Diffuse reflectance technique for the measurement of forbidden energy gap, E g , is discussed. The energy coordinate of the point at which the linear increase in the Kubelka‐Munk function starts gives the E g ‐value. The E g ‐values of fifteen semiconductors are reported. These E g ‐values are found to be in good agreement with those measured by other methods.
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Tandon et al. (1970) studied this question.
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