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Analytical Approximations for the Special Elliptic Functions of Standard Fowler-Nordheim Theory

机译:标准Fowler-Nordheim理论特殊椭圆函数的分析近似

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The Standard Fowler-Nordheim (Curve) Equation, as derived from the work of Murphy and Good, may be written in the form J = t{sub}F{sup}(-2)aΦ{sup}(-1) exp{-v{sub}FbΦ{sup}(3/2)/F}, where F is the barrier field, Φ is the local work-function, a and b are the First and Second Fowler-Nordheim Constants, and v{sub}F and t{sub}F are the values, taken for a "forwards-moving state at the Fermi level", of the special elliptic functions v and t. These functions have purely mathematical definitions, and depend only on a single mathematical variable, usually denoted by y. In their application to field electron emission theory, y is termed the Nordheim parameter, and is given by y = (e{sup}3/4πε{sub}0){sup}(1/2)F{sup}(1/2)/Φ,where e is the elementary positive charge and ε{sub}0 is the electric constant.
机译:从墨菲和良好的工作中得出的标准fowler-nordheim(曲线)方程可以用形式j = t {sub} f {sup}( - 2)aφ{sup}( - 1)exp { -v {sub}fbφ{sup}(3/2)/ f},其中f是屏障字段,φ是本地工作函数,a和b是第一和第二fowler-nordheim常数,并且v {sub f和t {sub} f是特殊椭圆函数v和t的“FERMI级别”的“前向移动状态”的值。这些函数具有纯粹的数学定义,并且只依赖于单个数学变量,通常由y表示。在他们对现场电子发射理论的应用中,Y被称为Nordheim参数,并且由Y =(e {sup} 3 /4πε{sub} 0)给出){sup}(1/2)f {sup}(1 / 2)/φ,其中e是基本电荷,ε{sub} 0是电常数。

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