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0009277746
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note
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EBIC detects the presence of an internal electric field in a sample. Because a concentration gradient of an electrically active impurity (dopant) creates an internal electric field, an EBIC signal indicates the presence of such a gradient (for example, between p-and n-type regions). If the gradient is abrupt, then the field is localized within a thin layer and shows up as a line (fig. 1b). If the gradient is smeared out (gradual change between p and n regions) the EBIC signal appears as black or white areas (fig. 3b). The contrast on the picture (black or white) will depend on the direction of the internal electric field with respect to the electrode used to collect the EBICurrent (toward or away from the working electrode). In fig. 1b the working electrode is at the right and the grounded one at the left. In figs. 3 the working electrode is at the top and the grounded one at the bottom. The p-n junction region shows up white and the n-p one black.
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7
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0000157330
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samples were kept in closed containers, that blocked all visible and near-infrared radiation. The power of the electron beam used to perform EBIC was negligible (30 kV × 10 nA = 0.3 mW) compared to what would be needed to induce any changes in the sample
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To avoid photo-segregation, (TREGILGAS J. and GNADE B., J. Vac. Sci. Technol. A, 3 (1985) 156) samples were kept in closed containers, that blocked all visible and near-infrared radiation. The power of the electron beam used to perform EBIC was negligible (30 kV × 10 nA = 0.3 mW) compared to what would be needed to induce any changes in the sample (BARBOT J. F., KRONEWITZ J. and SCHROTER W., Appl. Phys. Lett., 57 (1990) 2689).
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To avoid photo-segregation, (TREGILGAS J. and GNADE B., J. Vac. Sci. Technol. A, 3 (1985) 156) samples were kept in closed containers, that blocked all visible and near-infrared radiation. The power of the electron beam used to perform EBIC was negligible (30 kV × 10 nA = 0.3 mW) compared to what would be needed to induce any changes in the sample (BARBOT J. F., KRONEWITZ J. and SCHROTER W., Appl. Phys. Lett., 57 (1990) 2689).
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edited by M. O'KEEFE and A. NAVROTSKY (Academic, New York)
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SHANNON R. D., in Structure and Bonding in Crystals, edited by M. O'KEEFE and A. NAVROTSKY (Academic, New York) 1981, p. 53.
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GORSHKOV A. V., ZAITOV F. A., SHANGIN S. B. and SHALYAPINA G. M., Sov. Phys. Solid State, 26 (1984) 1787.
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0004091247
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Wiley, New York, Chapt. 26.5
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0, the electrostatic interaction is comparable with the thermal energy. Cf., for example, BERRY R. S., RICE S. A. and ROSS J., Physical Chemistry (Wiley, New York) 1980, Chapt. 26.5.
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