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Microwave absorption and series resistance of silicon-mesa parametric-amplifier diodes

机译:硅台参量放大二极管的微波吸收和串联电阻

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The series resistance and capacitance of a silicon-mesa parametric diode are calculated in terms of parent resistivity, geometry and diffusion. These properties have been measured both at 2Gc/s, using slotted-line techniques, and at low frequencies. The capacitance of those diodes tested is in agreement with p-n-junction theory. The diode series resistance, however, has consistently shown an excess resistance of 1.5 to 2???????? when measured at 2Gc/s, this being about twice as great as the series ohmic resistance. A series of blank mesas without p-n junctions had the same resistance using d.c. as they had at 2Gc/s. This result localises the source of excess resistance to the p-n junction. This excess resistance is assumed to be the result of dielectric losses within the p-n junction, due to the strong microwave-frequency fields at the junction, which force ionised donor and acceptor atoms to oscillate about their equilibrium position. The ions transfer energy to the silicon lattice, and hence the energy absorption in the p-n junction appears as a lossy element; i.e. a resistance in series with the junction. A series of diodes made from 0.100????????cm silicon were tested to determine the effect of reducing the density of ions at the junction. These diodes had a series ohmic resistance in substantial agreement with their resistance at 2Gc/s. The losses within the p-n junction suggest a new equivalent circuit for parametric diodes. This circuit includes an absorption resistance in series with the diode capacitance. The absorption resistance may be reduced by outdiffusion prior to formation of the p-n junction, in order to form the junction in a region of low ion density. If successful, this approach would yield silicon-mesa diodes with cutoff frequencies in excess of 100Gc/s at zero bias, using present fabrication techniques.
机译:硅台面参数二极管的串联电阻和电容是根据母体电阻率,几何形状和扩散来计算的。这些特性已使用缝线技术在2Gc / s和低频下进行了测量。测试的那些二极管的电容与p-n结理论一致。然而,二极管串联电阻一直显示出1.5至2Ω的过量电阻。当以2Gc / s的速度进行测量时,约为串联欧姆电阻的两倍。使用dc,一系列没有p-n结的空白台面具有相同的电阻。就像他们在2Gc / s时一样。该结果将过量电阻的源定位到p-n结。假定该过大的电阻是p-n结内介电损耗的结果,这是由于该结处的微波频率场强,该电场迫使电离的施主原子和受主原子在其平衡位置附近振荡。离子将能量转移到硅晶格,因此p-n结中的能量吸收表现为有损耗元素;即与结串联的电阻。测试了一系列由0.100Ω·cm的硅制成的二极管,以确定降低结处离子密度的效果。这些二极管的串联欧姆电阻与2Gc / s的电阻基本一致。 p-n结内的损耗为参数二极管提出了新的等效电路。该电路包括与二极管电容串联的吸收电阻。为了在低离子密度的区域中形成结,可以在形成p-n结之前通过扩散来降低吸收电阻。如果成功的话,使用现有的制造技术,该方法将产生在零偏压下截止频率超过100Gc / s的硅-台面二极管。

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