窄线宽可调谐半导体激光器

研究了一种利用光栅弱耦合外腔改善可见光半导体激光器性能的方法,并对６５０ｎｍ半导体激光器进行了实验,外腔镜由一个闪耀光栅构成,通过转动光栅角度,获得了窄线宽单模激光输出,谱线宽度０．１ｐｍ,线宽压窄比达９８００,边模抑制比＞２０,并且在约２０ｎｍ的荧光谱宽基础上得到约５ｎｍ波长的连续调谐范围     

全光纤激光器中光栅作为腔镜的特点研究

选用介质膜作谐振腔镜,光纤激光器就缺乏有效的选频机制,使得输出激光线宽较宽,纵模频率和输出功率不够稳定;而光纤光栅作为激光器的谐振腔镜,可以得到稳定的窄线宽激光输出.通过对光纤光栅的形成机理和布拉格光栅选频原理分析,得到双布拉格光纤光栅线型谐振腔的理论.光纤光栅谐振腔的长度与光纤光栅中心波长满足S=(2m-1)λmax...     

外腔半导体激光器的实验研究

本文报道了外腔半导体激光器的一些研究成果。利用闪耀光栅作反馈元件，对808nm波长的半导体激光器形成弱耦合外腔，实现了光谱特笥较好的窄线宽单模激光输出，线宽小于0.06nm，边模抑制比大于30dB，最大输出功率为35.4mW，总的光－光转换效率为46％。通过调整光栅转角，可以得到11.66nm的波长调谐范围。设计了光栅－反向镜联动结构，使外腔半导体激光器的输出方向不再随调谐而变化。     

846 nm半导体激光器线宽压窄的研究

研制了用于倍频蓝光的单模、可调谐的窄线宽光栅外腔反馈半导体激光器,它是由激光器底座、激光管组件、准直透镜组件和光栅组成.经过精密控制电流和温度,利用光栅反馈可获得激光单纵模输出,外腔的结构还使输出光的谱线宽度得以压窄.对研制的半导体激光器的特性测试表明,其输出功率稳定,阈值变小,模式单一稳定,波长可调谐,谱线宽度小于1 MHz.     

掺铒光纤激光器线宽压缩技术的研究

研究掺铒光纤激光器上实现的超窄线宽单模激光输出. 对复合环形腔压缩激光线宽的原理进行了理论分析,讨论了有源复合环形腔参数对激光理论极限线宽产生的影响,并对影响激光线宽的关键参数进行了实验验证,获得了稳定的单纵模激光输出,其线宽小于100Hz,输出最大功率可达2.779mW.     

基于表面等离子体激元的新型金属光栅波导的研究

对基于表面等离子体激元的五层金属光栅透射现象进行了分析研究。根据仿真得出的透射和发射谱线,分析得出五层金属光栅有良好的增透效果。研究中发现在1 550 nm通信波段附近,通过改变金属光栅的周期长度,可以对反射谱进行波长调谐,实现增透波长的选择。     

可调谐掺铒光纤环形腔单纵模激光器

利用驻波干涉和饱和吸收诱发的自写入光纤光栅的窄带滤波特性及反射波长自适应特性,通过内置可调谐介质薄膜滤波器研制成了可调谐掺铒光纤环形腔单纵模激光器。其有效可调谐波长范围达33nm,在波长连续调谐范围之内均为单纵模输出,激光线宽稳定在2.35KHz以下。     

掺镱（Yb3＋）双包层光纤激光器实验研究

光纤激光器具有转换效率高、光束质量好、散热方便、结构紧凑等优点,是高功率激光器领域的研究热点。本文设计了温控、水冷系统使半导体激光二极管泵浦源稳定在工作波长。通过设计的包层泵浦功率剥除器,有效地剥离了未被掺镱（Yb3＋）双包层光纤吸收的泵浦光。采用20w的半导体二极管激光器作为泵浦源,5m长掺镱（Yb3＋）双包层光纤作为增益介质,光纤光栅作为腔镜,在泵浦功率为19w时,获得10．42W的激光输出,激光波长1062nm,光一光转换效率约54．8％。     

基于伸缩杆结构的光纤光栅多级应变传感器

为了扩大光纤光栅称重传感器的测量范围,提高传感器的测量精度,在理论上设计了一套新型的可以扩大测量范围、提高测量精度的系统,并通过Matlab平台仿真.结果表明,单级传感器在波长变化小于0.2nm时具有良好的线性度.该系统将双光纤光栅串联,分别粘贴于等强度梁的上下两侧,采用光强解调的方法实现对光纤光栅输出信号的解调;在解调基础上,利用伸缩杆结构传递载荷重力.实验测试结果验证了多级应变测量的可行性,在保证分辨力的同时扩大了传感器的测量范围.     

