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Tunable band-gap structure and gap solitons in the generalized Gross-Pitaevskii equation with a periodic potential

机译:具有周期势的广义Gross-Pitaevskii方程中的可调谐带隙结构和带隙孤子

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摘要

The tunable band-gap structure is fundamentally important in the dynamics of both linear and nonlinear modes trapped in a lattice because Bloch modes can only exist in the bands of the periodic system and nonlinear modes associating with them are usually confined to the gaps. We reveal that when a momentum operator is introduced into the Gross-Pitaevskii equation (GPE), the bandgap spectra of the periodic system can be shifted upward parabolically by the growth of the constant momentum coefficient. During this process, the band edges become asymmetric, in sharp contrast to the standard GPE with an external periodic potential. Extended complex Bloch modes with asymmetric profiles can be derived by applying a phase transformation to the symmetric profiles. We find that the inherent parity-time symmetry of the complex system is never broken with increasing momentum coefficient. Under repulsive interactions, solitons with different numbers of peaks bifurcating from the band edges are found in finite gaps. We also address the existence of embedded solitons in the generalized two-dimensional GPE. Linear stability analysis corroborated by direct evolution simulations demonstrates that multi-peaked solitons are almost completely stable in their entire existence domains.
机译:带隙结构在陷于晶格中的线性和非线性模态的动力学中至关重要,因为Bloch模只能存在于周期系统的带中,并且与它们相关的非线性模通常被限制在间隙中。我们揭示出,当将动量算符引入Gross-Pitaevskii方程(GPE)时,周期系统的带隙谱可以通过恒定动量系数的增长而抛物向上移动。在此过程中,与具有外部周期性电势的标准GPE形成鲜明对比的是,带边缘变得不对称。通过将相位变换应用于对称轮廓,可以导出具有非对称轮廓的扩展复杂Bloch模式。我们发现,随着动量系数的增加,复杂系统固有的奇偶时间对称性永远不会被破坏。在排斥相互作用下,在有限的间隙中发现了从带边缘分叉的具有不同数量峰的孤子。我们还解决了广义二维GPE中嵌入式孤子的存在。直接进化模拟证实的线性稳定性分析表明,多峰孤子在其整个存在域中几乎完全稳定。

著录项

  • 期刊名称 Scientific Reports
  • 作者

    Changming Huang; Liangwei Dong;

  • 作者单位
  • 年(卷),期 -1(8),-1
  • 年度 -1
  • 页码 1374
  • 总页数 10
  • 原文格式 PDF
  • 正文语种
  • 中图分类
  • 关键词

  • 入库时间 2022-08-21 10:58:05

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