为抑制光参量振荡器（Optical Parametric Oscillator，OPO）振荡过程中信号光和闲频光向泵浦光的逆转换，首次采用在L型OPO腔的支路中插入信号光倍频晶体LiB₃O₅的（简称LBO）的方式，实现了BaGa₄Se₇（BGSe） OPO闲频光的高转换效率输出，当泵浦激光（1.06 μm）能量为115 mJ时，闲频光（3.5 μm）能量为16.18 mJ，光光转换效率为14.06%，斜效率为18.4%，这是目前已知1.06 μm激光泵浦BGSe OPO最高的转换效率。模拟了不同泵浦能量下L型腔中有无LBO晶体时BGSe OPO腔内的三波波形，并给出了闲频光在实验中的输出波形。与传统OPO腔相比，所提出的L型OPO腔（含倍频晶体）在大能量泵浦条件下抑制了逆转换，可获得更高的闲频光转换效率。

The first photon bias of photon detection results in distortion of the photon waveform, which seriously affects the accurate acquisition of target information. A rapid universal recursive correction method is proposed, which is suitable for multi-trigger and single-trigger modes of photon detection. The calculation time is 2 to 3 orders of magnitude faster than that of Xu et al.’s method. In the experiment, we have obtained good correction results for area targets and targets with varying depths. When the average number of echo photons is 0.89, the correlation distance of the correction waveform is reduced by 85%.

为提高电场传感器的抗电磁干扰能力、灵敏度和稳定性，将高Q值薄壁液芯毛细管微腔和电泳效应结合，增强回音壁模共振微腔对外加电场的感知能力，并进行了实验验证.基于时域有限差分法得到了液芯毛细管微腔回音壁模式共振特性随毛细管直径、壁厚等结构参数的变化规律，发现随着壁厚变薄灵敏度增加.采用熔融拉锥法制备了直径为86 μm，壁厚约为2 μm的薄壁毛细管微腔，通过高精度位移平台实现了锥形光纤和毛细管微腔的高效率耦合，测得回音壁模式Q值为2.8×10⁶.毛细管微腔内注入不同浓度的蛋白质溶液，利用电泳原理和蛋白质分子在缓冲溶液里带电的特性，实现的最大电场传感灵敏度为10.6 pm/（kV/m）.

We propose a nonparallel double-grating structure in a spectral-beam combining technique, where two gratings are placed nonparallel satisfying the Littrow mount in the focal region of the convergent lens. The most attractive advantage of this approach is that it will compress the spectral span into half of its original spectrum, which means the number of combined elements can be doubled in the gain range of diode lasers. Experimental results demonstrate that the CW output power of the combined beam is 30.9 W with a spectral span of 7.0 nm, compared with its original spectrum span of 13.6 nm, and the spectral beam combining efficiency is 70.5%. In consideration that a single grating could have a high efficiency of >97% in a bandwidth of over ten nanometers, the efficiency loss of the grating pair should be less than 6%, which is acceptable for most applications, so this method of using double gratings should be highly interesting for practical applications when a nearly doubled number of diode lasers could be combined into one single laser compared with the previous single-grating methods.