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of diamond, 0 is the permittivity of free space, and S is the electrode area. According to Equation (15.1), we estimated Ni as 2.5 1016 cm 3 from the reciprocal slope of the 1/C 2 V characteristics at the reverse bias voltage, as shown by the tting line in Figure 15.5(b). Also qV bi was estimated as 4.7 eV from the extrapolation of the tting line to zero. The estimated value of Ni is almost identical to the boron concentration of 2 5 1016 cm 3 , and is two orders of magnitude lower than the phosphorus concentration of 2 5 1018 cm 3 . Therefore, the Ni of the p n junction diode corresponds to the boron acceptor density in the p-type layer. These results indicate that the space charge layer extends practically to the p-type layer side. The estimated qV bi is in good agreement with the expected qV bi of about 4.3 eV, which was obtained with the simple equation qV bi = Eg EA ED at 500 C, where Eg is the energy gap of diamond. As shown in Figure 15.5(b), the 1/C 2 V characteristics have a peak at the forward bias voltage near the zero current. This peak showed a strong frequency dependence. These characteristics indicate the existence of electrically active deep levels except for the boron acceptors and phosphorus donors in the vicinity of the p n junction. The relatively high leakage current of I V characteristics as shown in Figure 15.4 would be affected by these deep levels. qr code generator java 1.4 Write a QR Code Reader in Java using Zxing | CalliCoder
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