Angular Probability Distribution of Three Particles near Zero Energy Threshold

Physics – Mathematical Physics

Scientific paper

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Scientific paper

We study bound states of the 3--particle system in $\mathbb{R}^3$ described by the Hamiltonian $H(\lambda_n) = H_0 + v_{12} + \lambda_n (v_{13} + v_{23})$, where the particle pair $\{1,2\}$ is critically bound, and particle pairs $\{1,3\}$ and $\{2,3\}$ are neither bound nor critically bound. We prove the following: if $H(\lambda_n)\psi_n = E_n \psi_n$, where $E_n \to 0$ for $\lambda_n \to \lambda_{cr}$, and besides $\lim_{n \to \infty}\int_{|\zeta| \leq R} |\psi_n (\zeta)|^2 d\zeta = 0$ for any $R>0$, then the angular probability distribution of three particles determined by $\psi_n$ for large $n$ approaches the exact expression, which does not depend on pair--interactions. The result has applications in Efimov physics and in the physics of halo nuclei.

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