Abstract

The positive ionization efficiency of alkali halide (MX) incident upon Mo or Ta heated in a high vacuum (∼ 0.2 μTorr) always attained an appreciable value (∼ 0.01) at the appearance temperature ( T 0) and then steeply increased up to unity at the saturation temperature ( T 1). The data on the threshold temperature range ( T 0– T 1) were analyzed to find the quantitative relation between each boundary temperature and the main factors governing it, thereby yielding the empirical formulae of T 0 = (D 0 + I 0 − φ 0 +) R 0k and T 1 = (D 1 + I 1 − φ 1 +) R 1k . Here, D, I and φ + are the dissociation energy of MX, the ionization energy of M and the effective work function for the ionization on each surface, respectively, in eV at T 0 or T 1 in K, and k is Boltzmann's constant. The empirical constants ( R 0 = 42.1 ± 1.0 and R 1 = 28.2 ± 1.1) thus determined are essentially equal to our previous values (41.7 ± 2.2 and 29.1 ± 1.4 for MX/Re and 41.5 ± 2.0 and 28.7 ± 1.1 for MX/W) and also present ones (39.5 ± 2.9 and 27.8 ± 1.1 for TlX/Re, InI/W, etc.) determined in high vacua (∼ 0.2–20 μTorr). These results indicate that our empirical formulae expressing the range are generally applicable to any diatomic halide molecule/metal surface system and also that the most probable values of R 0 and R 1 are 41.3 ± 2.2 and 28.4 ± 1.3, respectively.

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