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1.
提出并实现了一种基于均匀光纤布拉格光栅(Uniform fiber Bragg grating,UFBG)和双环复合子腔滤波器的可调谐单纵模掺铥光纤激光器。3 dB带宽为0.18 nm的UFBG作为波长选择器件,与可进行模式选择的双环复合子腔滤波器相结合,实现了单纵模激光输出。测得激光器的输出波长为2048.69 nm,光信噪比为71.82 dB。60 min内的最大波长和功率波动分别为0.03 nm和0.76 dB。此外,激光器的相对强度噪声在>0.5 MHz时,低于-127.81 dB/Hz;采用基于3×3耦合器的非平衡迈克尔逊干涉仪装置测得0.001 s时激光线宽为7.7196 kHz。通过调整微位移平台改变作用在均匀光栅上的应力,单纵模激光实现了5.1 nm范围可调谐输出。  相似文献   

2.
《发光学报》2021,42(9)
提出了一种基于光纤Bragg光栅Fabry-Pérot (F-P)窄带滤波器和复合双环腔滤波器的单纵模掺铥光纤激光器。通过对复合双环腔进行数值仿真并实验制作,结合光纤Bragg光栅F-P滤波器的窄带滤波特性,实现了光纤激光器的单纵模选取。激光器输出波长为1 941.56 nm,光信噪比为55.8 dB,70 min内的波长和功率波动分别小于0.019 nm和1.464 dB。由自制的基于非平衡迈克尔逊干涉仪线宽测试系统测量了所提出的掺铥光纤激光器输出单纵模激光的频率噪声特性,并用β线方法由频率噪声谱估计了不同测量时间下的激光线宽,2 ms测量时间下的典型激光线宽值为14.194 kHz。  相似文献   

3.
稳定可调谐的单纵模多环形腔掺铒光纤激光器   总被引:2,自引:1,他引:1  
提出了一种多环形腔(MRC)结构的稳定可调的单纵模(SLM)掺铒光纤激光器,多环形腔结构由双环形有源腔和两个次级无源腔组成.这种激光器是利用光纤法布里珀罗可调滤波器(FFP-TF)以及光学光栅滤波器(OGF)两种滤波器和多环形腔结构相结合来共同选模.可实现波长调节范围为1528~1565 nm,在整个波长调节范围内边模抑制比大于44.53 dB,在1554 nm附近边模抑制比可以达到最大值51.18 dB, 输出功率为-8.84 dBm,通过应用多环型腔结构,激光器的输出很稳定,在18 min的观察时间内,中心波长的变化小于0.02 nm,输出功率的变化小于0.04 dBm,实现了稳定且可调谐的单纵模输出.  相似文献   

4.
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   

5.
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   

6.
单纵模布里渊掺铒光纤激光器的实验研究   总被引:4,自引:0,他引:4  
陈伟  张艳  任民  谢亮  袁海庆  王欣  祝宁华 《光学学报》2008,29(9):1740-1744
提出了一种具有多环形腔(MRC)和光纤布拉格光栅可调谐滤波器(FBG-TF)相结合的单纵模布里渊掺铒光纤激光器(BEDFL).实验中通过观察激光器输出光的拍频信号分析其光谱精细结构,分别讨论了布里渊增益、FBG-TF、MRC对BEDFL单模输出的贡献,给出了激光器的功率特性曲线和波长稳定性测试图.实验得到了在1550 nm处功率为4 dBm,信噪比(SNR)>60 dB,线宽小于1.5 kHz的稳定单纵模输出光.  相似文献   

7.
陆俊军  陈淑芬  白杨 《光学技术》2005,31(2):212-213
单模光纤激光器在光通讯和光传感中具有广阔的应用前景。分析了复合腔光纤激光器的构成及单模的实现特点,提出了一种新颖的光纤复合环形腔激光器结构,并对其进行了实验研究。该激光器使用了波长为980nm的半导体激光器作为泵浦源。三个腔长均为2m,彼此之间的腔长差为1~2mm的光纤环形滤波器与主谐振腔构成复合腔。此激光器在波长为1562nm处得到了线宽小于0.1nm的单模激光输出,输出的光功率可达到1mW。该激光器的阈值为5mW,斜率效率为4%。  相似文献   

