB.  相似文献   

2.
基于多模光纤滤波器的可调谐掺铒光纤激光器   总被引:1,自引:0,他引:1  
研究了一种新型、全光纤、宽带可调谐环形腔掺铒光纤激光器。该激光器利用由单模-多模-单模光纤组成的滤波器实现波长可调谐及激光器的全光纤结构。该滤波器将多模光纤缠绕在偏振控制器上,两端分别与一段单模光纤相连,通过调整偏振控制器的状态,实现了中心波长1542~1560nm的不同激光输出。单波长连续可调谐激光器的波长可调范围为18nm,边模抑制比大于40dB,3dB线宽为0.096nm;进一步调整偏振控制器的状态和抽运功率,实验同时得到了连续可调谐的双波长、三波长等多波长激光输出。对于可调谐的多波长激光器,通过调整偏振控制器的状态,可实现波长间隔及输出中心波长两者可调。  相似文献   

3.
提出并设计了一种基于光纤环形滤波器的环形腔掺Er3+光纤激光器,实现了稳定的单波长和双波长激光输出.采用保偏光纤布喇格光栅作为选频器件;两支分光比为20∶80的1×2耦合器结合2m保偏光纤构成环形滤波器,抑制模式跳变,提高激光输出稳定性,通过调节滤波器内偏振控制器实现波长选择性输出;采用长度为1m的饱和吸收体起到稳频作用.实验结果表明:该激光器工作阈值为71mW,在熔接滤波器后,光谱特性得到改善;调节偏振控制器可实现单波长激光可切换输出或双波长激光同时输出,双波长间隔0.88nm,1 535.5nm和1 534.7nm单波长切换输出时最大功率分别为0.078dBm和-2.585dBm,激光3dB线宽为0.16nm和0.15nm;在室温20min内,输出激光波长漂移小于0.06nm,功率变化小于1.3dB.  相似文献   

4.
研究了一种新型、全光纤、宽带可调谐环形腔掺饵光纤激光器.该激光器利用由单模-多模-单模光纤组成的滤波器实现波长可调谐及激光器的全光纤结构.该滤波器将多模光纤缠绕在偏振控制器上,两端分别与一段单模光纤相连,通过调整偏振控制器的状态,实现了中心波长1542~1560 nm的不同激光输出.单波长连续可调谐激光器的波长可调范围...  相似文献   

5.
掺Yb3+光纤环形激光器研究   总被引:4,自引:4,他引:0  
报道了采用环形腔结构,使用偏振敏感的光隔离器构成掺Yb3+光纤激光器激光输出特性研究结果.用976 nm半导体激光器作为泵浦激光,获得了2.35 mW的最大输出功率,激光的中心波长为1.0537 μm,泵浦阈值功率为42 mW.在改变腔内偏振控制器的状态时,激光器的输出波长移动到1.066 μm.在时域,实验观测到掺Yb3+环形激光器的自脉动信号输出.  相似文献   

6.
单频窄线宽分布布拉格反射光纤激光器研究   总被引:8,自引:0,他引:8  
分析了单频窄线宽分布布拉格反射(DBR)光纤激光器的单模工作条件,在此基础上算出单模工作区域,制作了一个单频窄线宽分布布拉格反射光纤激光器。该激光器在波长为975.5nm的半导体激光器抽动下,在1556.91nm波长处。当抽运功率为55.35mW时输出功率可达1.43mW,频宽小于1.2MHz(受测量仪器分辨率限制)。经测量,该输出激光是稳定的单纵模输出。  相似文献   

7.
光纤光栅选频环形腔掺Yb3+光纤激光器   总被引:4,自引:0,他引:4  
采用自行研制的掺Yb^3 单模光纤和新颖的全光纤连接方案,实现了1060nm窄线宽、环形腔光纤激光器的成功运转。从理论和实验上探讨了耦合器输出比对激光器输出性能的影响,对不同光纤长度所构成的激光器进行了实验研究,发现在现有实验条件下12m为最佳长度。入纤抽运阈值功率约为30.2mW,当入纤功率达最大值42.8mW时,得到最大激光输出7.5mW,半峰全宽≤0.2nm,相对于入纤抽运功率的斜率效率为61.7%。  相似文献   

8.
 通过延长激光器环形腔腔长,利用高浓度掺杂的单模掺镱光纤,搭建了超低重复频率、全正色散结构的半导体可饱和吸收镜被动锁模光纤激光器。激光器的中心波长、重复频率、平均功率及单脉冲能量分别为1 064 nm,281.5 kHz,11 mW和39 nJ。为了稳定中心波长,实现自启动,激光器腔体内接入了一个带通滤波器。该激光器运行稳定,无调Q不稳定现象,极大减小了半导体可饱和吸收镜被损坏的机会。  相似文献   

