Charge storage and charge decay in silicon dioxide

P. Gunther, G. Sessler
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引用次数: 1

Abstract

SiO/sub 2/ layers with thicknesses between 150 nm and 2.5 mu m were either thermally grown or made by chemical vapour deposition on 2-inch p-type silicon wafers. Positive or negative charging of the samples was performed by liquid-contact, corona, and electron-beam methods. The decay of the surface potential was observed isothermally at room temperature and at 350 degrees C or by a thermally stimulated discharge (TSD) method at linearly increasing temperature. In the isothermal measurements, positively charged samples showed a somewhat faster decay than negatively charged ones. The decays can be interpreted with a simple theory based on carrier drift and compensation by conductivity. TSD peaks of negatively charged material occur at temperatures higher than those of positively charged samples. Activation energies of 1.0 and 1.4 eV for positively charged oxides and 1.9 eV for negatively charged oxides were found.<>
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二氧化硅中的电荷储存和电荷衰减
在2英寸p型硅片上热生长或化学气相沉积制备了厚度在150 nm ~ 2.5 μ m之间的SiO/sub 2/层。通过液体接触、电晕和电子束方法对样品进行正电荷或负电荷。在室温和350℃的等温条件下,或在线性升高的温度下,用热刺激放电(TSD)方法观察表面电位的衰减。在等温测量中,带正电的样品比带负电的样品衰减得快一些。衰减可以用一个基于载流子漂移和电导率补偿的简单理论来解释。负电荷材料的TSD峰出现在比正电荷样品更高的温度下。带正电的氧化物的活化能为1.0和1.4 eV,带负电的氧化物的活化能为1.9 eV。
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