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1.
光诱导雄黄矿物同质异象变化的显微成像拉曼散射研究   总被引:1,自引:0,他引:1  
利用拉曼光谱研究了激光照射诱导雄黄的同质异象变化,这些结果证实了下面的反应:由于As—As键相对较弱,首先As—As键被破坏,有1个S原子加入到As—As键中,形成As—S—As键。此时由As4S4(Realgar类型)变化为As4S5相,而As4S5处于不稳定状态,As4S5相变化为 Pararealgar时有1个S原子从As—S—As键中释放出来。释放出来的S原子又加入到另外1个As4S4(Realgar)中,引起As4S4(Realgar)相变化为As4S5,As4S5进而分裂为1个S原子和As4S4(Pararealgar类型)。照射促进雄黄经由 As4S5 分子被转换成副雄黄。  相似文献   
2.
We demonstrate a high efficiency multi-kW diode-side-pumped Nd:YAG laser. High cooling efficiency of the diode-side-pumped module in the laser is achieved. The middle portion of the Nd:YAG rod in the module is cooled by a coolant jet with screwed side surface, and the end-caps of the rod without screwed side surface are cooled by Au coated on the surface. The thermal effect of the laser rod is reduced, which leads to high output power with high optical-optical conversion efficiency. By using three identical Nd:YAG laser modules, an output power of 4.2 kW and beam quality of 58 mm・mrad with an optical-optical efficiency of 35% at 1064 nm is obtained in a laser oscillator. By using four identical Nd:YAG laser modules, an output power of 3.1 kW and beam quality of 17 mm・mrad with an optical-optical efficiency of 25.8% is demonstrated in a master oscillator power-amplifier system.  相似文献   
3.
1-苯胺基萘 - 8-磺酸盐 (ANS)在不同的固体基质中发光特性的研究发现 :(1 ) ANS分子发射峰位置与在甲醇溶液中相比 ,发生明显的蓝移 ,可能是由于约束在固体基质中的荧光分子的运动受到一定的限制而接近单分子发光的行为。与纯粉末 ANS荧光相比 ,发生红移。ANS在极性的滑石基质中 ,发射峰移向更短的波长 ,在非极性的石蜡基质中移向更长的波长 ,反映固体基质微观环境的变化。 (2 ) ANS分子荧光寿命明显缩短 ,主要原因是在固体基质中 ,荧光发射速率常数 kf 增大。 (3) ANS分子相对量子产率明显增大 ,荧光分子运动受限 ,减弱分子之间的相互作用 ,减小了由于碰撞引起的猝灭 ,分子结构刚性增强。该结果对于研究固体基质的物化性质、探讨光化学反应中能量转移现象具有重要意义。  相似文献   
4.
含油岩心显微荧光成像光谱研究   总被引:6,自引:1,他引:5  
发展了一种显微荧光光谱成像技术,并将其应用于天然岩心进行显微荧光成像光谱研究。利用这种技术同时采集含油岩心表面的荧光光谱信息和空间信息.并对获得的光谱图像给予光谱学和地质学解释。结果表明,不但能显示岩心形貌和组分的大致趋势,而且能揭示其精细细节.为石油地质研究提供了一种新方法,为今后的石油勘探开发工作提供了一种先进的指导手段。  相似文献   
5.
We demonstrate an all-solid quasi-continuous-wave (QCW) narrow-band source tunable to sodium D2a line at 589.159 nm. The source is based on sum-frequency mixing between lasers at 1064 nm and 1319 nm in a LBO crystal. The 1064 nm and 1319 nm lasers are produced from two diode side-pumped Nd:YAG master oscillator power amplifier (MOPA) laser systems, respectively. A 33 W output of 589 nm laser is obtained with beam quality factor M^2 = 1.25, frequency stability better than ±0.2 GHz and linewidth less than 0.44 GHz. A prototype 589 nm laser system is assembled, and a sodium laser guided star has been successfully observed in the field test.  相似文献   
6.
A Continuous-Wave Diode-Side-Pumped Tm:YAG Laser with Output 51W   总被引:1,自引:0,他引:1       下载免费PDF全文
A compact diode-side-pumped Tm:YAG laser is presented, which can output 51 W of cw power at 2.02 μm. The Tm:YAG rod is side pumped by nine diode arrays with the central wavelength of 783nm and the with bandwidth of about 2.5 nm at 25^o C. To decrease the thermal effect on the both ends and dissipate the heat effectively, one composite Tm:YAG rod with the undoped YAG end caps and the screw threads on the side surface of the rod is used as the laser crystal. The maximum optical-to-optical conversion efficiency of the 2.02-μm laser output is 14.2%, with a slope effciency of 26.8%  相似文献   
7.
8.
We report a Q-switched 2-μm Tm:YAG laser based on intracavity-pumped by a 1064-nm Nd:YAG laser operating at room temperature for the first time. An average output power of 5.1W is obtained with the repetition rate of 30kHz and a pulse width of 300ns. In addition, we demonstrate a 12.5-W continuous-wave 2-μm Tm:YAG laser, which is, to our best knowledge, the highest power for intracavity-pumping configuration.  相似文献   
9.
The essential goal of that paper (Chin. Phys. Lett. 26(2009) 124211) was to obtain a 2μm Tm:YAG laser with short pulse output. A Q-switched technique is used to realize the short pulse output in our laser system. The idea presented by Dr. Nieolaie Pavel is right. In our work, the directly Q-switched 2μm Tm:YAG pulse laser is not realized. As a matter of fact, the Q switch is used to directly switch the 1μm Nd:YAG laser.  相似文献   
10.
使用高数值孔径的物镜通过显微拉曼扫描成像的方法获得了方铅矿结晶体的空间分辨的分子信息。实验中包括不同尺寸大小的晶体和不同强度的激发光功率。从逐点扫描(步长为0.5μm)的显微探针成像方法获得的光谱数据分析,得到了化学组分的空间分布。多变量数据分析处理得到PbS及其退化产物的特征光谱。在非破坏性激发条件下,PbS的特征谱线很弱。在强激光的光化作用下,在微米尺度大的样品点上产生完全不可逆的氧化反应,把PbS氧化为α-PbO。对于大尺度的PbS晶体,通过拉曼扫描成像光谱在照明点附近还发现了铅的氧硫酸盐包括4PbO.PbSO4,3PbO.PbSO4和PbO.PbSO4。  相似文献   
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