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Irreducible correlation functions of the S matrix in the coordinate representation:Application in calculating Lorentzian half-widths and shifts

机译:S矩阵在坐标表示中的不可约相关函数:在计算洛伦兹半宽和位移中的应用

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By introducing the coordinate representation,the derivation of the perturbation expansion of the Liouville S matrix is formulated in terms of classically behaved autocorrelation functions.Because these functions are characterized by a pair of irreducible tensors,their number is limited to a few.They represent how the overlaps of the potential components change with a time displacement,and under normal conditions,their magnitudes decrease by several orders of magnitude when the displacement reaches several picoseconds.The correlation functions contain all dynamical information of the collision processes necessary in calculating half-widths and shifts and can be easily derived with high accuracy.Their well-behaved profiles,especially the rapid decrease of the magnitude,enables one to transform easily the dynamical information contained in them from the time domain to the frequency domain.More specifically,because these correlation functions are well time limited,their continuous Fourier transforms should be band limited.Then,the latter can be accurately replaced by discrete Fourier transforms and calculated with a standard fast Fourier transform method.Besides,one can easily calculate their Cauchy principal integrations and derive all functions necessary in calculating half-widths and shifts.A great advantage resulting from introducing the coordinate representation and choosing the correlation functions as the starting point is that one is able to calculate the half-widths and shifts with high accuracy,no matter how complicated the potential models are and no matter what kind of trajectories are chosen.In any case,the convergence of the calculated results is always guaranteed.As a result,with this new method,one can remove some uncertainties incorporated in the current width and shift studies.As a test,we present calculated Raman Q linewidths for the N_2-N_2 pair based on several trajectories,including the more accurate "exact" ones.Finally,by using this new method as a benchmark,we have carried out convergence checks for calculated values based on usual methods and have found that some results in the literature are not converged.
机译:通过引入坐标表示,Liouville S矩阵的摄动展开式的推导是根据经典表现的自相关函数来表示的。由于这些函数以一对不可约张量为特征,因此它们的数量有限。势分量的重叠随时间位移而变化,并且在正常情况下,当位移达到几皮秒时,其幅度会减小几个数量级。相关函数包含计算半角宽度所需的碰撞过程的所有动力学信息,并且它们的行为良好,尤其是幅度的迅速降低,使人们能够轻松地将其中包含的动态信息从时域转换到频域。更具体地说,因为这些相关性功能受时间限制,它们连续的傅立叶应该先限制频带的变换。然后,可以用离散傅里叶变换精确地替换后者,并使用标准的快速傅里叶变换方法进行计算。此外,人们可以轻松地计算其柯西主积分,并得出计算半角和位移所需的所有函数。引入坐标表示并选择相关函数作为起点的最大好处是,无论潜在模型有多复杂,无论哪种模型,都能够高精度地计算半角和位移。无论如何,始终保证计算结果的收敛性。因此,使用这种新方法,可以消除当前宽度和位移研究中包含的一些不确定性。作为测试,我们提出了计算的拉曼Q基于多个轨迹(包括更精确的“精确”轨迹)的N_2-N_2对的线宽。最后,通过将此新方法用作作为基准,我们已经根据通常的方法对计算值进行了收敛检查,发现文献中的某些结果没有收敛。

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