A particle locked inside an arrangement of Dirac delta potentials

[hilbert2]

TL;DR Summary

Would a dense enough set of point interaction potentials around a particle keep it confined in a limited space?

Suppose I have a 3D polyhedron with a large number of faces, and put a repulsing Dirac delta potential, $c\delta (\mathbf{x} - \mathbf{x}_i )$ with $c>0$ at each vertex point $\mathbf{x}_i$ of the polyhedron. Could this kind of an arrangement of delta potentials keep a particle such as an electron trapped inside that polyhedral surface as a bound state, or would probability density leak out even with a really densely spaced set of Dirac deltas?

Where I got this idea is this recent MIT study about a possibility to keep neutron locked inside a quantum dot, despite it interacting only with the (highly localized) nuclei and not the electrons.

https://pubs.acs.org/doi/10.1021/acsnano.3c12929

A quantum dot is often modelled as a "particle in 2D or 3D box", so I would guess some kind of arrangement of point interaction potentials is how the neutron quantum dot would be described with a theoretical model, but I can't access the full text of that publication yet.

The problem I posed could be investigated with a numerical calculation by approximating the delta functions with sharp gaussian spikes, but that would be less time consuming with an equivalent 2D version.

 

[Vanadium 50]

A delta function already has one bound state.

 

[hilbert2]

A delta function already has one bound state.

Yes, but only if it has a negative multiplier in front of it.

 

[Vanadium 50]

Are you saying that if you have a system with a potential of zero everywhere except a number of regions where it is greater than zero, does it have any bound states? It does not.

If you imagine a free particle, with a positive delta function at r = R, and a particle originally in the interior, it will eventually tunnel out. If you want to discuss how long this takes, that depends on the details of R and m. As you would expect, as R gets large (especially with respect to 1/m) the time gets long.

But this gets us into the question of "how almost is almost".

 

[hilbert2]

Are you saying that if
If you imagine a free particle, with a positive delta function at r = R, and a particle originally in the interior, it will eventually tunnel out. If you want to discuss how long this takes, that depends on the details of R and m. As you would expect, as R gets large (especially with respect to 1/m) the time gets long.

Actually now that makes sense to me, even if a whole spherical surface acts as a delta potential, the particle will escape. Maybe it's a different situation if there's an infinite number of shells at $r=R$, $r=2R$, $r=3R$ and so on. Or a 3D lattice with point interactions at each lattice site and an empty vacant space somewhere for the particle to stay in.

Edit: In fact, if you look at Fig. 4 of this article, in a 1D imperfect Kronig-Penney lattice with a larger distance between one of the pairs of neighboring potential energy barriers, a particle seems to have a ground state where it's quite localized inside the largest interval available for it. An equivalent 3D version would probably not necessarily have a bound state, because a particle-in-sphere model with finite potential step ($V(r)=0$ when $r<R$ and $V(r)=V_0$ when $r\geq R$) doesn't have one either if $V_0$ isn't large enough compared to how small the volume of the sphere is.