Zero-Energy Bound States of Neutron–Neutron or Neutron–Muon Systems

E. Oks
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Abstract

There exists the following paradigm: for interaction potentials U(r) that are negative and go to zero as r goes to infinity, bound states may exist only for the negative total energy E. For E > 0 and for E = 0, bound states are considered to be impossible, both in classical and quantum mechanics. In the present paper we break this paradigm. Namely, we demonstrate the existence of bound states of E = 0 in neutron–neutron systems and in neutron–muon systems, specifically when the magnetic moments of the two particles in the pair are parallel to each other. As particular examples, we calculate the root-mean-square size of the bound states of these systems for the values of the lowest admissible values of the angular momentum, and show that it exceeds the neutron radius by an order of magnitude. We also estimate the average kinetic energy and demonstrate that it is nonrelativistic. The corresponding bound states of E = 0 may be called “neutronium” (for the neutron–neutron systems) and “neutron–muonic atoms” (for the neutron–muon systems). We also point out that this physical system possesses higher-than-geometric (i.e., algebraic) symmetry, leading to the approximate conservation of the square of the angular momentum, despite the geometric symmetry being axial. We use this fact for facilitating analytical and numerical calculations.
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中子-中子或中子-介子系统的零能束缚态
存在以下范式:对于负的相互作用势U(r),当r趋于无穷时趋于零,束缚态可能只存在于负的总能量E。对于E > 0和E = 0,束缚态被认为是不可能的,无论是在经典力学还是量子力学中。在本文中,我们打破了这种范式。也就是说,我们证明了在中子-中子系统和中子-介子系统中存在E = 0的束缚态,特别是当一对中的两个粒子的磁矩彼此平行时。作为具体的例子,我们计算了这些系统的束缚态的最小允许角动量值的均方根大小,并表明它超过了中子半径一个数量级。我们还估计了平均动能,并证明它是非相对论性的。相应的束缚态E = 0可称为“中子”(用于中子-中子系统)和“中子-介子原子”(用于中子-介子系统)。我们还指出,这个物理系统具有高于几何(即代数)的对称性,导致角动量的平方近似守恒,尽管几何对称是轴向的。我们利用这一事实便于分析和数值计算。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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