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Synopsis The Sternglass theory [Sternglass, Phys. Rev. 108, (1957) 1] for fast-ion-induced secondary electron emission, which is proportional to the stopping powers, has been modified to calculate the electron impact secondary electron yield from both elemental and compound targets with atomic number Z = 4 92 for incident energy range 5 10 5   i E eV. This modification includes the use of a realistic stopping power expression that involves calcula-

Electron impact secondary electron emissions from atomic and molecular solid targets