The S matrix and the f matrix amplitudes are considered for the case of two coupled elastic scattering channels, which differ in values of orbital angular momenta. Matrix elements of S and f matrices are parametrized in terms of scattering phases δ i (i = 1, 2) and a mixing parameter e{epsilon} and are expressed in terms of matrix elements c ij = (K −1) ij where K is the reaction K matrix. Quantities gij(k)=kli+lj+1cij(k){g_{ij}(k)=k^{l_i+l_j+1}c_{ij}(k)} are expanded in powers of k 2, k being the relative momentum of colliding particles B and C. Then functions g ij (k) and c ij (k) are continued analytically to the pole of amplitudes f ij corresponding to the bound state A of colliding particles. This procedure allows to get the position of the pole as well as the residues of amplitudes f ij at that pole which are related directly to vertex constants and asymptotic normalization coefficients corresponding to the vertex A → B + C.
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机译:对于两个耦合的弹性散射通道,考虑了S矩阵和f矩阵的振幅,它们的轨道角动量值不同。 S和f矩阵的矩阵元素根据散射相位δ i sub>(i = 1,2)和混合参数e {epsilon}进行参数化,并根据矩阵元素c 表示。 ij sub> =(K −1 sup>) ij sub>其中,K是反应K矩阵。数量g ij sub>(k)= k l i sub> + l j sub> +1 sup> c ij sub>(k){g_ {ij}(k)= k ^ {l_i + l_j + 1} c_ {ij}(k)}扩展为k 2 sup>的幂,k为相对然后,函数g ij sub>(k)和c ij sub>(k)解析地持续到振幅f ij p>的极点。 sub>对应于碰撞粒子的束缚状态A。此过程允许获得极点的位置以及该极点处的振幅f ij sub>的残差,这些残差与顶点常数和对应于顶点A→B + C的渐近归一化系数直接相关。
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