原子与分子物理学报
原子與分子物理學報
원자여분자물이학보
CHINESE JOURNAL OF ATOMIC AND MOLECULAR PHYSICS
2015年
4期
531-537
,共7页
光解离动力学%光吸收截面%含时波包法
光解離動力學%光吸收截麵%含時波包法
광해리동역학%광흡수절면%함시파포법
Photodissociation dynamics%Photoabsorption cross section%Time-dependent wave packet method
利用含时波包动力学方法中的劈裂算符-傅里叶变换传播方案和切比雪夫多项式展开方案研究了NaCs分子的光吸收截面,并对由这两种方案计算得出的结果进行了比较。结果表明劈裂算符-傅立叶变换传播方案能更好地展示光吸收截面的中间动力学信息,而在研究初始波包与光吸收截面的关系时,由切比雪夫多项式展开方案获得的结果则更直观。利用后一方案计算的从基态X1∑+不同振动态跃迁到激发态B1∑+上相应的光吸收截面的结果表明,初始波包对光吸收截面有一定的影响,所有振动态的吸收截面均表现出谐振行为,即每一个振动态吸收截面最小值的个数恰好等于基态振动态波函数节点的个数,这种节点映射行为与映射原理相符合。
利用含時波包動力學方法中的劈裂算符-傅裏葉變換傳播方案和切比雪伕多項式展開方案研究瞭NaCs分子的光吸收截麵,併對由這兩種方案計算得齣的結果進行瞭比較。結果錶明劈裂算符-傅立葉變換傳播方案能更好地展示光吸收截麵的中間動力學信息,而在研究初始波包與光吸收截麵的關繫時,由切比雪伕多項式展開方案穫得的結果則更直觀。利用後一方案計算的從基態X1∑+不同振動態躍遷到激髮態B1∑+上相應的光吸收截麵的結果錶明,初始波包對光吸收截麵有一定的影響,所有振動態的吸收截麵均錶現齣諧振行為,即每一箇振動態吸收截麵最小值的箇數恰好等于基態振動態波函數節點的箇數,這種節點映射行為與映射原理相符閤。
이용함시파포동역학방법중적벽렬산부-부리협변환전파방안화절비설부다항식전개방안연구료NaCs분자적광흡수절면,병대유저량충방안계산득출적결과진행료비교。결과표명벽렬산부-부립협변환전파방안능경호지전시광흡수절면적중간동역학신식,이재연구초시파포여광흡수절면적관계시,유절비설부다항식전개방안획득적결과칙경직관。이용후일방안계산적종기태X1∑+불동진동태약천도격발태B1∑+상상응적광흡수절면적결과표명,초시파포대광흡수절면유일정적영향,소유진동태적흡수절면균표현출해진행위,즉매일개진동태흡수절면최소치적개수흡호등우기태진동태파함수절점적개수,저충절점영사행위여영사원리상부합。
The present work investigates the photoabsorption cross section of NaCs by using the split operator-Fourier transform propagation scheme and the Chebyshev polynomial expansion scheme.The comparison of the two calculated results shows that the split operator scheme can better exhibit the intermediate results of the dy-namics process, while the other scheme is hard to satisfy this requirement due to the long time step.In this paper the photoabsorption cross sections, corresponding to the wave packet of the different vibrational states in the ground state transited to the excited states, also are calculated.The results show that the initial wave packet has a certain impact on photoabsorption cross section.The photoabsorption cross section corresponding to the related vibrational state shows a resonant behavior, i.e.the number of the minimum of the cross section corresponding to the each vibrational state is exactly equal to the number of the node of the wave function in the ground vibrational state.This situation caused by the reflection of the wave packet is accordance with the well-known reflection principle.