共查询到20条相似文献,搜索用时 484 毫秒
1.
利用反应显微成像谱仪开展了56 keV/u的Ne~(4+)离子与羰基硫(OCS)气体的交叉碰撞实验,研究了Ne~(4+)离子诱导的OCS~(3+)的碎裂动力学.通过符合探测三个末态离子,重构了OCS~(3+)离子三体碎裂对应的牛顿图和Dalitz图,并明确区分了直接解离和次序解离两种碎裂过程.重构了OCS~(3+)离子解离过程的动能释放(KER)分布,发现其峰值在25 eV处,同时在18 eV处有肩膀结构的存在,其中25 eV左右的峰来源于直接解离过程,18 eV处的肩膀结构来源于次序解离和非次序解离两种过程.通过分析不同能量和不同电荷态下重离子碰撞实验所得到的KER谱,发现微扰强度不是影响态布居的主要因素.OCS~(3+)次序解离中的第二步KER的峰值在6.2 eV处.结合以往的实验结果,我们得出结论:多电离态的分子发生次序碎裂的根源在于二价离子碎片存在亚稳态,而重构得到的第二步KER可以反映亚稳态离子的电子态信息. 相似文献
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利用可调谐真空紫外同步辐射和分子束实验装置在8.0~15.5 eV的光子能量范围内,研究2-甲基-2-内烯-1-醇的光电离解离.测出母体离子和碎片离子:C_4H_8O~+、C_4H_7O~+、C_3H_5O~+、C_4H_7~+、C_4H_6~+、C_4H_5~+、C_2H_4O~+、C_2H_3O~+、C_3H_6~+、C_3H_5~+、C_3H_3~+、CH_3O~+和CHO~+的光电离效率曲线,并获得母体分子的电离能和碎片离子的实验出现势.在B3LYP/6-31+G(d,p)理论水平上,计算光电离过程中母体分子、过渡态和中间体的稳定结构.采用CCSD(T)/cc-pVTZ耦合簇方法计算零点能,得到母体电离能和碎片离子的出现势.通过实验和理论研究,提出2-甲基-2-丙烯-1-醇的光解离路径,分子内氢转移是其中大部分解离途径中的主要过程. 相似文献
3.
《化学物理学报》2019,(3)
利用可调谐真空紫外同步辐射和分子束实验装置在8.0~15.5 eV的光子能量范围内,研究2-甲基-2-内烯-1-醇的光电离解离.测出母体离子和碎片离子:C_4H_8O~+、C_4H_7O~+、C_3H_5O~+、C_4H_7~+、C_4H_6~+、C_4H_5~+、C_2H_4O~+、C_2H_3O~+、C_3H_6~+、C_3H_5~+、C_3H_3~+、CH_3O~+和CHO~+的光电离效率曲线,并获得母体分子的电离能和碎片离子的实验出现势.在B3LYP/6-31+G(d,p)理论水平上,计算光电离过程中母体分子、过渡态和中间体的稳定结构.采用CCSD(T)/cc-pVTZ耦合簇方法计算零点能,得到母体电离能和碎片离子的出现势.通过实验和理论研究,提出2-甲基-2-丙烯-1-醇的光解离路径,分子内氢转移是其中大部分解离途径中的主要过程. 相似文献
4.
532nm激光作用下甲基异丙基酮的电离解离研究 总被引:1,自引:1,他引:0
在532 nm激光波长下,利用时间飞行质谱(TOF-MS)对甲基异丙基酮的多光子电离解离机制进行了研究.实验结果显示,母体分子首先发生α断裂并且吸收(2+2)个光子到达离子态.主要的质谱峰C_2H_3~+,CH_3COC_3H_7~+,CH_3~+等在质谱图中清晰可见.结合Guassian03,运用HF/3-21G、CIS/3-21G对基态和激发态的构型进行了优化和频率计算,发现激发态的碳氧键变为介于碳氧单键和双键之间特殊键,并用QST2方法找到了其中的过渡态,对三个状态的几何结构参数进行了分析得出了其解离过程是α键断裂和基团构象转化协同进行的结论. 相似文献
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利用离子速度成像方法,研究CH2I2分子在277—305nm范围内若干波长处的光解离动力学.通过同一束激光经(2+1)共振多光子电离(REMPI)过程探测光解碎片I(2P32)和I(2P12),得到了不同激发波长处的离子速度分布图像,从而获得CH2I2光解产物的能量分配和角分布.实验发现,碎片CH2I自由基有很高的内能激发,约占总可资用能的80%,该能量分配可以较好地用冲击模型来解释.实验还发现,产物I(2P32)和I(2P12)具有很不相同的平动能分布,结合所得到的碎片能量分配和角分布,我们对碎片I(2P32)和I(2P12)生成机理进行了分析,指出CH2I2分子电子激发态的绝热和非绝热解离决定了碎片的平动能分布.