30Hz单模超窄线宽光纤激光器

介绍利用光子注入锁模技术在掺铒光纤激光器上实现了超窄线宽单模激光输出;对光子注入锁模技术压缩激光线宽的原理进行了理论分析,讨论了饱和吸收形成的瞬态光纤光栅的参数对激光线宽产生的影响,实现了高边模抑制比的激光输出. 在实验中,通过调节泵浦功率,获得了稳定的单纵模及多纵模激光输出,测量显示输出激光的线宽为30Hz,输出最大功率可达2mW,多纵模时自由光谱范围FSR为1.875kHz.     

基于波片棱镜组合能量调节的切趾光纤光栅

为提高飞秒激光制备高反射率 FBG(Fiber Bragg Grating)的边模抑制比, 提出了一种基于组合二分之一波片和格兰棱镜调节激光能量的加工方法, 制备出了高反射率和高边模抑制比的切趾光纤光栅。 通过上位机输入切趾函数模型, 实时精确调节步进电机速度, 机械旋转二分之一波片位置, 实现激光能量沿光纤方向呈切趾函数分布, 从而在光纤纤芯中折射率调制区域呈切趾函数分布, 获得参数可调的切趾光纤光栅。 实验表明,该方法制备的切趾光栅在 1 550 nm 处反射率可达 70% , 边模抑制比超过 20 dB, 半高峰宽度 0. 35 nm。 对其温度和应力传感特性研究显示, 其温度灵敏度为 1. 529*10^-2nm/ K, 应力灵敏度为 1. 61 nm/ N。 该种方法制备的高反射率切趾光纤光栅有望应用于大功率、 窄线宽的光纤激光器以及高速精确传感解调系统中。     

声光光纤模式耦合的分析

光纤声光器件是基于光纤中的超声光栅引起的两个光波同向模式间的耦合,此文比较了声切变波和疏密波激发的光纤超声光栅对双模光纤中对称模LP01,非对称模LP11间模式耦合的影响,得到一个重要结论：除了光纤超声光栅的周期必须满足这两个耦合模式间的相位匹配条件小,该光纤超声光栅还必须要破坏这两个模式间径向电场的正交性,这一结论为光纤声光器件控制光纤超声光栅产生有效的模式耦合提供了理论依据。     

单频掺Yb3+光纤激光器的研究

根据Yb^3 的光谱特性，提出一种实现激光单频运转的方法，这种方法使用简单的F－P腔，利用饱和吸收体的饱和吸收效应，就可以获得稳定的、窄线宽、单频的激光。     

Fabrication of high quality UV-written fiber bragg gratings

Conclusion In conclusion, we have reported that 98.5 % peak power reflectivity fiber Bragg gratings were fabricated in the core of B/Ge co-doped optical fiber using 248 nm KrF excimer laser pulses to irradiate a phase mask. The fiber gratings fabricated by the method described above have negligible sideband and good wavelength selectivity. They can find applications in WDM optical fiber transmission systems, fiber grating external cavity semiconductor lasers, and rearearth-doped fiber lasers. But more efforts are needed to further improve the transmission spectra of the gratings, because the ripple in the short wavelength side is harmful to their use in WDM systems.     

