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Dissipative Intrinsic Localized Modes in Nano-ferroelectrics

机译:纳米铁电体中的耗散本征局部模式

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Below Curie temperature, certain perovskites show important ferroelectric behaviour, which have a wide range of applications, notably in non-linear photonic devices and as non-volatile memory. Previously, a Klein-Gordon (KG) equation has been derived based on a discrete Hamiltonian. On a multiple time scale analysis (MTSA), based on discrete polarization domains, intrinsic localized modes (ILM) were observed [1], which are nonlinear excitations that are produced by the nonlinearity and discreteness of the lattice. These are highly localized pulses in space that are found in the discrete nonlinear model formulation. As the continuum limit formulation cannot be applied to their study, the present formulation is appropriate to highly localized pulses having widths that are not large compared to the domain widths. This question about the appropriate length scale drives us to nano-range of domain walls in ferroelectrics [2] having many interesting applications in nanostructured arrays of sensors, actuators, etc.
机译:在居里温度以下,某些钙钛矿表现出重要的铁电性能,具有广泛的应用,特别是在非线性光子器件中以及作为非易失性存储器。以前,已经基于离散哈密顿量导出了Klein-Gordon(KG)方程。在多时间尺度分析(MTSA)上,基于离散的极化域,观察到固有的局域模(ILM)[1],这是由晶格的非线性和离散产生的非线性激励。这些是空间中高度局部化的脉冲,可在离散非线性模型公式中找到。由于连续极限公式不能应用于他们的研究,因此本公式适用于宽度比畴宽不大的高度局部化的脉冲。关于合适的长度尺度的问题驱使我们进入铁电体中畴壁的纳米范围[2],在传感器,执行器等纳米结构阵列中有许多有趣的应用。

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