Complex structures on a material surface can significantly reduce totalsecondary electron emission from that surface. A velvet is a surface thatconsists of an array of vertically standing whiskers. The reduction occurs dueto the capture of low-energy, true secondary electrons emitted at the bottom ofthe structure and on the sides of the velvet whiskers. We performed numericalsimulations and developed an approximate analytical model that calculates thenet secondary electron emission yield from a velvet surface as a function ofthe velvet whisker length and packing density, and the angle of incidence ofprimary electrons. We found that to suppress secondary electrons, the followingcondition on dimensionless parameters must be met: {\pi}/2 DA tan {\theta} >> 1where {\theta} is the angle of incidence of the primary electron from thenormal, D is the fraction of surface area taken up by the velvet whisker bases,and A is the aspect ratio, A {\equiv} h/r, the ratio of height to radius of thevelvet whiskers. We find that velvets available today can reduce the secondaryelectron yield by 90% from the value of a flat surface. The values of optimalvelvet whisker packing density that maximally suppresses secondary electronemission yield are determined as a function of velvet aspect ratio and electronangle of incidence.
展开▼
机译:材料表面上的复杂结构可以显着减少该表面的总二次电子发射。天鹅绒是由一系列竖立的胡须组成的表面。这种减少的发生是由于捕获了在结构底部和天鹅绒晶须侧面发射的低能,真正的二次电子。我们进行了数值模拟,并开发了一个近似的分析模型,该模型可以根据天鹅绒晶须长度和堆积密度以及一次电子的入射角来计算天鹅绒表面的净二次电子发射量。我们发现要抑制二次电子,必须满足以下有关无量纲参数的条件:{\ pi} / 2 DA tan {\ theta} >> 1其中{\ theta}是一次电子与法线的入射角,D为天鹅绒晶须基底所占表面积的分数,A是长宽比,A {equiv} h / r,天鹅绒晶须的高度与半径之比。我们发现,当今可用的天鹅绒可以将二次电子产率从平坦表面的值降低90%。确定最大抑制二次电子发射产率的最佳天鹅绒晶须堆积密度的值,取决于天鹅绒纵横比和入射电子角。
展开▼