关键词:
CH2I2
离子速度成像
绝热和非绝热解离 相似文献
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采用密度泛函理论研究了中性循环中Ir(CO)_3I催化甲醇羰基化制乙酸的反应机理,计算得到了反应路径上各驻点的几何构型与频率,通过能量和振动分析证实了过渡态的真实性.结果表明,Ir(CO)_2I与CH_3I作用后,亲核加成过程出现反应路径中最大能垒(40. 3 kJ/mol),使用能量跨度模型分析了反应过程的动力学信息,确定了反应的能量跨度和决速中间体和决速过渡态分别为IM1和TS12,亲核加成过程为反应的决速步骤,得到了298 K催化剂的转化频率3. 2×10~(-6)s~(-1). 相似文献
10.
利用同步辐射真空紫外光,研究了HFC-152a(CH3CHF2)的光电离和光解离过程,通过测量各离子的光电离效率曲线,得到了该分子的电离能(11.94±0.04eV)和所有碎片离子的出现势,运用GAUSSIAN-03程序计算了母体和碎片及相应离子的结构、电子态和能量. 结合理论计算的结果,分析了母体离子可能的光电离解离通道及相关通道的解离能.
关键词:
同步辐射
光电离
出现势
HFC-152a 相似文献
11.
卤代烷烃会破坏臭氧层,而碘乙烷(C2H5I)是卤代烷烃中重要代表物质之一.采用离子速度成像技术、飞秒激光技术和飞行时间质谱技术,探究了C2H5I的多光子电离解离动力学.通过分析C2H5I在强场作用下多光子电离解离得到的解离通道、碎片的动能、角度分布和各向异性参数等信息来研究碘乙烷离子(C2H5I+)C–I键裂解机理.根据飞行时间质谱实验,C2H5I在飞秒激光脉冲作用下发生多光子电离解离得到的碎片有C2H5+,I+,CH2I+,C2H2+,C2H3+,C2H4+等.与C–I键相关的碎片为C2H5+和I+,解离机制分别对应于C2H5I+→C2H5++I和C2H5I+→C2H5+I+.同时,采用离子速度成像技术研究C2H5I+的C–I键裂解产生的C2H5+和I+的速度影像,得出两者的速度分布和动能分布,分析结果表明C–I键裂解产生C2H5+和I+的过程都存在高能通道和低能通道.进一步分析解离碎片离子的角度分布发现C2H5+解离时各向异性参数接近于0,可能对应于慢速的振动预解离过程.I+在解离时各向异性参数较高,可能源于排斥势能面上的快速解离过程.最后采用密度泛函理论计算了C2H5I分子电离前后构型变化、离子态的能级强度及谐振强度,对C2H5I+的解离机制做了更进一步的分析和讨论. 相似文献
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By using strong-field scheme, the complete d5 energy matrix with symmetry has been constructed. Then, by diagonalization of this matrix at normal and various pressures,the whole energy spectrum [including the ground-state zero-field splitting (GSZFS)] and its pressure-induced shift (PS) of Znlb:Mn2+ have uniformly been calculated. The results are in very good agreement with experimental data. According to the eigenfimctions and PS, the assignments of four absorption bands have been given. By taking into account the dect of different deformations of t2 and e radial wavefunctions on t23(4A2)e2(3A2)4 A1 and t23(2E)e2(3A2)4E, the position of the third absorption band at normal pressure has been estimated.The tetragonal field is important for GSZFS of ZnTe:Mn2+ and its PS, which supports the existence of tetragonal Jahn-Teller distortion in ZnTe:Mn2+ The physical essentials of typical levels, GSZFS and their PS have been revealed. 相似文献
14.
