闪存模式下p + n二极管SAW存储相关器的原理

M. Nokali
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引用次数: 1

摘要

摘要:介绍了工作在闪光模式下的间隙耦合表面声波二极管存储相关器的工作原理。回顾了用于分析存储过程和读出过程的电路模型。本文首次将少数载流子寿命和二极管电容电压依赖性的影响纳入闪存模式写入过程的分析中。提出了一种直接的传输线理论方法来求二极管电位在读出过程中激发的表面波幅度。该理论的计算预测与实验数据很好地吻合,并倾向于确认单次写入短脉冲保持高效存储的可能性。Gautier等人[1]将HE FLASH技术应用于p'n二极管SAW存储相关器,当使用具有较长少数载波寿命(60 p)的平面视屏阵列时,他们无法在一个写入短脉冲的二极管中存储任何信号。这一负面结果解释如下。用于给阵列充电的脉冲持续时间为5-10纳秒。由于少数载流子寿命长,从p岛注入到n侧的空穴不会重新组合,并且在脉冲关闭后,大量载流子将倾向于扩散回结。当时的普遍共识是,由于需要长时间充电,扩散二极管器件的使用仅限于窄带宽信号应用;也就是说,参数化技术应与扩散pn二极管结合使用。利用v型凹槽台面二极管结构,Borden和Kino[2]证明了p+n二极管可以用单个短脉冲充电,并且电荷存储时间为几毫秒。他们将他们的成功归功于这样一个事实,即在这种结构下,少数载流子寿命比其他小组使用的平面视屏阵列短几个数量级。然而,他们报告的存储时间的大幅度似乎与明显的事实相矛盾,即减少少数载流子寿命无疑会减少存储时间。Loh等人[3]评论了Borden和Kino的结果,得出结论,故意引入非对称而非对称的捕获电平是他们成功地用单个短脉冲给pfn二极管充电的原因
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Theory of the p + n Diode SAW Storage Correlator in the Flash Mode
Abstmct-The theory of the gap-coupled surface acoustic wave p'n diode storage correlator operated in the flash mode is presented. The circuit model used in the analysis of both the storage and the read-out processes is reviewed. The effect of the minority carrier lifetime and the voltage dependence of the diode capacitance are included for the first time in the analysis of the flash-mode writing process. A straightforward transmission line theory approach is developed to find the surface wave amplitude excited by the diode potential during the readout process. The calculated predictions of this theory are in good agreement with experimental data and tend to confirm the possibility of ohtaining efficient storage with a single write-in short pulse. HE FLASH technique was applied to the p'n diode SAW storage correlator by Gautier et al. [l], who were unable to store any signal in the diodes with one write-in short pulse when using a planar vidicon array with a long minority carrier lifetime (60 p). This negative result is explained as follows. The pulse used to charge the array has a duration of 5-10 ns. With a long minority carrier lifetime the holes injected from the p-island into the n-side do not recombine and a large number of these carriers will tend to diffuse back across the junction after the pulse is turned off. The general consensus then was that the use of diffused diode devices was limited to narrow bandwidth signal applications because of the long charging times required; i.e., that the parametric technique should be used in conjunction with diffused pn diodes. Using a V-groove mesa diode structure, Borden and Kino [2] demonstrated that p+n diodes can be charged with a single short pulse and that the charge is stored for milliseconds. They attributed their success to the fact that with such structures the minority carrier lifetime is several orders of magnitude shorter than the planar vidicon array used by other groups. However, the large magnitude of the storage time which they reported seems to contradict the obvious fact that a reduction in the minority carrier lifetime will undoubtedly reduce the storage time. Loh et al. [3], commenting on Borden and Kino's results, concluded that the deliberate introduction of asymmetric, rather than symmetric, trapping levels was responsible for their success in efficiently charging a pfn diode with a single short pulse since the presence of these
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