“…Substituting [2] and [3] into [1] dV = dQsc (1/Co + 1/Cs) = dQsc/Cm [4] where Cm is total measured capacitance, Cs = es/W, and W is space charge width. Using the relation dQsc = q N(W)dW in [4], where N(W) is the doping concentration as a function of W, we get dV = q N (W) dW/Cm [5] But, dW = "s d(1/Cs) = ,s d(1/Cm) [6] as 1/Cs = 1/Cm-1~Co. Substituting [6] into [5] and solving for N(W), we get N (W) = 2 (qes d(1/Cm2)/dV) -1 [7] This equation shows that the doping concentration N(W) can be calculated from the slope of the 1/C 2 vs. V curve.…”
“…Substituting [2] and [3] into [1] dV = dQsc (1/Co + 1/Cs) = dQsc/Cm [4] where Cm is total measured capacitance, Cs = es/W, and W is space charge width. Using the relation dQsc = q N(W)dW in [4], where N(W) is the doping concentration as a function of W, we get dV = q N (W) dW/Cm [5] But, dW = "s d(1/Cs) = ,s d(1/Cm) [6] as 1/Cs = 1/Cm-1~Co. Substituting [6] into [5] and solving for N(W), we get N (W) = 2 (qes d(1/Cm2)/dV) -1 [7] This equation shows that the doping concentration N(W) can be calculated from the slope of the 1/C 2 vs. V curve.…”
“…They are all based on clever use of the nonlinear circuit properties incorporated in Eq. [la] to [lc], as discussed originally by Meyer and Guldbrandsen (15). The authors also use an automated instrument designed and built some years ago by Rusche (16).…”
The capacitance of a Schottky barrier diode measured as a function of reverse voltage yields the dope concentration and eventually the thickness of an epitaxially grown silicon layer. It is shown that mercury can be used as the metal contact to the silicon. This allows for a rapid and nondestructive C‒V measurement, particularly when combined with an automated instrument. The results obtained with different surface treatments are discussed. For reliable and reproducible results N‐type silicon should be covered with a thin oxide layer about 50Aå thick, which can easily be made wet chemically. The precision which can be attained with this system in actual practice amounts to ±2% or better and the accuracy depends on the definition of thickness used. This technique with the mercury contacting accessory works equally well on
normalGaAs
and
normalGaP
“…The density of accumulated charges dependent on the active layer depth was calculated by the second-harmonic of the CV measurement at 500 Hz. [30][31][32] To determine if all trap states have been filled in a current-voltage measurement of a TFT, the TFL transition voltage (V tfl ) for a given material must be known. V tfl can be determined with capacitance/voltage (CV) measurements.…”
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