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Parametric instability of oscillations of a vortex ring in a $z$-periodic Bose-Einstein condensate and the recurrence to starting state (1706.04348v2)

Published 14 Jun 2017 in cond-mat.quant-gas and nlin.PS

Abstract: The dynamics of deformations of a quantum vortex ring in a Bose-Einstein condensate with periodic equilibrium density $\rho(z)= 1-\epsilon\cos z$ has been considered within the local induction approximation. Parametric instabilities of the normal modes with azimuthal numbers $\pm m$ have been revealed at the energy integral $E$ near values $E_m{(p)}=2m\sqrt{m2-1}/p$, where $p$ is the resonance order. Numerical simulations have shown that already at $\epsilon\sim 0.03$ a rapid growth of unstable modes with $m=2$, $p=1$ to magnitudes of order of unity is typical, which is then followed, after a few large oscillations, by fast return to a weakly excited state. Such behavior corresponds to an integrable Hamiltonian of the form $H\propto \sigma(E_2{(1)}-E)(|b_+|2 + |b_-|2) -\epsilon(b_+ b_- + b_+* b_-*) +u(|b_+|4 +|b_-|4) + w |b_+|2|b_-|2$ for two complex envelopes $b_\pm(t)$. The results have been compared to parametric instabilities of vortex ring in condensate with density $\rho(z,r)=1-r2-\alpha z2$, which take place at $\alpha\approx 8/5$ and at $\alpha\approx 16/7$.

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