“…Note in (1) that, if using the definition coth P = (ep + e-')/(ePe-'), the Gummel integral P ( N s ) can be shown to be a function of X , [5], Further, under the transparent emitter condition: P(N,) < 1 or W < L&), needed for an interpretation of measured values of &O,h(e) [2 to 41, (1) can be approximated by In addition, as developed in I, the above expressions (1) and (3) have been obtained, based on the two following assumptions:…”