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SYMMETRY-BREAKING BIFURCATION IN NONLINEAR SCHRODINGER/GROSS-PITAEVSKII EQUATIONS

机译:非线性schrodinding / GROss-pITaEVsKII方程中的对称破裂分岔

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摘要

We consider a class of nonlinear Schrödinger/Gross–Pitaeveskii (NLS-GP) equations, i.e., NLS with a linear potential. NLS-GP plays an important role in the mathematical modeling of nonlinear optical as well as macroscopic quantum phenomena (BEC). We obtain conditions for a symmetry-breaking bifurcation in a symmetric family of states as ${\cal N}$, the squared $L^2$ norm (particle number, optical power), is increased. The bifurcating asymmetric state is a “mixed mode” which, near the bifurcation point, is approximately a superposition of symmetric and antisymmetric modes. In the special case where the linear potential is a double well with well-separation $L$, we estimate ${\cal N}_{cr}(L)$, the symmetry breaking threshold. Along the “lowest energy” symmetric branch, there is an exchange of stability from the symmetric to the asymmetric branch as ${\cal N}$ is increased beyond ${\cal N}_{cr}$.
机译:我们考虑一类非线性Schrödinger/ Gross-Pitaeveskii(NLS-GP)方程,即具有线性势的NLS。 NLS-GP在非线性光学和宏观量子现象(BEC)的数学建模中起着重要作用。我们获得了对称状态族中对称破缺分叉的条件,其中$ {\ cal N} $,平方L ^ 2 $范数(粒子数,光焦度)的平方增加了。分叉的不对称状态是“混合模式”,其在分叉点附近近似为对称和反对称模式的叠加。在线性势是具有良好分离$ L $的双阱的特殊情况下,我们估计对称破坏阈值$ {\ cal N} _ {cr}(L)$。沿着“最低能量”对称分支,当$ {\ cal N} $增加超过$ {\ cal N} _ {cr} $时,从对称分支到非对称分支之间存在稳定性交换。

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