排序方式: 共有84条查询结果,搜索用时 31 毫秒
21.
激光烧蚀一分子束(LA-MB)法是研究金属离子与分子团簇反应的有效方法.在气相条件下,用飞行时间质谱观测到激光烧蚀Al等离子体与脉冲分子束超声膨胀产生的甲醇团簇碰撞反应生成的(CH30H)nCH3O-(n=3~23)团簇负离子.实验发现,此序列的团簇负离子主要生成于烧蚀激光作用于脉冲分子束的后段,(CH3OH)3CH3O-离子强度始终远远大于其后的离子,并且这些离子随尺寸大小的分布变化平缓.结合量化计算,在133LYP/6-31G(d)水平上得到(CH3OH)nCH3O-(n=1~4)的可能几何构形,并推断(CH3OH)3CH3O-为-幻数结构. 相似文献
22.
532nm丙酮和丁酮的多光子电离解离研究 总被引:1,自引:1,他引:0
利用激光质谱法,通过分析丙酮和丁酮的多光子电离飞行时间质谱,对其532 nm多光子电离机制进行了研究.结果发现丙酮相干吸收若干光子跃迁到高能超激发态,再继续吸收光子产生各种碎片离子,而丁酮先解离后电离,两质谱中都有质荷比为4、6、8的离子,原则上是高价离子.但在相似条件下未见相关报道,因此对离子出险原因及确认尚待进一步研究,实验中丁酮发生异构现象,其异构体电离解离出较强的C2H3O (m/e=43).丙酮没有相关离子产生. 相似文献
23.
激光烧蚀-分子束(LA-MB) 法是研究金属离子与分子团簇反应的有效方法。在气相条件下,用飞行时间质谱观测到激光烧蚀Al等离子体与脉冲分子束超声膨胀产生的甲醇团簇碰撞反应生成的(CH3OH)nCH3O-(n=3~23)团簇负离子。实验发现,此序列的团簇负离子主要生成于烧蚀激光作用于脉冲分子束的后段,(CH3OH)3CH3O-离子强度始终远远大于其后的离子,并且这些离子随尺寸大小的分布变化平缓。结合量化计算,在B3LYP/6-31G(d)水平上得到(CH3OH)nCH3O-(n=1~4)的可能几何构形,并推断(CH3OH)3CH3O¯为一幻数结构。 相似文献
24.
运用Gaussian 03W程序中的密度泛函B3LYP方法,在6-31 G(d)基组水平上对氨质子化团簇(NH3)nH (n=1~8)的可能的几何构型进行了结构优化,得到了该系列团簇的稳定结构及其对应的总能量.结果表明,氨质子化团簇的稳定结构是质子与一个氨分子结合形成一个NH 4离子核,其它氨分子通过氢键作用形成氨链后与该离子核的四个氢以氢键结合形成的,它们之间的结合力均为中强氢键.另外,我们还利用能量的二阶差分理论对团簇的稳定性进行了研究,并计算了团簇的平均束缚能,发现随着团簇尺寸的增大,团簇的平均束缚能逐渐减小. 相似文献
25.
The multiphoton ionization spectra of dimethylamine are given in the 445-470 nm region. A time of flight mass spectrometer was used,and experiment was done under collision free condition. It is found that (2+2) resonance enhanced multiphoton ionization through (nN,3s) Rydberg state produces parent ions which endure pseudo-α and C—N bond cleavages. The former forms CH3N+H=CH2 ions,and the latter gives CH2=N+H2 ions . 相似文献
26.
二乙胺分子的多光子电离:"梯转换"过程 总被引:1,自引:0,他引:1
The multiphoton ionization (MPI) of diethylamine is first reported in this paper. A time-of-flight mass spectrometer was used in the experiment under collision-free condition. MPI mass spectra were measured in the region of 464 ~486 nm using a dye laser and at double frequency of a Nd:YAG laser. Molecular ion was created through resonance enhanced multiphoton ionization (REMPI) via Rydberg states. Fragment, ion distribution was formed through “ladder switching” process. The experimental demonstration of the process is reported for the first time by the discussion of dependence of ion relative, abundance on laser wavelength and energy. The competition between further up-pumping and fragmentation of Parent ion also exists, and higher laser intensity favors the former. 相似文献
27.
激光诱导Al等离子体在背景气体中的流体现象 总被引:3,自引:2,他引:1
调Q-YAG脉冲激光(波长1.06μm,脉宽10ns,能量为250mJ/pu1se)烧蚀Al靶,用短焦距照相系统和光学多道分析仪(OMA)记录了等离子体在氩气背景气体及不同压强下所呈现的流体现象及其等离子体辐射的空间分辨光谱。实验发现,当背景气压为400Pa以下时,在靶面上存在一个明亮的发光球体,球体直径远大于激光烧蚀斑的大小,此球体向四周辐射等离子体光谱,只是在垂直靶面的方向辐射相对较强。在气压约为400Pa,等离子体辐射才以较为明显的羽状体形态向前喷散,且随气压增高,喷散的立体角变小。随着背景气压的继续升高,等离子体羽被压缩,成为一个明亮的发光小羽状体,当气压达20~30kPa,发光羽状体开始出现分解的迹象,在羽状体前端形成一个光球。气压继续升高,等离子体羽完全变成一串发光球。离开靶面越远,发光球的半径越大。用光学多道分析系统分析这些发光球的光谱特征,发现在靶面附近主要是Al等离子体的谱线,而较远的发光球,其主要谱线则来自背景气体。在气压为20kPa左右,等离子休羽呈现烧蚀点为明亮的白色亮点,而羽端为鲜艳绿色(氩的514nm)的彩色羽。 相似文献
28.
在低真空条件下(5Pa),通过测量脉冲激光烧蚀平面Al靶产生的等离子体辐射谱的时间分辨特征,得到辐射粒子速度的空间分布.在激光脉冲宽度为10ns,烧蚀斑直径为200μm,靶面上功率密度分别为1.91×1010,5.10×1010和7.64×1010W/cm2时,测得辐射粒子Al的速度均在106cm/s量级,且随着靶面径向距离的增大而近似呈指数衰减.在距靶面的相同距离处,激光功率密度的增大反而使速度减小.利用激波模型(shockwave model)较好地解释了实验结果,并得出激波的波面基本为柱对称
关键词:
激光等离子体
平面Al靶
粒子速度分布
激波 相似文献
29.
30.
Potential energy curves (PECs) for the ground state (X2∑+) and the four excited electronic states (A2∏, B2∏, C2∑+, 4∏) of a Bell molecule are calculated using the multi-configuration reference single and double excited configuration interaction (MRCI) approach in combination with the aug-cc-pVTZ basis sets. The calculation covers the internuclear distance ranging from 0.07 nm to 0.70 nm, and the equilibrium bond length Re and the vertical excited energy Te are determined directly. It is evident that the X2∑+, A2∏, B2∏, C2∑+ states are bound and 4∏ is a repulsive excited state. With the potentials, all of the vibrational levels and inertial rotation constants are predicted when the rotational quantum number J is set to be equal to zero (J = 0) by numerically solving the radial SchrSdinger equation of nuclear motion. Then the spectroscopic data are obtained including the rotation coupling constant w e, the anharmonic constant WeXe, the equilibrium rotation constant Be, and the vibration-rotation coupling constant ae. These values are compared with the theoretical and experimental results currently available, showing that they are in agreement with each other. 相似文献