9.
为实现具有高脉冲能量的调Q脉冲激光输出,利用微纳光纤-单壁碳纳米管复合的方法制备可饱和吸收体,并对基于该类型可饱和吸收体器件的被动调Q掺镱光纤激光器进行研究。采用拉伸法将普通单模石英光纤拉制成微纳光纤,将其与单壁碳纳米管溶液复合,进一步制备成全光纤集成型器件。将该器件置于环形腔掺镱光纤激光器中,利用976 nm半导体激光器作为抽运源。当抽运功率为53 mW时,实现了调Q脉冲激光输出,激光中心波长为1 039 nm。进一步提升抽运功率至76 mW,可获得脉冲宽度为3.1μs、重复频率为25.5 kHz、单脉冲能量为941nJ的调Q脉冲激光输出。研究表明,利用微纳光纤制备的可饱和吸收体器件具有较高的损伤阈值,可用于实现高脉冲能量的激光输出。  相似文献   

10.
设计了一种基于受激布里渊散射和掺铒光纤混合增益的随机光纤激光器,该激光器选用两段长为20km的单模光纤组成全开放腔结构,利用单模光纤的瑞利散射提供随机光反馈.研究表明,固定布里渊泵浦波长和泵浦功率分别为1 550.00nm和2.19mW时,增加掺铒光纤泵浦功率,可以实现两个波长的随机激光输出,一阶和二阶受激布里渊散射光与布里渊泵浦光波长间隔分别约为0.088nm和0.174nm,产生一阶和二阶受激布里渊散射对应的掺铒光纤泵浦功率分别为190mW和370mW;当掺铒光纤泵浦功率为433mW时,激光器两端的最大输出功率为1.60mW和1.68mW.当掺铒光纤泵浦功率明显高于阈值功率时,获得的一阶和二阶随机激光输出稳定,3dB线宽约为0.022nm,峰值强度和位置基本不随时间而变化.  相似文献   

11.
The generation of a multiple wavelength source using a bismuth-based erbium-doped fiber (Bi-EDF) in a linear cavity configuration is demonstrated. The configuration uses a pair of optical circulators at the input and output ends of the cavity to form a resonator for multi-wavelength generation in conjunction with optical couplers to inject the Brillouin pump (BP) and to tap the output at the two ends. The Brillouin erbium fiber laser (BEFL) comb with a 2.15 m of Bi-EDF has a wavelength spacing of 0.09 nm and operates in long-wavelength (L-) band region. A stable output laser comb of 50 lines is obtained at a BP of 1568.2 nm and 5 dBm and two 1480 nm pumps at 120 mW. The injected BP wavelength and power as well as the 1480 nm pump powers have a great effect on the number of lines and output power of the BEFL. This configuration is compact due to the use of the significantly shorter Bi-EDF as the linear gain medium, and can be made more compact by replacing the single-mode fiber with highly non-linear fibers such as holey fibers.  相似文献   

12.
利用琼斯矩阵对一种三环嵌套的无源谐振腔的选频特性进行了分析,并根据无源谐振腔选频的原理,设计了一种基于三环嵌套无源谐振腔的掺铒光纤激光器。实验结果表明:三环嵌套的无源谐振腔具有良好的选频特性,当泵浦功率为159 mW时,得到了稳定的单纵模激光信号输出;输出功率的最大波动为0.04 dB,输出中心波长最大漂移为0.016 nm;耦合器的耦合比减小时,激光器会处于多纵模振荡状态。  相似文献   

13.
Abstract: Laser resonator is very important in the study and fabrication of lasers. The work conditions and work parameters of rare-earth element-doped optical fiber lasers with two different structures of laser resonators, i. e., the fiber ring resonator and Fabry-Perot resonator are studied. The fineness, laser resonant conditions, laser oscillation conditions and threshold inversion of these two different cavity are deduced. A series of experiments are also given. The result is very valuable to evaluate the output of optical fiber laser and can be a foundation of device fabrication. The Nd~(3 )-doped silica single-mode fiber laser pumped by Ar~ laser with a low threshold of 1.02 mW and a maximum output of more than 1 mW are presented in this paper.  相似文献   

14.
A compact and tunable erbium-doped fiber laser is demonstrated using a highly doped fiber and a microfiber knot resonator (MKR) structure which is laid on the surface of a small peltier. The MKR functions as both a reflector and a tunable filter where tunability is achieved by varying the temperature of the resonator by heating the peltier. A stable laser output is achieved at the 1533 nm region with an optical signal to noise ratio (OSNR) of 27 dB using a 65 mW of 980 nm pump power. The operating wavelength of the laser can be tuned from 1532.60 nm to 1533.49 nm as the temperature is increased from the room temperature of 24 to 90 °C. It is observed that the operating wavelength shifts to a longer wavelength as the temperature increases with an efficiency of 12.4 pm/°C. This is due to the thermally induced optical phase shift attributable to the changes in effective refractive index and optical path length of the MKR loop.  相似文献   