Rhallabi A. Catherine Y. 《IEEE transactions on plasma science. IEEE Nuclear and Plasma Sciences Society》1991,19(2):270-277
A transport and reaction model of a low-pressure, high-frequency (13.56 MHz) CH4 plasma used for diamondlike carbon (a -C :H ) deposition was developed. The model includes reactions among four molecular species (CH4, C2 H6, C2H4, and H2), five radicals and atom (CH3, CH2, CH, C2H5, and H), and four ions (CH4+ , CH3+, CH5+, and C 2H5+). It also accounts for the influence of the sticking coefficient of species at the walls. Calculated values of the dissociation degree for several flow rates are in good agreement with experimental measurements made by quadrupole mass spectroscopy. A simple surface-model based on the hydrogen coverage of surface and ion flux and energy at the substrate surface was established. This model permitted the calculation of the deposition rate on the powered electrode as a function of the power applied to this electrode. Good agreement between experimental and calculated growth rates was obtained when CH3, C2H5, and CH2 were assumed to participate in film formation, and when hydrogen removal by ion bombardment with variable energy as a function of the power was included in the model 相似文献
15.
采用高温固相法制备了SrZn2(PO4)2:Sn2+(SZ2P:Sn2+), SrZn2(PO4)2:Mn2+(SZ2P:Mn2+), SrZn2 (PO4)2:Sn2+, Mn2+(SZ2P:Sn2+, Mn2+) 荧光粉. 通过X射线衍射、激发和发射光谱详细研究了荧光粉的物相和发光性质. 在SrZn2(PO4)2 基质中, Sn2+离子发射光谱是峰值位于461 nm宽带谱, 归属于Sn2+离子的3P1→1S0能级跃迁, SZ2P:Mn2+激发光谱由基质吸收带(200–300 nm)和位于352, 373, 419, 431和466 nm的一系列激发峰组成, 分别对应Mn2+离子的6A1(6S)→4E(4D), 6A1(6S)→4T2(4D), 6A1(6S)→[4A1(4G), 4E(4G)], 6A1(6S)→4T2(4G)和6A1(6S)→4T1(4G)能级跃迁, 因此, SZ2P:Sn2+ 的发射光谱与SZ2P:Mn2+的激发光谱有较大范围的重叠. 结果表明Sn2+对Mn2+发光有明显的敏化作用. 基于Dexter电多极相互作用能量传递公式和Reisfeld近似原理分析, 荧光粉SZ2P:Sn2+, Mn2+中Sn2+-Mn2+离子之间的能量传递机理属于电四极-电四极相互作用引起的共振能量传递, 并计算出Sn2+-Mn2+离子之间能量传递临界距离Rc ≈ 1.78 nm. 通过改变Sn2+, Mn2+离子掺杂浓度, 实现了荧光粉发光颜色的调节, 在254 nm短波紫外激发下荧光粉发出较强的蓝白光. 研究结果表明SZ2P:Sn2+, Mn2+荧光粉有望应用于紧凑型节能灯照明领域, 随着半导体紫外芯片技术的发展, 有潜力应用于未来的白光发光二极管照明领域. 相似文献
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By using strong-field scheme, the complete d5 energy matrix with D2d symmetry has been constructed. Then, by diagonalization of this matrix at normal and various pressures,the whole energy spectrum [including the ground-state zero-field-splitting (GSZFS)], its PS and the g factor of the ground state for zns:Mn2+ have uniformly been calculated. According to the eigenfunctions and PS, the new assignments of five absorption bands have been given.The variation of tetragonal field with pressure makes a main contribution to the pressureinduced shift (PS) of GSZFS of zns:Mn2+, which supports the existence of tetragonal Jahn-Teller distortion in zns:Mn2+. It is found that when P≥62 kbar, t24(3T1)e4T1 merges with t2e4 2T2, which has to be taken into account in the calculation of PS of the fifth band in the range of 1 bar ~ 95 kbar. It is demonstrated that the Mn2+ ions in ZnS:Mn2+ have tetrahedral coordination, and the difference between ζ and ζ' caused by the covalency effect is very important for GSZFS. The physical essentials of typical levels, GSZFS and their PS have been revealed. By taking into account the influence of covalency on t23(4A2)e2(3A2)4A1 and t23(2E)e2(3A2)4E, the positon of the third absorption band at normal pressure has been estimated. 相似文献
18.
