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arXiv:1204.0435 · Journal of Spectral Theory

Absence of bound states implies non-negativity of the scattering length

Robert Seiringer

Published Jun 24, 2012• 5 citations
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Abstract

We show that bosons interacting via pair potentials with negative scattering length form bound states for a suitable number of particles. In other words, the absence of many-particle bound states of any kind implies the non-negativity of the scattering length of the interaction potential.
DOI
10.4171/jst/31

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We consider bosons interacting through a narrow sss-wave resonance. Such a resonance is characterized by an infinite scattering length and a large and negative effective range r0r_0r0​. We argue that any number N≥3N\ge3N≥3 of bosons can form a self-bound cluster with the binding energy per particle increasing as N2N^2N2 for 1≪N≪(−r0/abg)1/21\ll N\ll (-r_0/a_\text{bg})^{1/2}1≪N≪(−r0​/abg​)1/2, where abga_\text{bg}abg​ is the background scattering length (between atoms and molecules). In the opposite limit N≫(−r0/abg)1/2N\gg (-r_0/a_\text{bg})^{1/2}N≫(−r0​/abg​)1/2, bosons form droplets with binding energy per particle saturating to a constant value independent of the particle number. The stability of clusters and droplets when the interaction is detuned from the resonance is also studied.
We establish that the ability of a localized trapping potential to bind weakly interacting bosons is dramatically enhanced in the vicinity of the threshold of formation of the single-particle bound state of the trap. Specifically, for repulsive particles and a superthreshold trapping potential the equilibrium number of bound bosons and the size of the ground state diverge upon approaching the single-particle threshold from above. For attractive interactions and a subthreshold trap, a collective bound state always forms for a sufficiently large number of bosons, despite the inability of interparticle attraction alone to form a two-body bound state.
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