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Estimation of Copper, Silver and Gold Coverages on the Iridium Field Emitter Tip Surface
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作者 Khalil Ismaiel Hashim 《World Journal of Engineering and Technology》 2018年第3期556-566,共11页
The work described in this paper is a study of the estimation of copper, silver and gold coverages on the iridium field emitter tip surface. The study has been carried out by using a simple field emission microscope d... The work described in this paper is a study of the estimation of copper, silver and gold coverages on the iridium field emitter tip surface. The study has been carried out by using a simple field emission microscope designed especially for the purpose of the adsorbate coverage calibration. It was equipped with an iridium field emitter tip. On one side of the microscope was the vapor source 12.5 cm from the tip, and on the other side 16.2 cm from the source was a quartz crystal oscillator. The crystal leads were spot welded to a two-pin tungsten-glass press-seal. In front of the crystal, a nickel shield was mounted in which there was a circular hole of an area of 0.0804 cm2, slightly smaller than the surface of the crystal, to prevent shorting of the conducting ends of the crystal which would be brought about by the condensed metal. The sensing crystal inside the microscope was driven by a small circuit placed just outside the microscope. The driving circuit was in turn connected to another circuit which comprised a frequency comparator unit which could read the frequency of the quartz crystal oscillator before and after the deposition of the adsorbate and gave a direct digital reading of ?(f is the resonance frequency of the crystal before the deposition of the adsorbate and Δf is the difference in the frequency of the oscillator after and before the deposition of the adsorbate on the crystal). The mass added to either side of the crystal alters its resonant frequency. The frequency shift obtained for a certain thickness of the deposited film depends on the density of the deposited film [1] [2]. 展开更多
关键词 field Emission MICROSCOPE Electron Work function ADSORBATE Coverage Calibration A Quartz Crystal Oscillator Resonant FREQUENCY fundamental FREQUENCY A FREQUENCY COMPARATOR unit Deposition MONOLAYER
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实二次代数函数域的单位群(英文)
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作者 王鲲鹏 张贤科 《中国科学院研究生院学报》 CAS CSCD 2003年第2期139-145,共7页
对于实二次代数函数域K,给出了求K的基本单位ε的一个方法。利用此方法,对于 4个系列(细分为 1 6类)的实二次代数函数域K。
关键词 二次代数函数域 基本单位 连分式
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实二次函数域基本单位的范
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作者 纪春岗 《数学杂志》 CSCD 1997年第2期173-178,共6页
作为H.F.Troter[3]中一个结果的模拟,本文给出实二次函数域K中基本单位ε的范为N(ε)=g的一些充分必要条件,其中g为K的常数域Fq的非零乘法群F*q的生成元(2q)。利用图论的语言,本文还给出了N(ε)=... 作为H.F.Troter[3]中一个结果的模拟,本文给出实二次函数域K中基本单位ε的范为N(ε)=g的一些充分必要条件,其中g为K的常数域Fq的非零乘法群F*q的生成元(2q)。利用图论的语言,本文还给出了N(ε)=g的一些充分条件,这些条件对于数域也同样地适用。 展开更多
关键词 函数域 基本单位 实二次函数域
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实二次函数域基本单位的范
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作者 纪春岗 《南京师大学报(自然科学版)》 CAS CSCD 1995年第4期7-12,共6页
研究了实二次函数域基本单位的范.给出了一些范等于g的充分必要条件,并利用图论的语言,给出了一些充分条件.
关键词 函数域 基本单位 实二次函数域
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函数域_q(T,((D^l+d))^(1/l))的基本单位
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作者 雍锡琪 《数学进展》 CSCD 北大核心 2000年第5期411-416,共6页
设 Fq(T)= k, q是凡的特征, J是奇素数,a‘d。,。 E IF:, d。,D是 F。[T]中首一多项式, M是 J-暴自由的,记的基本单位,我们有结果:其中e是J的P-adic表示中p的最高幂次数.
关键词 DIOPHANTINE方程 基本单位 函数域
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几个关于二次域基本单位的结果(英文)
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作者 姚钟磊 李江华 《大学数学》 2011年第6期35-41,共7页
给出了当m是二个或三个素数之积时,二次域OK中有范数为-1单位的证明.还给出了m是其他值时的情况.
关键词 二次域 范数为-1的基本单位
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