利用C-Si本征电阻率研究激光诱导光导与毫米波吸收的关系

B. Roy, A. Tsui, O. Oni, B. Vlahovic
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摘要

在非接触式光电导测量系统中,射频(RF)探针传输(ΔV/ V0)应通过灵敏度因子(a)与激光诱导载流子浓度和载流子迁移率(I·Σμ)的乘积成正比。我们使用532 nm激光(泵浦)-毫米波(mmw-探针)系统,其浓度(I·)是通过考虑激光束的单表面反射和从模型导出的迁移率(Σμ)来计算的。为了确定A,我们使用5个电阻率在15-130 Ω-cm范围内的c-Si(100)样品。为了将(ΔV/V0)与I·Σμ联系起来求A,我们取它们的比值,一次使用样品电阻率与空气电阻率之比(ρ/ρ0)的二次拟合函数形式量化A,另一次使用自由空间阻抗与样品厚度的乘积(ρ/Z0t)。确定了(ΔV/V0)-激光能量通量线性区A,能量通量在0 ~ 1.7 μJ/cm2范围内,探针频率固定在140 GHz。将A的值与0.85相乘进一步微调(使比率与无因次函数线性化),最终得到灵敏度A=0.291。两种方法之间毫米瓦光电导的标准误差(通过计算A获得)随着激光衰减大致以±0.53 × 10-5 S的速率减小,每十进制中性密度滤波器尺寸。
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Inter-Relation between Laser Induced Photoconductance and Millimeter Wave Absorption Using C-Si Intrinsic Resistivity
In a contactless photo conductance measurement system the radio-frequency (RF) probe transmission (ΔV/ V0) should be proportional to the product of laser-induced carrier concentration and carrier mobility (I•Σμ) through a sensitivity factor (A). We use 532 nm laser (pump)-millimeter wave (mmw-probe) system whose concentrations (I•) are calculated by considering single-surface reflection of the laser beam and mobility (Σμ) derived from a model. In order to ascertain A we use five c-Si (100) samples having resistivity in the range 15-130 Ω-cm. For relating (ΔV/V0) with I•Σμ to find A, we take their ratio and quantify A once using a quadratic-fit functional form of the ratio of sample resistivity to air resistivity (ρ/ρ0), and another time using product of free-space impedance and sample thickness (ρ/Z0t). A is ascertained for (ΔV/V0)-laser fluence linear region while fluence is in range 0-1.7 μJ/cm2 and probe frequency is fixed at 140 GHz. Value of A is further fine-tuned by multiplying with 0.85 (to linearize the ratio with the non-dimensional function) and finally obtain sensitivity A=0.291. Standard error in mmw photo conductance (obtained using calculated A) between the two approaches diminish with laser attenuation roughly at a rate ± 0.53 × 10-5 S, per decimal neutral density filter size.
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