2004
DOI: 10.1016/j.apsusc.2003.08.021
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Electronic resonances in the photofield emission spectra from Ta(1 1 1)

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Cited by 2 publications
(3 citation statements)
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“…By this means it is possible to change the thickness of the apex microcrystal and to observe the change of the maxima spacing. This anticipation has been proved and confirmed for the tantalum field emitter [19]. For the small tip radius r, otherwise for the great geometrical coefficient β (β ≈ 1/r), we observe four maxima (β = 9975 cm −1 ) and for the smaller β, after heating the tip at high temperature, we observe eight maxima (β = 5474 cm −1 ), see Fig.…”
Section: Discussionmentioning
confidence: 63%
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“…By this means it is possible to change the thickness of the apex microcrystal and to observe the change of the maxima spacing. This anticipation has been proved and confirmed for the tantalum field emitter [19]. For the small tip radius r, otherwise for the great geometrical coefficient β (β ≈ 1/r), we observe four maxima (β = 9975 cm −1 ) and for the smaller β, after heating the tip at high temperature, we observe eight maxima (β = 5474 cm −1 ), see Fig.…”
Section: Discussionmentioning
confidence: 63%
“…This means, that the grain boundary between the two microcrystals is displaced from the top of the tip, and the thickness of the emitting microcrystal is greater now. Moreover, it has appeared that polarization of the light beam does not change the apparent frequency of the photocurrent oscillations, and the general shapes of two curves reflect different band structures of bulk metal and that of the metal surface, but the small maxima remain practically unchanged [19].…”
Section: Discussionmentioning
confidence: 99%
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