低温下熔淬 Ge2Sb2Te5 相变存储器线路电池的电阻漂移

A. Talukder, Md Tashfiq Bin Kashem, R. Khan, F. Dirisaglik, A. Gokirmak, H. Silva
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引用次数: 0

摘要

我们通过对 20 nm 厚、〜70 - 100 nm 宽的侧向 Ge2Sb2Te5 (GST) 线路电池进行测量,确定了相变存储器件在 80 K 至 300 K 温度范围内的电阻漂移特性。使用持续时间为 ~50 - 100 ns 的 1.5 - 2.5 V 脉冲对电池进行非晶化,从而产生 ~0.4 - 1.1 mA 的峰值复位电流,导致非晶化长度介于 ~50 - 700 nm 之间。非晶化电池中的电阻漂移系数是通过在非晶化后一秒内开始并持续 1 小时的恒压测量计算得出的。漂移系数介于 ~0.02 和 0.1 之间,在测量期间器件与器件之间存在显著的差异和变化。在较低的温度下(较高的电阻状态),一些器件显示出复杂的动态行为,电阻在几秒钟的时间内反复大幅增加和减少。这些结果表明,电荷捕获和去捕获事件是造成电阻漂移的原因。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Resistance Drift in Melt-Quenched Ge2Sb2Te5 Phase Change Memory Line Cells at Cryogenic Temperatures
We characterized resistance drift in phase change memory devices in the 80 K to 300 K temperature range by performing measurements on 20 nm thick, ~70 – 100 nm wide lateral Ge2Sb2Te5 (GST) line cells. The cells were amorphized using 1.5 – 2.5 V pulses with ~50 – 100 ns duration leading to ~0.4 – 1.1 mA peak reset currents resulting in amorphized lengths between ~50 and 700 nm. Resistance drift coefficients in the amorphized cells are calculated using constant voltage measurements starting as fast as within a second after amorphization and for 1 hour duration. Drift coefficients range between ~0.02 and 0.1 with significant device-to-device variability and variations during the measurement period. At lower temperatures (higher resistance states) some devices show a complex dynamic behavior, with the resistance repeatedly increasing and decreasing significantly over periods in the order of seconds. These results point to charge trapping and de-trapping events as the cause of resistance drift.
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