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Magnetic neutron scattering anti-Bragg solution

机译:磁中子散射抗布拉格溶液

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摘要

A new solution for the elastic spin magnetic scattering of slow neutrons by a N-electron target is obtained. The angular dependence of the differential cross section (DCS) has very unusual (anti-Bragg) shape for a target, which degenerate ground state has zero z -projection (M = 0) of the total spin. Contrary to usual assumption that neutron is scattered by each atomic spin independently, the scattering by the whole target spin system is considered. The many-electron many-determinant wave functions Ψ_a(x _1,...,x_N) (x_j ≡r_jσ _j) are used for analytical calculations of the scattering amplitude. The total spin square eigenfunctions Θ_(S0)(σ_1,...,σ_N) have been used for the spin part of Ψ_a. Explicit analytical expressions for the DCS are obtained and the initial and final neutron polarization effects are discussed. It is shown that the regular pattern of the anti-Bragg diffraction has no relation to the periodic magnetization of the target.
机译:获得了一种慢速中子被N电子靶弹性自旋磁散射的新解决方案。对于目标,微分横截面(DCS)的角度依赖性具有非常不寻常的形状(抗布拉格),其简并基态的总自旋为零z投影(M = 0)。与通常的假设相反,即中子被每个原子自旋独立散射,而是考虑了整个目标自旋系统的散射。多电子多行波函数Ψ_a(x _1,...,x_N)(x_j≡r_jσ_j)用于散射幅度的解析计算。总自旋平方本征函数Θ_(S0)(σ_1,...,σ_N)已用于Ψ_a的自旋部分。获得了DCS的明确解析表达式,并讨论了初始和最终中子极化效应。结果表明,抗布拉格衍射的规则图案与靶材的周期性磁化无关。

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