可调谐激光器腔内色散棱镜及其组合

分析了色散棱镜的特性及其顶角设计问题。讨论了色散棱镜和扩束棱镜在布鲁斯特角入射状态下，可组合使用的形式及单程角色散。提出将色散棱镜与扩束棱镜组合使用，可减少色散棱镜个数而获得更大角色散的方法。并据此设计了两个色散棱镜组，在Ｔｉ∶Ｓ激光器中得到实际使用。     

分析双Amici棱镜角度误差对色散的影响

双Amici棱镜为复合棱镜结构,作为成像光谱系统中的分光元件,避免了单棱镜色散结构存在的多种问题。双Amici棱镜的加工生产要对其各个角度提出生产指标,而角度误差对于光谱成像系统的色散性是有影响的。针对一种编码孔径成像光谱仪,设计了符合性能指标要求的双Amici棱镜,并从光线追迹的角度出发,计算得到双Amici棱镜色散的数学模型。针对给出的一特定光学系统中的棱镜结构推导了棱镜各个角度单独对线色散的影响,并分析给出各个角度构成的误差链对线色散的综合影响,最终给出了棱镜的生产指标。分析结果有助于指导系统中该棱镜的加工生产。     

二棱镜系统二阶和三阶色散的理论计算

基于光的色散和棱镜光谱仪的特点,采用等光程方法推导了紧凑累加型二棱镜系统二阶和三阶色散的表达式,并分析具体实例。通过计算机模拟得出二阶和三阶色散曲线,为可调谐激光的线宽压窄提供了一定的理论依据。     

非布儒斯特角情况下四棱镜组二阶、三阶色散的解析表示

给出非布儒斯特角情况下四棱镜组二阶、三阶色散的解析表示,并给出改变入射角和入射波长以及棱镜顶角对二阶、三阶色散的影响. 关键词：     

棱镜对色散补偿系统的时域ABCD矩阵分析方法

讨论了棱镜对的负色散效应,利用时域ABCD矩阵方法分析了高斯型光脉冲经棱镜对色散补偿系统的脉宽和啁啾的变化,指出输出光脉冲的脉宽是展宽还是压缩,与棱镜啁啾、棱镜间距和光脉冲在棱镜中传输的距离的取值有关.讨论了棱镜对色散补偿系统对脉冲压缩的最佳条件,指出此时输出光脉冲脉宽随棱镜啁啾的增大而骤减,且骤减程度随啁啾增大而逐渐削弱,最后趋于一稳定值.     

恒偏向高分辨率变束棱镜光谱仪

现有的各种棱镜光谱仪器中,色散分光棱镜都采用等腰或等边棱镜(简称三棱镜),棱镜顶角一般为58-63°.这种棱镜都工作于最小偏向角状态,这时光线的出射角等于入射角,棱镜内的光线平行于底边,而出射光束宽度显然等于入射光束宽度,即两侧光束是对称的.当旋转棱镜时,满足上述条件波长的单色光即被分离出来.这就是单色仪的工作原理.对于摄谱仪器,只有一个波长工作于最小偏向角,其他则近似工作于最小偏向角,但其出射光束宽度仍等于成近似等于入射光束宽度.我们把这种等束工作的棱镜称作“等束棱镜”.至今,所有棱镜光谱仪器中的分光棱镜,均是这种棱…     

采用双石英棱镜对的掺钛蓝宝石自锁模激光器

给出了双棱镜对二、三阶色散的解析式。报道了采用双石英棱镜对的掺钛蓝宝石自锁模激光器的实验结果，获得与理论分析一致的结论。     

温差条件下组合色散棱镜支撑结构的实验分析

介绍了超光谱成像仪采用的组合色散棱镜的支撑结构形式,讨论了温度变化对成像的影响。根据使用需求选择了支撑座的材料,模拟了5～10℃温差条件下棱镜组件的变形情况。利用有限元法解决材料线膨胀系数不同所引起的棱镜反射面变形,并分析了采用聚四氟乙烯垫片做温度补偿后垫片的厚度及接触面积对石英棱镜面型的影响。实验结果表明,在支撑座和棱镜之间增加聚四氟乙烯垫片后,石英棱镜的面型达到了λ/6的指标要求。本文提出的优化方法为组合色散棱镜支撑结构的设计提供了参考依据。     

薄膜法布里-珀罗滤光片中的超棱镜效应

基于薄膜法布里珀罗滤光片在其峰值波长处具有较大群延迟的特性,设计并从实验上验证了光束倾斜入射时这种结构中存在的超棱镜效应。根据光学薄膜理论中的特征矩阵法,数值模拟计算了器件的群延迟和空间色散曲线,镀制并对器件进行了测试。测试结果表明器件在透射峰值波长处因超棱镜效应引起的空间色散最大位移值达到65μm,与理论计算结果非常吻合;相对于传统的光栅和棱镜器件而言器件具有更高的空间角度色散,实际测试在784.5 nm至786.5 nm波长范围内器件的角色散达到30°/nm。     