8.
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   

9.
波长无啁啾调谐窄线宽掺Yb3+双包层光纤激光器   总被引:1,自引:0,他引:1  
用相位掩模法, 在圆形掺Yb3+双包层光纤上制作了Bragg光纤光栅,并用它作为双包层光纤激光器的输出腔镜, 在光栅反射中心波长1055.2 nm位置得到了窄线宽的激光输出, FWHM为0.271 nm, 信噪比约为40 dB.这种结构的双包层光纤激光器, 在双包层增益光纤和后腔镜间没有连接损耗, 减小了双包层光纤激光器体积. 用自行制作的等强度梁对作为输出腔镜的光纤光栅做双向应力调谐, 实现了激光波长无啁啾调谐输出, 调谐范围1051.1~1060.04nm,调谐量达8.9nm, 调谐过程中激光3 dB线宽基本无变化.  相似文献   

10.
基于光纤布拉格光栅对(DFBGs)的双波长线形腔光纤激光器利用偏振烧孔效应实现双波长激光稳定输出的研究颇多,但有关3 dB光纤环形镜(FLM)与光纤布拉格光栅(FBG)构成腔镜或仅FBG构成腔镜,以及DFBGs的选择对其激光输出性能[光信噪比(OSNR)、斜率效率及稳定性等]的影响的研究很少。本文实验首先在双波长线形腔掺铒光纤激光器中比较了3 dB FLM与FBG构成腔镜和仅FBG构成腔镜的双波长激光的输出性能,结果表明,仅FBG构成腔镜的输出性能优于3 dB FLM与FBG构成腔镜的输出。其次在仅FBG构成腔镜的线形腔中对低反射率FBG(输出镜)反射率相同与不同时的输出性能进行了对比,研究表明,低反射率FBG的反射率相同时双波长激光输出具有较高的OSNR、斜率效率和稳定性。接着改变构成腔镜的两对FBG的中心波长间隔分别为4、8、12 nm,研究表明,中心波长间隔越大输出越稳定,OSNR越高,但激光器的斜率效率有所降低。最后在室温环境下实现了两个激光波长分别为1550 nm和1562 nm、OSNR分别为50.24 dB和51.19 dB左右、中心波长变化分别小于0.030 nm和0....  相似文献   

11.
A tunable single-longitudinal-mode(SLM) semiconductor optical amplifier(SOA)-based fiber laser based on a dispersion-shifted fiber(DSF) is proposed and successfully demonstrated. SLM operation is obtained due to the spectral narrowing effect resulting from inverse four-wave mixing in a DSF. A tunable optical filter performs wavelength selection function. By inserting a length of DSF in the laser cavity, SLM lasing can possibly be obtained when laser oscillation is stably established after traveling through the DSF many roundtrips. Stable tunable SLM oscillation with a signal-to-noise ratio as high as 65 dB over a wavelength range of about 35 nm is achieved experimentally, and each spectral linewidth is less than 6.5 kHz.  相似文献   

12.
Chen H 《Optics letters》2005,30(6):619-621
A multiwavelength fiber ring laser obtained by use of a semiconductor optical amplifier (SOA) with a simple laser cavity configuration is reported. A Fabry-Perot filter was used in the fiber laser ring cavity to achieve more than 50 simultaneous wavelength lasing oscillations with a frequency separation of 50 GHz. The resulting stable broadband multiwavelength lasing operation was attributed to broadband and flat gain of the SOA, which has a gain flatness of 0.8 dB for more than 20 nm. The laser has a total output power of -3 dBm and a signal-to-spontaneous-noise ratio of 30 dB.  相似文献   

13.
D. Chen  H. Fu  W. Liu 《Laser Physics》2007,17(10):1246-1248
A novel single-longitudinal-mode (SLM) erbium-doped fiber laser with a simple linear cavity based on a fiber Bragg grating Fabry-Perot filter (FBG-FPF) and a narrowband (~0.06 nm) FBG is proposed and demonstrated experimentally. Two uniform FBGs form the FBG-FPF, which has two ultranarrow transmission bands with a bandwidth of 0.12 pm and a wavelength spacing of 0.095 nm. By slightly tuning the central wavelength of the narrowband FBG, SLM lasing at 1549.658 or 1549.563 nm (corresponding to the two transmission peaks of the FBG-FPF) is achieved with a laser output power of ~4 mW, when the pump power is ~75 mW.  相似文献   

14.
We present a stable linear-cavity single longitudinal mode (SLM) erbium-doped silica fiber laser. It consists of four fiber Bragg gratings (FBGs) directly written in a section of photosensitive erbium-doped fiber (EDF) to form asymmetric three-cavity structure. The stable SLM operation at a wavelength of 1545.112 nm with a 3-dB bandwidth of 0.012 nm and an optical signal-to-noise ratio (OSNR) of about 60 dB is verified experimentally. In laboratory condition, the performance of power fluctuation of less than 0.05 dB observed from the power meter for 6 h and wavelength variation of less than 0.01 nm obtained from the optical spectrum analyzer (OSA) for about 1.5 h are demonstrated. The gain fiber length is no longer limited to only several centimeters for SLM operation because of the excellent mode-selecting ability of the asymmetric three-cavity structure. The proposed scheme provides a simple and cost-effective approach to realizing a stable SLM fiber laser.  相似文献   

