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BOUNDARY DRIVEN WAVEGUIDE ARRAYS: SUPRATRANSMISSION AND SADDLE-NODE BIFURCATION

机译:边界驱动的波导管阵列:超透射和鞍形节点分叉

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In this paper, we consider a semi-infinite discrete nonlinear Schrodinger equation driven at one edge by a driving force. The equation models the dynamics of coupled waveguide arrays. When the frequency of the forcing is in the allowed band of the system, there will be a linear transmission of energy through the lattice. Yet, if the frequency is in the upper forbidden band, then there is a critical driving amplitude for a nonlinear tunneling, which is called supratransmission, of energy to occur. Here, we discuss mathematically the mechanism and the source of the supratransmission. By analyzing the existence and the stability of the rapidly decaying static discrete solitons of the system, we show rigorously that two of the static solitons emerge and disappear in a saddle-node bifurcation at a critical driving amplitude. One of the emerging solitons is always stable in its existence region and the other is always unstable. We argue that the critical amplitude for supratransmission is then the same as the critical driving amplitude of the saddle-node bifurcation. We consider as well the case of the forcing frequency in the lower forbidden band. It is discussed briefly that there is no supratransmission because in this case there is only one rapidly decaying static soliton that exists and is stable for any driving amplitude.
机译:在本文中,我们考虑了由驱动力在一个边缘驱动的半无限离散非线性Schrodinger方程。该方程对耦合的波导阵列的动力学建模。当强迫的频率在系统的允许范围内时,能量将通过晶格进行线性传输。但是,如果频率在禁止的上限频带内,则对于发生能量的非线性隧穿(称为超传输),存在临界驱动振幅。在这里,我们在数学上讨论超传输的机制和来源。通过分析系统中快速衰减的静态离散孤子的存在和稳定性,我们严格表明,在临界驱动振幅下,两个静态孤子会在鞍形节点分叉中出现和消失。一个新兴的孤子在其存在区域中始终稳定,而另一个则始终不稳定。我们认为超传输的临界振幅与鞍形节点分叉的临界驱动振幅相同。我们还要考虑在较低的禁带中强迫频率的情况。简要讨论了不存在超传输,因为在这种情况下,仅存在一个快速衰减的静态孤子,并且对于任何驱动振幅都是稳定的。

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