A steady-state superradiant laser with less than one intracavity photon

The spectral purity of an oscillator is central to many applications, such as detecting gravity waves, defining the second, ground-state cooling and quantum manipulation of nanomechanical objects, and quantum computation. Recent proposals suggest that laser oscillators which use very narrow optical transitions in atoms can be orders of magnitude more spectrally pure than present lasers. Lasers of this high spectral purity are predicted to operate deep in the 'bad-cavity', or superradiant, regime, where the bare atomic linewidth is much less than the cavity linewidth. Here we demonstrate a Raman superradiant laser source in which spontaneous synchronization of more than one million rubidium-87 atomic dipoles is continuously sustained by less than 0.2 photons on average inside the optical cavity. By operating at low intracavity photon number, we demonstrate isolation of the collective atomic dipole from the environment by a factor of more than ten thousand, as characterized by cavity frequency pulling measurements. The emitted light has a frequency linewidth, measured relative to the Raman dressing laser, that is less than that of single-particle decoherence linewidths and more than ten thousand times less than the quantum linewidth limit typically applied to 'good-cavity' optical lasers, for which the cavity linewidth is much less than the atomic linewidth. These results demonstrate several key predictions for future superradiant lasers, which could be used to improve the stability of passive atomic clocks and which may lead to new searches for physics beyond the standard model.     

基于延时零拍法的DFB光纤激光器线宽测量

DFB单频光纤激光器输出的超窄线宽作为光学系统中的一个重要参数需要进行准确的测定,因此,采用延时零拍法重点对1053 nm波长的DFB掺Yb3 光纤激光器的超窄线宽进行了测量,并且研究了差拍光电流谱线的输出特性.针对超窄线宽DFB光纤激光器输出的特点设计了相应的光电转换放大电路,测得1053 nm的DFB光纤激光器的线宽为31 kHz.该测量结果对于窄线宽DFB光纤激光器应用于光纤传感、光纤通信领域具有一定的指导意义.     

基于深紫外激光器的大面积干涉光刻装置研究

搭建了基于266 nm波长深紫外光源的干涉光刻装置，使用平顶光整形器将高斯光整形成平顶光束，在硅基底上制备出面积为8.9 mm×25.4 mm、周期为407 nm的一维光栅结构图形和周期为860 nm的二维孔洞结构。使用扫描电子显微镜（SEM）测量了平顶光产生的一维干涉结构的线宽、周期等参数，并与高斯光产生的一维干涉结构参数进行对比。实验结果表明，加入了平顶光整形器的干涉光刻装置产生的周期性光栅结构图形均匀性提升了21.36％。     

Numerical study of three phase shifts and dual corrugation pitch modulated (CPM) DFB semiconductor lasers based on reconstruction equivalent chirp technology

A distributed feedback (DFB) semiconductor laser with three phase shifts based on reconstruction equivalent chirp (REC) tech-nology is proposed and investigated numerically. With the combination of multiple phase shifts and corrugation pitch modulated (CPM) structure, we also propose a novel and more complex structure named dual CPM, which has a flatter light power distribution along the laser cavity compared with the true double phase shifts DFB laser diode (LD), while the P-I curves are nearly the same. The proposed dual CPM structure is also designed and analyzed based on REC technology. The simulation results show that, the DFB semiconductor laser with complex structure such as phase shifts, or even arbitrary variation of the grating period can be achieved equivalently and easily by changing the sampling structure. But its external characteristics are almost the same as those DFB lasers with true phase shifts, or true arbitrary variation of the grating period. The key advantage of the REC technology is that it varies only the sampling structure and keeps the seed grating (actual grating in sampling structure) period constant. So its fabrication needs only low-cost and standard holographic exposure technology. Therefore we believe this method can achieve the high-end and low-cost DFB LD for mass production.     

外耦合布拉格光栅5um量子级联激光器

窄带宽的AlGaAs/GaAs布拉格光栅耦合到InP的半导体量子级联激光器从而产生稳定的激光频谱,其激 光谱线宽度在1纳米左右。如果不加光栅，非稳定的自由激射的激光器的谱线宽度有30nm左右。隔离的分布式布 拉格光栅可以独立调谐几个纳米。     

外耦合布拉格光栅5μm量子级联激光器

窄带宽的AlGaAs/GaAs布拉格光栅耦合到InP的半导体量子级联激光器从而产生稳定的激光频谱,其激光谱线宽度在1纳米左右.如果不加光栅,非稳定的自由激射的激光器的谱线宽度有30 nm左右.隔离的分布式布拉格光栅可以独立调谐几个纳米.