1971
DOI: 10.1109/proc.1971.8459
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Current status of negative electron affinity devices

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1978
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Cited by 64 publications
(8 citation statements)
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“…An early observation by Goldstein suggests that amorphous overlayers of CsO are not sufficient to induce (effective) NEA on Si – crystalline layers are required. The surface dipole of the silicon itself is not altered but the overlayer possesses a strong dipole moment of its own . Intuitively, one expects that in the case of diamond it will be much harder to produce a crystalline overlayer of Cs due to the very large difference between the atomic size of Cs and C/O.…”
Section: Brief Review Of Alternative Approaches To Neamentioning
confidence: 99%
“…An early observation by Goldstein suggests that amorphous overlayers of CsO are not sufficient to induce (effective) NEA on Si – crystalline layers are required. The surface dipole of the silicon itself is not altered but the overlayer possesses a strong dipole moment of its own . Intuitively, one expects that in the case of diamond it will be much harder to produce a crystalline overlayer of Cs due to the very large difference between the atomic size of Cs and C/O.…”
Section: Brief Review Of Alternative Approaches To Neamentioning
confidence: 99%
“…The reactant gases were mixed immediately before flowing into the reaction chamber. 3 Iron, chromium, and sulfur-doped InP substrates were obtained4 in the form of rough sawn wafers, which were <100> oriented. These wafers were polished by mechanical lapping with successively finer grits, the final polishing being done with 0.06 #m alumina.…”
Section: Substrate Etchingmentioning
confidence: 99%
“…One of the most fundamental and technologically relevant phenomena in light-matter interaction is the demonstration of the photoelectric effect, where photons have been used to emit electrons in free space. Efficient electron emission from various types of materials has enabled technologies for many cutting-edge applications such as free-electron lasers, image intensifiers for night imaging, sources for next-generation electron-beam lithography, electron microscopy, and photomultipliers; it has also led to the elucidation of novel materials physics probed through the investigation of the spin, momentum, and energy of the emitted electron [14][15][16][17] . State-of-the-art electron sources (or photocathodes) are classified into three families depending on the active material type: metals (Cu, Mg, Pb), alkali antimonide and tellurides (Cs 2 Te, K 2 CsSb, Cs 3 Sb), and III-V semiconductors (GaAs, GaN, tertiary alloys of III-V materials) 18 .…”
mentioning
confidence: 99%