15.
An all-optical widely tunable Raman fiber laser has been realized by incorporating a highly nonlinear fiber in a ring cavity. By feedback a portion of Raman Stokes wave back into the highly nonlinear gain medium, a Raman fiber laser is generated. We found that the lasing wavelength of Raman fiber laser can be tuned from 1537 to 1568 nm with peak power fluctuation within 1 dB, giving a total wavelength tunability of 31 nm. The optical signal-to-noise ratio is found to be wavelength dependent, and the highest optical signal-to-noise ratio of about 59 dB is recorded. The lasing threshold of the Raman fiber laser with this configuration is found to be as low as 300 mW.  相似文献   

16.
We present a stable linear-cavity single longitudinal mode (SLM) erbium-doped silica fiber laser. It consists of four fiber Bragg gratings (FBGs) directly written in a section of photosensitive erbium-doped fiber (EDF) to form an asymmetric three-cavity structure. The stable SLM operation at a wavelength of 1545.112 nm with a 3-dB bandwidth of 0.012 nm and an optical signal-to-noise ratio (OSNR) of about 60 dB is verified experimentally. Under laboratory conditions, the performance of a power fluctuation of less than 0.05 dB observed from the power meter for 6 h and a wavelength variation of less than 0.01 nm obtained from the optical spectrum analyzer (OSA) for about 1.5 h are demonstrated. The gain fiber length is no longer limited to only several centimeters for SLM operation because of the excellent mode-selecting ability of the asymmetric three-cavity structure. The proposed scheme provides a simple and cost-effective approach to realizing a stable SLM fiber laser.  相似文献   

17.
In this demonstration, we propose and experimentally investigate a wavelength-selection erbium-doped fiber (EDF) laser in single-longitudinal-mode (SLM) by using simple fiber ring scheme design. We use a tunable bandpass filter (TBF) inside the gain cavity to restrict the lasing frequency. The proposed ring cavities can also serve as the mode filters for side mode suppression. Based on the simple ring cavity design, the mode hopping can be avoided to achieve SLM output. The TBF inside the laser scheme also obtains the wavelength tuning in the range of 1520.02 to 1562.02 nm. In addition, the output performance of the proposed fiber laser has also been discussed.  相似文献   

18.
A stable room-temperature multi-wavelength Brillouin–Raman fiber laser with a ring cavity configuration was proposed and experimentally investigated. An obvious suppressant effect for unstable mode hopping of multi-wavelength lasing oscillations induced by deeply saturated effect was observed in the ring cavity configuration. Stable room-temperature multi-wavelength lasing oscillations with more than 30 lasing lines and wavelength spacing of 0.076 nm were obtained with only 250 mW Raman pump power and a section of high nonlinear fiber with a length of 1.5 km. The lasing output is so stable that the maximum power fluctuations for the foremost three Stokes lines over more than 20 min of observation were less than 0.30 dB. The lasing stability of the laser was also compared with a linear cavity configuration with the same gain components and pump conditions. While using the linear laser cavity configuration, obvious mode hopping was observed. The minimum value of the maximum power fluctuations at all lasing lines over more than 10 min of observation was more than 0.90 dB.  相似文献   

19.
A stable and broad bandwidth multiwavelength erbium-doped fiber laser is proposed and demonstrated successfully. A nonlinear optical loop mirror which induces wavelength-dependent cavity loss and behaves as an amplitude equalizer is employed to ensure stable room-temperature multiwavelength operation. Up to 50 wavelengths lasing oscillations with wavelength spacing of 0.8 nm within a 3-dB spectral range of 1562-1605 nm has been achieved. The measured power fluctuation of each wavelength is about 0.1 dB within a 2-h period.  相似文献   

20.
We propose a simple dual-wavelength Er-doped fiber laser configuration based on a dual-wavelength fiber Bragg grating written on the splice joint between two different fibers for wavelength-selective filter in the Sagnac loop interferometer. The wavelength separation between the adjacent lasing wavelengths is 1.12 nm and the side-mode suppression ratio (SMSR) is over 55 dB. The output power variation is less than 0.8 dB over a two-minute period. Moreover, the lasing wavelength can be effectively tuned using the thermal heating method.  相似文献   

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