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Film thickness-dependent ferroelectric polarization switching dynamics of undoped HfO2 thin films prepared by atomic layer deposition

机译:通过原子层沉积制备的未掺杂HFO2薄膜的膜厚度依赖性铁电偏振切换动力学

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摘要

Metal-ferroelectric-metal capacitors were fabricated to evaluate the ferroelectricity and switching dynamics of the undoped-HfO2 thin films prepared by atomic layer deposition. The film thickness was controlled to be 9 to 16 nm as an important control parameter. The value of remnant polarization (P-r) decreased with increasing the film thickness owing to the modulations in amounts of ferroelectric orthorhombic phase. The 11-nm-thick HfO(2 )thin film, which was strategically suggested as a critical film thickness, showed the P-r value of 8.47 mu C/cm(2). Based on the accurately calculated P-r by double-pulse switching measurement and Kolmogorov-Avrami-Ishibashi (KAI) model, the ferroelectric polarization switching time (t(s)) and the activation electric field (BO for polarization reversal were estimated with the variations in film thickness of the HfO2 thin films. The t(s) and E-a showed decreasing and increasing trends with increasing the film thickness, respectively. The values of P-r for the MFN capacitor were also found to be gradually modulated by controlling the ferroelectric partial polarization with pulse-width and pulse-number modulations, which corresponded to the emulations of assigning the synaptic weights for the synapse device applications.
机译:制造金属铁电金属电容器以评估通过原子层沉积制备的未掺杂-HFO2薄膜的铁电性和切换动力学。将膜厚度控制为9至16nm,作为重要的控制参数。随着膜厚度的增加,由于铁电正式正常相量的调节,随着铁电正性阶段的调节,随着铁电正性阶段的调节,残余极化(P-R)的值降低。将11-NM厚的HFO(2)薄膜作为临界膜厚度策略性地表明,显示为8.47μc/ cm(2)的p-r值。基于双脉冲切换测量和Kolmogorov-Avrami-ishibashi(kai)模型的准确计算的PR,通过变化估计铁电偏振切换时间(T(s))和激活电场(用于偏振反转的波动HFO2薄膜的膜厚度。T(s)和EA分别表现出降低和增加膜厚度的趋势。还发现了通过控制铁电局部极化来逐渐调节PR的PR值。脉冲宽度和脉冲数调制,其对应于分配Synapse设备应用程序的突触权重的仿真。

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