首页> 外文期刊>Physical Review, B. Condensed Matter >Ballistic-electron-emission-microscopy studies on Au/SiO2 n-type Si(100) and Ir/SiO2 n-type Si(100) structures with very thin oxides
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Ballistic-electron-emission-microscopy studies on Au/SiO2 n-type Si(100) and Ir/SiO2 n-type Si(100) structures with very thin oxides

机译:含极薄氧化物的Au / SiO2 n型Si(100)和Ir / SiO2 n型Si(100)结构的弹道电子发射显微镜研究

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摘要

Ballistic electron emission microscopy (BEEM) has been used to study metal-oxide-semiconductor (MOS) structures such as Au/SiO2-type Si(100) and Ir/SiO2-type Si(100), with the thin SiO2 layer varying from 10 to 30 Angstrom. As expected, the presence of a 30-Angstrom oxide layer at the interface induces much higher electronic barriers than in the case of Schottky diodes. Samples with Au show a barrier height of similar to 4.1 eV, while those with Ir have a barrier as high as 5.6 eV. When the interface oxide-layer thickness is reduced to similar to 10 Angstrom, the BEEM spectra behavior is different. For Au/SiO2/Si junctions, although a clear threshold is always observed around 4 eV, showing that a high barrier is already formed at these small thicknesses, a leakage current is often detected below this threshold. In the case of Ir/SiO2/Si structures, the BEEM spectra display an anomalous behavior. Below the high-energy threshold around 5.5-6 eV, a first threshold (similar to 1.5 eV) and a broad peak (similar to 4 eV) are observed. These structures could result from a resonant tunneling effect through the oxide layer. A striking result is also observed in the reverse BEEM (RBEEM) mode. In contrast to what is normally observed, where the RBEEM current is much weaker than the BEEM current, for these ultrathin barriers we find a broad peak at 4 eV with approximately the same intensity in RBEEM as in BEEM. [References: 26]
机译:弹道电子发射显微镜(BEEM)已用于研究金属氧化物半导体(MOS)结构,例如Au / SiO2 / n型Si(100)和Ir / SiO2 / n型Si(100), SiO2层在10到30埃之间变化。如所预期的,与肖特基二极管的情况相比,界面处存在30的氧化层会引起更高的电子势垒。 Au样品的势垒高度接近4.1 eV,而Ir样品的势垒高度高达5.6 eV。当界面氧化物层的厚度减小到类似于10埃时,BEEM光谱行为就不同了。对于Au / SiO2 / Si结,尽管始终在4 eV附近观察到清晰的阈值,表明在这些较小的厚度处已经形成了高势垒,但通常会在此阈值以下检测到泄漏电流。在Ir / SiO2 / Si结构的情况下,BEEM光谱显示出异常行为。低于5.5-6 eV的高能量阈值时,观察到一个第一阈值(类似于1.5 eV)和一个宽峰(类似于4 eV)。这些结构可能是由于穿过氧化物层的共振隧穿效应引起的。在反向BEEM(RBEEM)模式下也观察到惊人的结果。与通常观察到的情况相反,RBEEM电流比BEEM电流弱得多,对于这些超薄势垒,我们在4 eV处发现了一个宽峰,RBEEM中的强度与BEEM中的强度大致相同。 [参考:26]

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