Traditional ligand-field theory has to be improved by taking into account
both pure electronic contribution and electron-phonon interaction one
(including lattice-vibrational relaxation energy). By means of improved
ligand-field theory, the R line,
t23 2T1 and t23 2T2
lines, t22 (3T1)e4T2, t22 (3T1)e4T1 and t2
e2(4A2)4T1 bands, g factors of t23 4A2 and t23 2E, four strain-induced level-splittings and R-line thermal shift of
MgO:V2+ have been calculated. The results are in very good agreement with the experimental data. It is found that for
MgO:V2+, the
contributions due to electron-phonon interaction (EPI) come from the
first-order term; the contributions from the second-order and higher terms
are insignificant. In thermal shift of R line of MgO:V2+, the
temperature-dependent contribution due to EPI is dominant. The results
obtained in this work may be used in theoretical calculations of other
effects of EPI. 相似文献
19.
S. P. Feofilov A. A. Kaplyanskii A. B. Kulinkin R. S. Meltzer T. N. Vasilevskaya 《Journal of luminescence》2002,100(1-4):155-161
We report optical studies of the new material – Cr3+-doped lithium–germanate glass, containing Li2Ge7O15 (LGO) nanocrystalline particles. While only broadband 4T2–4A2 fluorescence from the low-field octahedral Cr3+ sites was observed from Cr3+ ions in the glass, in LGO nanocrystals high-field Cr3+ centers emit 2E–4A2 (R–lines) fluorescence. The process of crystallization in the course of isothermal annealing of glasses was monitored spectroscopically and the nucleation of LGO crystallites was observed starting from the smallest clusters. Using the 2E–4A2 fluorescence spectra it is possible to detect the ferroelectric phase transition in LGO:Cr3+ nanocrystals, whose critical temperature was found to be similar to that of the bulk crystals. Long-lived spectral holes were burned in the inhomogeneously broadened R-lines of Cr3+ in LGO nanocrystals at low temperatures. The linear temperature dependence of hole widths shows that the homogeneous broadening of 4A2–2E transitions of Cr3+ in nanocrystals is due to interaction of Cr3+ electronic levels with the two-level systems (TLS) of the surrounding glass. The range of the Cr3+-TLS elastic dipole–dipole interaction is estimated. 相似文献
20.
大气臭氧层因吸收太阳紫外光, 是人类必不可少的保护伞. 氟利昂在太阳光辐射下解离生成破坏臭氧的游离态氯原子, 是破坏大气臭氧层的主要元凶之一. 本文利用飞行时间质谱技术和离子速度成像技术研究了氟利昂F113(三氟三氯乙烷)分子在800 nm 飞秒光作用下的多光子电离解离动力学. 利用飞行时间质谱探测技术, 得到了三氟三氯乙烷在该波长飞秒激光作用下发生多光子电离解离产生的碎片质谱. 通过荷质比对碎片质谱进行了详细的标定和分析. 在质谱上未发现母体离子, 所有观察到的离子都是由于激光脉冲作用下产生的碎片. 三个最主要的碎片离子是CFCl2+, CF2Cl+, C2F3Cl2+. 通过飞行时间质谱标定, 发现并归属了多个解离通道. 三个主要的解离机理分别为: 1) C-Cl键断裂直接生产氯自由基的通道C2F3Cl3+→C2F3Cl2++Cl; 2) C--C键断裂C2F3Cl3+→CFCl2++CF2Cl; 3) C--C键断裂C2F3Cl3+→CF2Cl++CFCl2. 利用离子速度成像技术对这三个主要通道产生的碎片离子进行成像, 得到了C2F3Cl2+, CFCl2+和CF2Cl+离子的速度影像. 由C--Cl键断裂产生的碎片离子C2F3Cl2^{+}的速度分布由两个高斯分布曲线拟合, 而由C--C键断裂产生的碎片离子CFCl2+和CF2Cl+可以用一个高斯曲线拟合. 通过影像分析得到了解离碎片的平动能分布和角向分布各向异性参数等详尽的动力学信息. 结合高精度密度泛函理论计算对解离动力学进行了进一步的分析和讨论.深入认识氟利昂的解离动力学可为进一步控制破坏臭氧层提供理论参考和实验依据. 相似文献