Why there is no Efimov effect for four bosons and related results on the finiteness of the discrete spectrum

Abstract

We consider a system of $N$ pairwise interacting particles described by the Hamiltonian $H$, where ${\sigma }_{ess}(H)=[0,\infty )$ and none of the particle pairs has a zero energy resonance. The pair potentials are allowed to take both signs and obey certain restrictions regarding the fall off. It is proved that if $N\ge 4$ and none of the Hamiltonians corresponding to the subsystems containing $N-2$ or less particles has an eigenvalue equal to zero then $H$ has a finite number of negative energy bound states. This result provides a positive proof to a long--standing conjecture of Amado and Greenwood stating that four bosons with an empty negative continuous spectrum have at most a finite number of negative energy bound states. Additionally, we give a short proof to the theorem of Vugal'ter and Zhislin on the finiteness of the discrete spectrum and pose a conjecture regarding the existence of the "true" four--body Efimov effect.

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• Comment on the article "On the Existence of the N-Body Efimov Effect" by X. P. Wang
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• Progress in methods to solve the Faddeev and Yakubovsky differential equations
• Zero Energy Bound States and Resonances in Three--Particle Systems
• Zero Energy Bound States in Many--Particle Systems
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Cited by in corpus (4)

• Proof of the Super Efimov Effect
• Absence of a four-body Efimov effect in the 2 + 2 fermionic problem
• The absence of the Efimov effect in systems of one- and two-dimensional particles
• Universal low-energy behavior in three-body systems