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掺铒光纤激光器输出特性的解析研究 总被引:9,自引:4,他引:5
从描述掺铒光纤激光器的速率方程组出发,对980nm和1480nm波段泵浦下掺铒光纤激光器的输出特性进行了解析研究,得到了这两个波段泵浦下下输出功率,斜效率等重要参烽的隐式或显示解析表达式。 相似文献
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掺铒光纤激光器输出特性的研究 总被引:9,自引:3,他引:6
根据掺铒光纤激光器的速率方程,对线性腔连续掺铒光纤激光器的输出特性进行了详细的理论分析,得到了980 nm泵浦的掺铒光纤激光器在稳态条件下的解析表达式.利用数值模拟结果对光纤激光器的上下能级粒子数和泵浦功率沿光纤长度分布以及泵浦阈值、斜率效率等进行了分析和讨论,并进行了980 nm泵浦的掺铒光纤激光器的实验,实验证明:光纤激光器的阈值与理论计算基本一致. 相似文献
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《光学学报》2017,(2)
实验采用共振增强式非线性折射率调制技术实现了半导体可饱和吸收镜锁模全保偏掺镱光纤激光器重复频率的精确锁定。在掺镱光纤激光器的腔内加入一个980/1064nm的波分复用器(WDM)和一段掺铒增益光纤,通过反馈控制加载在该掺铒光纤上的976nm抽运光LD2功率调控掺铒光纤的非线性折射率,进而对激光器的光学腔长实施控制,最终实现重复频率的精确锁定。优化了不同掺铒光纤长度及抽运光初始功率对激光器重复频率控制范围和锁定精度的影响。结果表明:当掺铒光纤长度为1.75m时,通过调整抽运光功率能够实现180Hz的重复频率调整范围;而重复频率的锁定精度仅与抽运光的初始功率密切相关,并不受掺铒光纤长度的明显影响。当LD2抽运光强度为18mW时,重复频率峰-峰值的波动范围小于0.5mHz,相应的标准偏差为0.16mHz,输出功率的标准偏差为0.009mW。此外,通过反馈控制抽运源LD1的强度,并取掉了腔内的掺铒增益光纤及与其相连的WDM,发现由于共振增强非线性和克尔非线性对光纤折射率的叠加,在稳定的单脉冲锁模区间内,重复频率单调变化的范围增加至1kHz,而锁定精度略有降低。 相似文献
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通过求解速率方程,建立了环形掺铒光纤激光器的理论模型.获得了激光器的阈值泵浦功率、输出功率.斜率效率以及最佳掺铒光纤长度的解析解.对结果给予了清晰的物理解释 相似文献
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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
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提出一种简单的理论模型,并通过数值模拟详细研究了可调谐光纤环形腔激光器的输出特性随掺铒光纤长度、输出耦合比、抽运功率、腔内损耗等参量的变化关系.理论分析得到,通过参量优化可以实现在铒离子增益范围内超过130nm带宽(1500—1630nm)的激光输出.实验获得了100nm带宽(15185—16185nm)的可调谐激光输出,激光器输出功率高,信噪比在大部分可调范围内高于60dB,实验结果与理论分析符合得较好
关键词:
掺铒光纤
光纤环形腔激光器
可调谐
光纤珐布里珀罗滤波器 相似文献
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本文对掺铒光纤的自发辐射特性进行了研究,分析了掺杂铒离子光纤的吸收截面、辐射截面、自发辐射谱、净增益系数等的特性,以及在掺铒光纤中,泵浦功率、自发辐射功率、光纤长度、自发辐射谱之间的关系,并用单色仪和波长为1.48um的InGaAsP半导体激光器测试了国产掺铒光纤的吸收谱和它的自发辐射谱。 相似文献
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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
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L波段线型腔波长可调谐掺铒光纤激光器 总被引:7,自引:2,他引:5
报道了工作波长在L波段的由两个光纤环境构成线型谐振腔的掺铒光纤激光器,通过调整环境中偏振控制器的状态来改变环境对不同波长的反射率以实现某些波长的激光输出。线型腔内的激光工作介质为两段不同掺杂浓度的掺铒光纤,其中一段铒光纤由一980nm激光器抽运,其产生的放大自发辐射谱在腔内再同时对两段掺铒光纤进行抽运,使它们的增益谱移位到L波段。实验中观察到了波长从1566.4nm到1592.4nm范围内可调的稳定的连续激光输出,其波长调谐范围达26nm。 相似文献
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The effect of output coupler reflectivity (or output coupling ratio) on the performance of a linear cavity Brillouin/erbium
fiber laser (BEFL) is demonstrated. The operating wavelength, output laser power and number of channels vary with changes
in the coupling ratio in the linear cavity system. The optimum BEFL operation is obtained with an output coupling of 40%,
i.e., 60% of the laser power is allowed to oscillate in the cavity. A stable laser comb consisting of up to 40 channels with
line spacings of approximately 0.09 nm are obtained at the Brillouin pump and 980 nm pump with powers of 2.5 mW and 100 mW,
respectively. The linear cavity BEFL has the potential to be used in inexpensive wavelength division multiplexing system.
相似文献
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A stable and short pulse train of ∼100 MHz repetition frequency was obtained from an erbium doped fiber laser excited by a “continuous” semiconductor laser and by using a linear cavity defined by a Bragg grating pair. The operation frequency of the fiber laser was greater (∼5-15 times) than the cavity round-trip frequency. Emission properties obtained from the erbium doped fiber laser were correlated with those taken from the pump laser, which presented a particular optical noise (very short pulses) added to the continuous emission. From the temporal and radio-frequency analysis of both systems, we conclude that the pump emission characteristics are the responsible of the fiber laser pulsed behaviour. 相似文献
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We developed two kinds of erbium (Er)-bismuth (Bi) co-doped silica fibers with different erbium doping concentrations. After
investigation of its spectral characteristics, it was found that the co-doping of the bismuth could alleviate the clustering
of the erbium ions in the silica fiber and thus improve the fluorescence efficiency. However, the near-infrared (NIR) fluorescence
spectrum attributed to the bismuth ions was different from that reported before and needs further comprehensive investigation.
For the heavy Er doped erbium-bismuth (Er-Bi) co-doped fiber (about 8000 ppm Er concentration), the optical absorption coefficients
at the wavelengths of 976 and 1530 nm are more than 40 and 90 dB/m, respectively. A couple of fiber Bragg gratings with proper
reflectivity were chosen to be spliced to 2 cm long of this fiber forming a compact linear cavity fiber laser. Upon the excitation
of the 976 nm laser diode, stable single frequency fiber laser operation was realized with a maximum side mode suppression
ratio more than 60 dB and a line-width less than 1 kHz. By splicing a segment of the Er fiber to the output end of the fiber
laser, the fiber laser worked in a master oscillator pumping amplifier (MOPA) structure and emitted an increased laser power
of more than 100 mW. 相似文献