15.
黄元庆 《发光学报》1997,18(3):212-216
本文介绍了一种用波长为809nm的激光二极管(LD)端面泵浦厚度为1mm的微片Nd:YVO4全固化固体激光器。器件结构上采用了一种独特的光学系统,该系统由分别用于LD激光束的耦合和聚焦的两部分组成。由Nd:YVO4的一个平面与一个曲率半径为21mm的球面镜组成半共焦腔,以获得高的转换效率。文中详细讨论了单横模运转时的泵浦光与激光腔模之间的匹配问题。当泵浦光功率为400mW时,获得152mW的1064nm波长的TEM00模激光输出。器件阈值功率为48.3mW,总的光-光转换效率为38%,斜效率为43%.  相似文献   

16.
We report on a wide-band and stable mode-locked all-polarization-maintaining fiber iaser configuration using a noniinear optical loop mirror.The central wavelength of the laser is 1080.14 nm and the 3dB bandwidth is 20.29 nm.The repetition rate of the pulse is 3.28 MHz and the pulse width is 848 ps.By tuning the pump power,which is centered at 980 nm,from 300 mW to 380 mW,we obtain a linearly changed output power from 6mW to 7.12 mW.The all-polarization-maintaining fiber configuration is fundamental to the stability of the output power.  相似文献   

17.
15波长输出的布里渊掺铒光纤激光器   总被引:8,自引:3,他引:5  
多波长布里渊掺铒光纤激光器是一种新型的多波长光纤激光器,其原理是利用受激布里渊增益和掺铒光纤的线性增益,可以在常温下得到波长间隔约为0.08nm(~10GHz)的多波长输出。报道的布里渊掺铒光纤激光器,在布里渊抽运功率为1.7mW、980nm抽运功率为300mW的情况下得到稳定的15个波长(间隔~10GHz)的输出,这种激光器用作光传感器、光谱分析仪以及密集波分复用系统的光源。实验发现,输出波长的个数随着980nm抽运功率的增大而增加。另外,布里渊掺铒光纤激光器的信号功率主要来自于掺铒光纤的增益,而布里渊增益对它的影响不大。  相似文献   

18.
一种结构新颖的L波段掺铒光纤激光器   总被引:1,自引:1,他引:0  
提出了一种结构新颖的L波段环形腔掺铒光纤激光器。用掺铒光纤作为增益介,采用980nm激光器作为前向抽运源,利用起偏器和偏振控制器获得L波段激光,利用光环形器将后向的放大自发辐射再引入铒光纤的前端,重复利用。当抽运功率为103mW时得到了阈值功率约为23.87mW,输出功率达6.34mW的激光输出,斜率效率约为8.05%,与没有重复利用后向放大自发辐射谱的掺铒光纤激光器做比较,该结构对L波段掺铒光纤激光器的性能有明显的提升作用。对于长度不合适的铒纤,在没有重复利用后向放大自发辐射谱时没有获得激光输出;而在利用后向放大自发辐射后,在阈值功率约为88mW时得到了激光输出,从而很好地证明了上述结论。  相似文献   

19.
Fiber laser resonator configurations have been analyzed theoretically on the basis of steady-state rate equations to optimize the laser conversion efficiency. Evolution of the pump- and signal powers and the saturated gain coefficient along the length of the laser medium has been simulated for high- and low-finesse resonators in forward- and backward pumping schemes. The corresponding fiber laser configurations have been setup to verify the results of simulation. Backward pumping configuration in an Yb-doped fiber laser has been found to be the most efficient, and in this configuration a maximum cw output power of 10.75 W in single transverse mode with an optical-to-optical conversion efficiency of 62.5% has been achieved. The laser output spectrum was peaked at 1093 nm with full-width at half-maximum (FWHM) line-width of about 9 nm. In the low-finesse resonator configuration, it has been found that experimental observations differ from theoretical simulation results. In this case, output power from both ends ceases to increase linearly beyond 1.8 W, and starts fluctuating due to the onset of strong random self-pulsing phenomenon. Our investigation shows that a non-uniform steady-state gain along the fiber length facilitates the self-pulsing process.  相似文献   

20.
用于Rb原子冷却系统的半导体激光放大(TPA)装置   总被引:2,自引:2,他引:0  
报道了我们最近研制的780 13m半导体激光放大装置.激光放大管采用Eagleyard公司生产的(EYP-TPA-0780-01000)半导体锥形放大器,当输入的种子源激光功率为25 mW时,放大器输出的激光功率达600mW左右,该光束经过透镜整形,声光调制器频移,然后耦合到单模保偏光纤后,输出功率达110 mW.该激光放大装置可很好的用于高密度冷原子的俘获.  相似文献   

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