Orthogonally linear polarized lasers(Ⅰ)--principle and devices

Two kinds of orthogonally polarized lasers, i.e. Zeeman dual-frequency lasers and four-frequency ring lasers (laser gyros) have been developed since the invention of lasers, in which circularly polarized lights oscillate. This paper summarizes recent progress of the study on orthogonally linear polarized lasers with the standing wave cavity. Firstly, the expression of producing orthogonally linear polarized lights in standing wave cavity, i.e. laser frequency splitting, is given. Almost all the birefringence effects made in laser cavity are used to produce orthogonally linear polarized lights. The effect includes quartz crystal birefringence effect, calcite birefringence effect,stress (photo-elastic) birefringence effect and electro-optical birefringence effect. Secondly, several physical phenomena of orthogonally linear polarized lasers are discovered such as aberrance of frequency splitting curves caused by optical activity of quartz crystal, order-passing of longitudinal modes with frequency splitting and strong modes competition. Finally, because the traditional Zeeman dual frequency laser cannot output frequency difference larger than 3 MHz, the approaches of obtaining larger frequency difference are studied. The sequential results, several kinds of orthogonally polarized lasers, are described, such as birefringence dual frequency lasers outputting a frequency difference from 40 MHz to hundreds of megahertz, birefringence-Zeeman dual frequency lasers outputting a frequency difference from 1 MHz to hundreds of megahertz, the LD pumped YAG birefringence dual frequency laser outputting frequency difference of several gigahertz, and the lasers whose longitudinal mode spacing is c/4L instead of c/2L.     

工业铝酸钠溶液比热数学模型的研究

本文在实验测定的基础上用数理统计方法建立了工业铝酸钠溶液比热的数学模型,为工业设计与生产中的热工计算提供了一个简单的计算公式,该公式描述了工业铝酸钠溶液中苛性碱、氧化铝、碳酸钠、硫酸钠和温度对比热的影响。     

TDRSS中多普勒频移消除方法的研究

在TDRS通信系统中,用户星相对于中继星的高动态性引入的多普勒频移对扩频信号的捕获造成了很大的困难。文章在分析多普勒频移对PN码捕获性能影响的基础上,采用基带正交对消法去消除多普勒频移,消除了多普勒频移对PN码捕获电路的影响,解决了低信噪比情况下在基带上消除多普勒频移的难题。     

混合设计模型固定效应估计的效率

本文首先给出了混合设计模型中度量估计效率的准则；并证明了在区组设计正交条件下，区组内估计，经曲ＬＳＥ的效率都是１。     

纵向加筋圆柱壳静动力性能分析

用壳条元和流体边界元统一分析了纵向加筋圆柱壳的静动力性能，利用Ｄ′Ａｌｅｍｂｅｒｔ原理和Ｈａｍｉｌｔｏｎ变分原理建立系统运动控制方程．对纵向加筋的布置形式及尺寸大小对于静动力性能的影响进行了系列的数值计算，得出了一些有价值的结论。     

无限大正交加筋层合板的隔声性能分析

基于经典层合板理论,计及加强筋弯曲及扭转运动影响,建立无限大正交加筋层合板传声损失的理论模型.采用空间谐波展开和虚功原理的方法,推导出正交加筋层合板的传声损失计算公式,并将计算结果与简化模型和板梁组合模型的计算结果进行对比,结果吻合良好,验证了所建模型的有效性及广适性.最后,数值分析了层合板铺设方式、铺设角度、刚度、材料损耗因子和加筋间距等参数对结构隔声性能的影响.     

Orthogonally linear polarized lasers (I) — principle and devices

Two kinds of orthogonally polarized lasers, i.e. Zeeman dual-frequency lasers and four-frequency ring lasers (laser gyros) have been developed since the invention of lasers, in which circularly polarized lights oscillate. This paper summarizes recent progress of the study on orthogonally linear polarized lasers with the standing wave cavity. Firstly, the expression of producing orthogonally linear polarized lights in standing wave cavity, i.e. laser frequency splitting, is given. Almost all the birefringence effects made in laser cavity are used to produce orthogonally linear polarized lights. The effect includes quartz crystal birefringence effect, calcite birefringence effect, stress (photo-elastic) birefringence effect and electro-optical birefringence effect. Secondly, several physical phenomena of orthogonally linear polarized lasers are discovered such as aberrance of frequency splitting curves caused by optical activity of quartz crystal, order-passing of longitudinal modes with frequency splitting and strong modes competition. Finally, because the traditional Zeeman dual frequency laser cannot output frequency difference larger than 3 MHz, the approaches of obtaining larger frequency difference are studied. The sequential results, several kinds of orthogonally polarized lasers, are described, such as birefringence dual frequency lasers outputting a frequency difference from 40 MHz to hundreds of megahertz, birefringence-Zeeman dual frequency lasers outputting a frequency difference from 1 MHz to hundreds of megahertz, the LD pumped YAG birefringence dual frequency laser outputting frequency difference of several gigahertz, and the lasers whose longitudinal mode spacing is c4L instead of c2L.     

Orthogonal linear polarized lasers (Ⅱ)--Study on the physical phenomena

The physical phenomena and corresponding theoretical analysis of orthogonal polarized laser are reviewed. Four lasers (or systems) with orthogonal polarized beams are involved. For the birefringence dual frequency laser, its physical phenomena discussed include the alternation between strong mode competition and medium mode competition in cavity tuning; the range of frequency difference of strong mode competition (about 0-40 MHz); four polarization statuses (o-light oscillating but e-light extinguishing, both o-light and elight oscillating, e-light oscillating but o-light extinguishing, both o-light and e-light extinguishing) in cavity tuning; the tuning curves of frequency difference; the influence of optical activity of quartz crystal on polarization direction; and the aberrance of frequency splitting.For the Birefringence-Zeeman dual frequency laser, we focus on its intensity tuning and frequency difference tuning. For the feedback system of orthogonally polarized laser, we discuss the mutual suppression between two orthogonal frequencies, intensity exchange between two orthogonal frequencies and double of intensity fringe frequency. For orthogonally polarized LD-pumped Nd: YAG microchip laser, its property of the dependence of intensity sensitivity on frequency difference is described.     

空间c上正规的正交可加泛函

设ｃ为全体收敛序列所成的空间，赋予常数用的上确界范数，Ｆ为ｃ上的泛函。本文讨论空间ｃ上正规的正交可加泛函的表现形式。     

Orthogonal linear polarized lasers (II)--Study on the physical phenomena

The physical phenomena and corresponding theoretical analysis of orthogonal polarized laser are reviewed. Four lasers (or systems) with orthogonal polarized beams are involved. For the birefringence dual frequency laser, its physical phenomena discussed include the alternation between strong mode competition and medium mode competition in cavity tuning; the range of frequency difference of strong mode competition (about 0?40 MHz); four polarization statuses (o-light oscillating but e-light extinguishing, both o-light and e-light oscillating, e-light oscillating but o-light extinguishing, both o-light and e-light extinguishing) in cavity tuning; the tuning curves of frequency difference; the influence of optical activity of quartz crystal on polarization direction; and the aberrance of frequency splitting. For the Birefringence-Zeeman dual frequency laser, we focus on its intensity tuning and frequency difference tuning. For the feedback system of orthogonally polarized laser, we discuss the mutual suppression between two orthogonal frequencies, intensity exchange between two orthogonal frequencies and double of intensity fringe frequency. For orthogonally polarized LD-pumped Nd: YAG microchip laser, its property of the dependence of intensity sensitivity on frequency difference is described.