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Using steady state rate equations, closed form solutions for carrier density in the active layer is deduced.

利用稳态速率方程, 导出了激光器有源区载流子密度与偏置电流及输入信号光功率关系的隐函数表达式.

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Offset currents generated within picoammeters, electrometers, and SMUs are included in the instrument's specifications.

皮安计 、 静电计和SMU中产生的偏置电流在仪器的技术指标中给出.

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Offset currents can also be generated externally from such sources as triboelectric and piezoelectric effects.

这种偏置电流也可以由摩擦电效应和压电效应等原因在外部产生.

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Electrometers are known for their low input bias current, which is usually a few femtoamps.

静电计以低输入偏置电流而闻名,其输入偏置电流通常在几个飞安(fA).

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GMI ratio profile shows symmetric two peaks for f > 100 kHz at zero DC bias current.

直流偏置电流改变了非晶带横向磁导率,造成阻抗变化的不对称.

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Using steady - state rate equations, closed form solutions for carrier density in the active layer is deduced.

利用稳态速率方程, 导出了激光器有源区载流子密度与偏置电流及输入信号光功率关系的隐函数表达式.

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However, also consider amplifier noise, input bias current, offset voltage, MDAC resolution, and glitch energy.

然而, 也要考虑放大器的噪声 、 输入偏置电流 、 偏置电压 、 MDAC分辨率 和毛刺能量等因素.

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External offset currents can be generated by ionic contamination in the insulators connected to the ammeter.

外部偏置电流可以由与安培计相连的绝缘体上的离子沾污产生.

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The card chosen must have wide bandwidth as well as good isolation and low offset current.

所选的开关卡必须具有宽带宽,以及良好的隔离和低偏置电流.

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