利用啁啾光纤光栅色散特性实现波长可调谐的主动锁模掺铒光纤环行腔激光器

在环形腔主动锁模光纤激光器中引入啁啾光纤光栅，利用啁啾光纤光栅的大色散特性，通过调节调制频率，实现波长调谐，调谐范围2nm。所得脉冲为重复频率2．5GHz，脉宽约60ps的正啁啾脉冲，。     

若干二维问题的WKB近似能级

讨论了二维空间的WKB近似方法，导出了Bohr-Sommerfeld量子化条件，并计算了若干具体问题的能级，包括中心势情况和Aharonov-Bohm势加中心势情况。     

基于光纤光栅的可调谐半导体激光器

本文利用光纤光栅(FBG)形成外腔反馈及F-P半导体激光器的多模特性,得到波长稳定、可调谐的半导体激光光源,系统研究了不同反馈比率对激光器光谱特性的影响.通过向FBG施加轴向拉力和压力可实现10nm的波长调谐,得到一系列波长间隔0.94nm的激光输出,边模抑制比达35dB,光谱线宽小于0.2nm.     

再谈“负温状态的稳定性”——答王家庆同志

重申了关于负温状态稳定性的观点，认为关于负温状态稳定性的讨论是必要的，稳定性条件的推导是合理的。     

一维Coulomb势

研究了Ｓｃｈｒｏｅｄｉｎｇｅｒ方程在一维ｏｕｌｏｍｂ势ｂ│ｘ│下的精确解，得到决定能级的超越方程及波函数，并给出了大量子数下能级的具体表式。     

介质的物化性质对PstI和PstI^＊活性的影响

利用限制性核酸内切酶PstI在不同的有机介质中的催化反应。研究了水含量、相对粘度，介电常数和渗透压等介质的物化性质对PstI原活性和星号活性的影响。结果表明这4种物化性质对PstI原活性和星号活性的影响恰好相反。     

Description of 114 Cd in the E（5） Symmetry

By analysing the known low-lying levels and the E2 transition rates, it is shown that the empirical scheme of 114Cd is in good overall agreement with the predictions of the transitional dynamical symmetry E(5) proposed by Iachello [Phys. Rev. Lett. 85 (2000) 3580]. This suggests that 114Cd may be better described by an E(5) nucleus than a U(5) nucleus as known before.     

A Novel Method for Measuring the Photo－Induced Birefringence of Photosensitive Fibres Based on a Fibre Loop ＊

We report a novel method for measuring photo-induced birefringence of photosensitive fibres based on a fibre loop.The method is simple and is only slightly affected by the surroundings. The experimental results show that thephoto-inducing normalized birefringence of the photosensitive fibre is multi-decaying-exponentially proportionalto the exposure and it can attain 10^-5.     

A Dual-Wavelength Cladding-Pumped Er^3＋/Yb^3＋ Codoped Fibre Laser System with More Than 2 W Output and Tunable Wavelength Spacing

A dual-wavelength laser system with wideband tunable wavelength spacing and more than 2 W output power is proposed and demonstrated. The operation principle of the laser system is based on the saturation gain characteristic of a cladding-pumped Era＋ /yba＋ co-doped fibre amplifier combining with a wideband tunable fibre laser with fiat power spectrum. The tuning range of the wavelength spacing is continuous within a 35 nm spectral range, and the power difference between both lasing wavelengths can be easily adjusted and controlled by a variable optical attenuator. The total output power can approximately keep unchangeable when the wavelength spacing and the power difference between both lasing wavelengths are continuously tuned and changed. The maximum total output power of the laser system is about 2.22 W.