Here we present a novel method to stabilize solitons in 2D by making
the interatomic interaction oscillate rapidly using Feshbach
resonance.
The stabilization mechanism is similar to those of the inverted
pendulum (Kapitza pendulum) with an oscillating pivot, alternating-gradient focusing, and
the Paul trap.
(WMV, 407KB)
The system considered here is a BEC confined in the quasi-2D trap.
We assume that the interaction is rapidly oscillated as g = g0 + g1
sin(wt) using the Feshbach resonance.
The interaction is adiabatically switched on and simultaneously the
radial trapping potential is turned off from t = 0 to t = 20.
Soliton stabilization
(WMV, 112KB)
(GIF, 307KB)
In this movie, the right panel shows a noninteracting case for
comparison.
When the adiabaticity of the ramp of the interaction and the radial
trapping potential is break down, the lowest breathing mode is
excited in the soliton.
The frequency of the breathing oscillation is much smaller than that
of the oscillating interaction.
Breathing-mode excitation
(WMV, 95KB)
(GIF, 200KB)
In order to examine the interaction between solitons, we place two
solitons prepared by the above method.
When the relative phase between the solitons is pi, they repel each
other.
Repulsive interactions between solitons
(WMV, 77KB)
(GIF, 373KB)
Here weak radial trapping potential is present and the two solitons
oscillate.
On the other hand, when two solitons have the same phase, they merge
into one condensate.
Attractive interactions between solitons
(WMV, 77KB)
(GIF, 342KB)
The repulsive interaction between solitons implies that possibility of
soliton "lattice" formation.
We then examine stabilities of four solitons, where the relative phase
between adjacent solitons is taken to be pi.
Instability of "soliton lattice"
(WMV, 426KB)
(GIF, 698KB)
We found that the soliton lattice is dynamically unstable.
However, if we insert a potential barrier at the center of the four
solitons, they become stable.
Stability of "soliton lattice"
(WMV, 78KB)
(GIF, 698KB)
Thus, the soliton lattice may be formed if we put optical plugs
between diagonal solitons.