Download PDF by E. W. Müller (auth.), John J. Hren, S. Ranganathan (eds.): Field-Ion Microscopy

By E. W. Müller (auth.), John J. Hren, S. Ranganathan (eds.)

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Kubaschewski and E. LI. Evans, Metallurgical Thermochemislry, Pergarnon Press (London), 1958. 18. 0. Kubaschewski, Landolt-Bornstein, Tab/es li, 2(b) (1962), p. 2-1. 19. 0. Kubaschewski, Landolt-Bornstein, Tabfes li, 4 (1962), p. 837. 20. J. F. Mulson and E. W. Müller, J. Chem. Phys. 38:2615 (1963). 21. R. ), 1961, p. 45. 22. W. P. Dyke and W. W. Dolan. Adran. Electron. Electron Phvs. 8: 89 (1956). 23. M. Drechsler and P. Wolf, Proc. 4th Intern. Conf. Electron Microscopy, Berlin, 1958. Vol. I, p.

D. G. Brandon, Surface Science 5: 137 (1966). 14. S. Glasstone, K. J. Laidler, and H. Eyring, The Theory of Rate Processes, McGraw Hili (New York). 1941. 15. D. G. Brandon, Brit. J. Appl. Phys. 14: 474 ( 1963). 16. G. Ehrlich, Brit. J. App/. Phys. 15:349 (1964). 17. 0. Kubaschewski and E. LI. Evans, Metallurgical Thermochemislry, Pergarnon Press (London), 1958. 18. 0. Kubaschewski, Landolt-Bornstein, Tab/es li, 2(b) (1962), p. 2-1. 19. 0. Kubaschewski, Landolt-Bornstein, Tabfes li, 4 (1962), p.

0 ··' (VVOLTS) LOG 1• ... Fig. 1 0. The current-voltage characteristics of a tungsten emitter of about 630 A radius at various temperatures and at a helium pressure of 6 x 10- 3 torr. The upper Iimits of the curves for 63° and 77°K are at the evaporation voltages. At the remaining temperatures, current measurements were terminated weil below the evaporation voltages in order to avoid changes of emitter radius due to field evaporation. The dashed extrapolations for temperatures from 113 to 210°K are terminated at voltages corresponding to calculated evaporation fields.

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