首页> 外文期刊>American Journal of Materials Science >On the Conduction Mechanism of Silicate Glass Doped by Oxide Compounds of Ruthenium (Thick Film Resistors). 2. Nanocrystals in the Glass and Charge Carrier's Localization
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On the Conduction Mechanism of Silicate Glass Doped by Oxide Compounds of Ruthenium (Thick Film Resistors). 2. Nanocrystals in the Glass and Charge Carrier's Localization

机译:钌的氧化物化合物(厚膜电阻器)掺杂硅酸盐玻璃的导电机理。 2.玻璃中的纳米晶体和电荷载体的定位

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Conduction mechanism of doped silicate glasses based on existence of nanocrystals is proposed. These nanocrystals are effective centers of localization of free charge carriers, and variable range hopping of last ones takes place. It is shown that dopant atoms generate narrow impurity subband of about 0,03 eV in width, which is slightly (less than 0.01 eV) separated from the top of the valence band of the glass or abutted on them, so thermal activation coexists with hopping conduction. Because of it the resistivity of the doped silicate glass is proportional to exp(-aT-ζ) at low temperatures (T < 50 K), 0.4 < ζ < 0.8. Structural transitions of nanocrystals take place at high temperatures (T > 800 K) and the conductivity of the doped silicate glass decreases sharply. Beyond the conductivity minimum (above 1000 K) the impurity subband and the top of the valence band of glass are separated by energy gap of 0.05 – 1.5 eV in width, so doped silicate glass behaves like a typical semiconductor.
机译:提出了基于纳米晶体存在的掺杂硅酸盐玻璃的导电机理。这些纳米晶体是自由电荷载流子的有效定位中心,并且发生了最后一个的可变范围跳跃。结果表明,掺杂剂原子产生的窄杂质子带宽度约为0,03 eV,与玻璃价带的顶部略微分开(小于0.01 eV)或邻接在其上,因此热活化与跳跃并存。传导。因此,在低温(T <50 K),0.4 <ζ<0.8的情况下,掺杂硅酸盐玻璃的电阻率与exp(-aT-ζ)成正比。纳米晶体的结构转变发生在高温下(T> 800 K),掺杂硅酸盐玻璃的电导率急剧下降。除了最小的电导率(高于1000 K)以外,玻璃的杂质子带和价带的顶部之间的能隙宽度为0.05 – 1.5 eV,因此掺杂的硅酸盐玻璃的行为类似于典型的半导体。

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