Sakaguchi Hidetsugu, Malomed Boris A
Department of Applied Science for Electronics and Materials, Interdisciplinary Graduate School of Engineering Sciences, Kyushu University, Kasugu, Fukuoka 816-8580, Japan.
Phys Rev E Stat Nonlin Soft Matter Phys. 2005 Oct;72(4 Pt 2):046610. doi: 10.1103/PhysRevE.72.046610. Epub 2005 Oct 24.
We introduce a dynamical model of a Bose-Einstein condensate based on the one-dimensional (1D) Gross-Pitaevskii equation (GPE) with a nonlinear optical lattice (NOL), which is represented by the cubic term whose coefficient is periodically modulated in the coordinate. The model describes a situation when the atomic scattering length is spatially modulated, via the optically controlled Feshbach resonance, in an optical lattice created by interference of two laser beams. Relatively narrow solitons supported by the NOL are predicted by means of the variational approximation (VA), and an averaging method is applied to broad solitons. A different feature is a minimum norm (number of atoms), N = N(min), necessary for the existence of solitons. The VA predicts N(min) very accurately. Numerical results are chiefly presented for the NOL with the zero spatial average value of the nonlinearity coefficient. Solitons with values of the amplitude A larger than at N = N(min) are stable. Unstable solitons with smaller, but not too small, A rearrange themselves into persistent breathers. For still smaller A, the soliton slowly decays into radiation without forming a breather. Broad solitons with very small A are practically stable, as their decay is extremely slow. These broad solitons may freely move across the lattice, featuring quasielastic collisions. Narrow solitons, which are strongly pinned to the NOL, can easily form stable complexes. Finally, the weakly unstable low-amplitude solitons are stabilized if a cubic term with a constant coefficient, corresponding to weak attraction, is included in the GPE.
我们基于一维(1D)含非线性光学晶格(NOL)的格罗斯 - 皮塔耶夫斯基方程(GPE)引入了玻色 - 爱因斯坦凝聚体的动力学模型,该模型由坐标中系数呈周期性调制的三次项表示。该模型描述了一种情况,即通过光学控制的费什巴赫共振,在由两束激光干涉产生的光学晶格中,原子散射长度在空间上被调制。借助变分近似(VA)预测了由NOL支持的相对窄的孤子,并将平均方法应用于宽孤子。一个不同的特征是孤子存在所需的最小范数(原子数)(N = N_{min})。VA能非常准确地预测(N_{min})。主要给出了非线性系数空间平均值为零的NOL的数值结果。振幅(A)大于(N = N_{min})时的孤子是稳定的。振幅(A)较小但不太小的不稳定孤子会重新排列成持久的呼吸子。对于更小的(A),孤子会缓慢衰变为辐射而不形成呼吸子。振幅(A)非常小的宽孤子实际上是稳定的,因为它们的衰变极其缓慢。这些宽孤子可以自由穿过晶格,具有准弹性碰撞的特征。强烈钉扎在NOL上的窄孤子很容易形成稳定的复合体。最后,如果在GPE中包含一个对应于弱吸引的常数系数的三次项,弱不稳定的低振幅孤子会被稳定下来。