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Physical Review A

Fate of multiparticle resonances: From Q -balls to He3 droplets

Dam Thanh Son, Mikhail A. Stephanov, Ho-Ung Yee

Published Nov 28, 2022• 9 citations
Publisher

Abstract

The authors study a system of $N$ nonrelativistic particles which form a near-threshold resonance. They find that some many-body quantum objects, for example, clusters of about 30 ${}^{3}$He atoms, while being metastable, cannot decay through emission of one particle at a time. Rather, they decay via a spontaneous mini-explosion where all the constituent atoms are released at once.

DOI
10.1103/physreva.106.l050801

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The authors study a system of NNN nonrelativistic particles which form a near-threshold resonance. They find that some many-body quantum objects, for example, clusters of about 30 3{}^{3}3He atoms, while being metastable, cannot decay through emission of one particle at a time. Rather, they decay via a spontaneous mini-explosion where all the constituent atoms are released at once.
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We consider a system of NNN nonrelativistic particles which form a near-threshold resonance. Assuming no subset of these particles can form a bound state, the resonance can only decay through an "explosion" into NNN particles. We show that the decay width of the resonance scales as EΔ−5/2E^{Δ-5/2}EΔ−5/2 in the limit when the energy EEE of the resonance goes to zero, where ΔΔΔ is the ground state energy of a system of NNN particles in a spherical harmonic trap with unit frequency. The formula remains valid when some pairs of final particles have zero-energy sss-wave resonance, but the Efimov effect is not present. In the limit of large NNN, we show that the final particles follow a Maxwell-Boltzmann distribution if they are bosons, and a semicircle-like law if they are fermions. We argue that metastable 3^33He droplets exist with the lifetime varying over many orders of magnitudes ranging from a fraction of a nanosecond to values greatly exceeding the age of the Universe.
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.
In a recent work [Phys. Rev. Lett.94, 143201 (2005)], we reported an accumulation of three-body resonant states attached to n=2n=2n=2 and higher two-body thresholds. A more careful investigation revealed that there are resonances of the same kind above the n=1n=1n=1 threshold as well. This suggests that the resonances attached to the thresholds are Efimov resonances.
In the frames of quantum electrodynamics, the behavior of spontaneous decay is investigated for a single two-level atom embedded into a microscopic object (cluster). The transition frequency of cluster atoms is supposed to be considerably detuned from the transition frequency of decaying atom. The consideration is performed on the base of fully microscopic quantum-electrodynamical approach with simultaneous solution of Heisenberg equations for atomic and quantum field operators. The special attention is paid to the investigation of renormalization of spontaneous emission rate due to proper account of discrete structure of medium. The formula for decay rate is obtained without using the notion of refractive index. It is obtained that spontaneous decay strongly depends on the geometrical arrangement of atoms in microstructure. For some form of clusters, decay rate is found to be considerably large compared to its vacuum value that is not the case for macroscopically large dielectrics.