星载高分辨率超光谱成像仪分光方式的选择

从多个方面分析了棱镜和光栅色散分光的优缺点,分析结果表明棱镜更适于星载高分辨率超光谱成像仪的分光。在透过率方面,棱镜光谱仪透过率高达95.24％(VNIR),而光栅的衍射效率仅为60%~70%。在杂散光方面,棱镜光谱仪的杂散光可达10－4,而光栅的杂散光为10－2。在0.4 －2.5 范围,棱镜光谱仪相对光栅光谱仪有优越性。在色散线性方面,光栅光谱仪基本线性,棱镜光谱仪的短波非线性问题可通过复合棱镜进行补偿。可靠性方面,棱镜光谱仪较光栅光谱仪有优势;在光谱带宽和成本方面,棱镜光谱仪与光栅光谱仪基本接近。     

In-line dispersion prisms and methods of tuning for different wavelengths

Some in-line dispersion prisms have been previously devised to select a particular wavelength line of a multiple-wavelength laser. This paper considers how these prisms could be coupled and scanned so there is no deviation of the beam at any given wavelength line and no lateral displacement of the line.     

宽谱段共光轴线色散成像光谱仪三棱镜分光系统设计

针对棱镜型成像光谱仪结构复杂、具有严重的色散不均匀性,进行了共光轴线色散棱镜式宽谱段成像光谱仪研究。利用棱镜的色散公式建立了对称型三棱镜组合分光结构的数学模型,获得了满足直视结构的棱镜组合,并在此基础上分析影响棱镜组色散线性因素：棱镜材料的折射率和色散率对棱镜组线色散影响比较大,入射角度对其影响比较小,并提出改善色散线性的方法,获得了满足线色散要求的棱镜组合的折射率条件,从而为共光轴结构的线色散棱镜式成像光谱仪初始结构的选择提供了重要理论依据。在工作波段为400~1 000 nm、中心波长偏向角为0°、最大色散角为0.6°、光谱仪系统数值孔径NA为0.18、光谱分辨率为5 nm条件下,实现共光轴三棱镜分光系统的线色散设计,最后利用ZEMAX进行了模拟分析表明,理论计算结果与实际仿真结果基本相符。     

Dispersion theory of multiple-prism beam expanders for pulsed dye lasers

The single pass dispersion of multiple-prism beam expanders of interest for practical pulsed dye laser cavities is calculated. The theory is extended to enable evaluation of the overall (outward and return pass) dispersion of multiple-prism-grating combinations. It is found that although the contribution to overall dispersion from the prisms can be minimized (though not eliminated for practical expanders) by arrangement of the prisms in compensating pairs, it is in any case small (≈2%) compared to the contribution to dispersion from the grating in practical cavities. Formulae for dispersion of multiple-prism-grating combinations including up to four prisms arranged in additive or compensating configurations are given; the dispersion of an arbitrary number of prisms arranged in conjunction with a grating can also be calculated. The implications for output linewidth of pulsed dye lasers incorporating prism beam expanders are discussed.     

脉冲染料激光振荡器的色散问题

本文通过理论推导给出了脉冲染料激光器由多块不同棱镜构成的扩束系统和光栅组合后多程色散的通用计算公式。同时本文也指出光栅与棱镜组合的正确光路安排,从而加大整个系统的色散,减少输出线宽。     

Achromatization of Wollaston polarizing beam splitters

We describe the achromatization of Wollaston prisms to reduce the angular dispersion in the splitting angle. Analytical theory and ray-tracing modeling is presented. In an example application, a sixfold reduction in dispersion is achieved for wavelengths in the region 400 nm to 1.7 μm. Experimental proof of concept is demonstrated, and in an example application, the spectral dispersion of extended images recorded through cascaded Wollaston prisms is shown to be reduced by an order of magnitude.     

Novel dispersion properties of one-dimensional photonic crystals containing a defect made of twin prisms

We design a one-dimensional photonic crystal containing a defect made of twin prisms and study its transmission properties using the transfer matrix method. The incident waves with different wavelengths can be transmitted out at different positions of the last interface of the structure, i.e., one wavelength corresponds to a single export point. Such a structure can be used as a novel dispersion separator. The resolution of this dispersion separator depends on the structure and indices of the twin prisms.     

An accurate method to calculate the negative dispersion generated by prism pairs

Based on the principle of diffraction for light transport in prisms, we figured the physical image for light beams passing through a pair of prisms. The mechanism to induce negative dispersion was analyzed and the numerical expression of optical path length was provided. From a series of mathematical equations, we calculate the quantity of negative dispersion, such as the second- and third-order dispersion, induced by prism pairs. Compared with the expressions of Fork et al. (Opt. Lett. 9(5) (1984) 150), our equations can lead to accurate results and reasonably elucidate the implication of dispersion.