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激光偏振特性对丙酮和氧气多光子电离质谱信号的影响 总被引:23,自引:11,他引:12
在极性分子丙酮复合物CH3COCH3*H2O和非极性分子氧气的REMPI谱中,母体离子信号强度与激光偏振方向的关系是不同的.改变532 nm激光偏振方向,记录了两种分子母体离子信号强度,实验结果表明,对于氧气分子的母体离子信号强度,激光偏振方向的改变对其没有影响,而对于CH3COCH3*H2O的母体离子信号强度,随偶极矩与激光偏振方向夹角的增加,其母体离子信号强度呈余弦曲线变化,且与夹角余弦的2.1次幂成正比.理论分析显示,CH3COCH3*H2O的REMPI母体离子信号强度应与此夹角的余弦的2次幂成正比.这就说明实验结果和理论分析是相符的. 相似文献
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One-colour resonant two-photon ionization spectrum of the 1-fluoronaphthalene dimer and ab initio calculation 下载免费PDF全文
The one-colour resonant two-photon ionization(R2PI) spectrum of the 1-fluoronaphthalene(1FN) dimer has been studied in the wavelength range of 304 to 322 nm by using a supersonic molecular beam and time-of-flight mass spectrometry.Compared with the original band 00(at 313.8 nm) of the S1 ← S0 transition of the 1FN monomer,a red-shifted band was observed in the 1FN dimer spectrum at about 315 nm with a relatively large linewidth,nearly 2 nm.Based on the consideration of inductive effect and ab initio calculations,this red-shifted band is assigned to the first electronic excited transition of the 1FN dimer.A possible geometric structure of the 1FN dimer is also obtained with calculations that the two 1FN molecules are combined through two hydrogen bonds which are formed between the hydrogen atom of a molecule and the fluorine atom of a neighbouring molecule.A time-dependent calculation was also carried out and the results are consistent with the experimental data. 相似文献
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使用密度泛函理论B3LYP方法,在6-311++G(d , p)基组水平上,研究了C4H5N3O·(H2O)n (n=1~3)分子团簇的基态结构及红外线光谱。通过对C4H5N3O·(H2O)n (n=1~3)分子团簇结构优化,获得了团簇的六种稳定结构。三种最稳定结构的分子团簇的红外光谱表明O—H…O和N—H…O氢键的形成使得O—H和N—H之间伸缩频率减小,发生了红移; O—H…N氢键使O—H之间的伸缩振动频率变大,发生了蓝移。AIM程序分析表明:电子密度的强弱反映了红移和蓝移的大小。之后使用Veda4软件对C4H5N3O·(H2O)n (n=1~3)分子团簇红外光谱的振动频率进行了分析,并对振动频率进行了比较。 相似文献
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355 nm激光作用下质子化丙酮-水团簇的多光子电离质谱 总被引:1,自引:0,他引:1
为研究由氢键形成的超分子体系内的质子化构型,利用355 nm多光子电离(MPI)技术结合飞行时间质谱(TOF-MS)得到丙酮和水的系列团簇质谱.实验观察到的主要产物是质子化的丙酮水团簇.其团簇构型归纳为(CH3COCH3)n(H2O)n-2H+,(CH3COCH3)n(H2O)n-1H+和(CH3COCH3)n(H2O)nH+.利用Gaussian 98程序优化了团簇的离子态构型,通过频率验证了构型的稳定性,并给出了相关能量和零点修正能. 相似文献
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奇偶相干态的Wehl商和Shannon熵 总被引:3,自引:0,他引:3
研究了奇、偶相干态的Wehrl熵和Shannon熵、结果表明,其Wehrl熵随总噪声的增加而增大,并趋向同一个常数。Shannon熵随力学量起伏的减小而减小,且这两种态的Shannon熵均可小于相干态的Shannon熵,但这时并不与压缩效应的出现相对应,因而Shannon熵不能成为压缩存在的判据.。 相似文献
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