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Analyzing the Contribution of Individual Resonance Poles of the S-Matrix to Two-Channel Scattering

机译:分析S矩阵的各个共振点对两通道散射的贡献

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A two-channel problem is considered within a method based on first-order differential equations that are equivalent to the corresponding Schrodinger equation but more convenient for dealing with resonant phenomena.Using these equations,it is possible to calculate directly the Jost matrix for practically any complex value of the energy.The spectral points (bound and resonant states)can therefore be located in a rigorous way,namely,as zeros of the Jost matrix determinant.When calculating the Jost matrix,the differential equations are solved and thus,at the same time,the wave function is obtained with the correct asymptotic behavior analytically embedded in the solution.The method offers a very accurate way of calculating not only total widths of resonances but their partial widths as well.For each pole of the S-matrix,its residue can be calculated rather accurately,which makes it possible to obtain the Mittag-Leffler-type expansion of the S-matrix as a sum of the singular terms (representing the resonances)and the background term (contour integral).As an example,the two-channel model by Noro and Taylor is considered.It is demonstrated how the contributions of individual resonance poles to the scattering cross section can be analyzed using the Mittag-Leffler expansion and the Argand plot technique.This example shows that even poles situated far away from the physical real axis may make significant contributions to the cross section.
机译:在基于一阶微分方程的方法中考虑了两个通道的问题,该方程等效于对应的薛定inger方程,但更易于处理共振现象。使用这些方程式,可以直接计算出约斯特矩阵因此,可以严格地定位光谱点(束缚状态和共振状态),即作为Jost矩阵行列式的零。在计算Jost矩阵时,需要求解微分方程,从而同时,通过解析地嵌入解决方案中获得正确的渐近行为来获得波动函数。该方法不仅提供了计算共振的总宽度,还计算出其局部宽度的非常准确的方法。对于S矩阵的每个极点,它的残基可以相当精确地计算出来,这使得获得S矩阵的Mittag-Leffler型展开成为奇异项之和成为可能。例如,考虑了Noro和Taylor的双通道模型。它演示了如何使用Mittag分析单个共振极对散射截面的贡献。 -Leffler展开和Argand绘图技术。此示例表明,即使极点远离物理实轴,也可能对横截面做出重大贡献。

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