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Mean work functions effective for negative-ionic, electronic and positive-ionic emissions from polycrystalline surfaces

机译:平均功函数对多晶表面的负离子,电子和正离子发射有效

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To elucidate the thermionic property of polycrystalline surfaces, a further study is made on the mean work functions (phi(-), phi(e) and phi(+)) effective for negative-ionic, electronic and positive-ionic emissions. Comparison between theoretical analyses and experimental data yields the conclusions as follows. (1) The equation of phi(-) = phi(e) holds always with both mono- and polycrystalline surfaces. (2) The relation of phi(-) = phi(e) < phi(+) applies to polycrystalline surfaces because they bear the thermionic contrast (Delta phi* phi(+) - phi(e) > 0). (3) The value of Delta phi* ranges from similar to 0.4 to 0.9 eV depending upon the surface species of polycrystalline metals (e.g., W, Re and Pt), whilst Delta phi* = 0 for monocrystalline surfaces. (4) When the degree of mono-crystallization (delta(m)) is less than similar to 50%, the theoretical value of Delta phi* is virtually independent of 3 and agrees well with experimental data, nearly the same within +/- 0.1 eV among the so-called "polycrystalline" surfaces of W. (5) As delta(m). increases beyond similar to 80 up to 100%, Delta phi* decreases rapidly down to 0 cV, showing again a good agreement between theory and experiment. (6) Our theoretical model is valid in evaluating the effective mean work functions, irrespective of the range of delta(m). (c) 2005 Elsevier B.V. All rights reserved.
机译:为了阐明多晶表面的热电子性质,对有效用于负离子,电子和正离子发射的平均功函数(phi(-),phi(e)和phi(+))进行了进一步研究。理论分析和实验数据之间的比较得出以下结论。 (1)方程phi(-)= phi(e)始终适用于单晶和多晶表面。 (2)phi(-)= phi(e)hi(+)的关系适用于多晶表面,因为它们具有热电子对比度(Delta phi * phi(+)-phi(e)> 0)。 (3)取决于多晶金属的表面种类(例如,W,Re和Pt),Delta phi *的值在约0.4至0.9eV的范围内,而对于单晶表面,Delta phi * = 0。 (4)当单晶度(delta(m))小于50%时,δphi *的理论值实际上与3无关,并且与实验数据吻合良好,+ /-范围内几乎相同W的所谓“多晶”表面之间为0.1 eV。(5)As delta(m)。如果增加超过80%直至100%,Delta phi *会迅速下降至0 cV,这再次表明理论与实验之间的良好一致性。 (6)我们的理论模型对于评估有效平均功函数是有效的,而与delta(m)的范围无关。 (c)2005 Elsevier B.V.保留所有权利。

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