Field emission from metal covered by film of polymer insulator

A. Ionov, E. O. Popov, A. Pashkevich, V. Svetlichnyi, M. Nikolaeva
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引用次数: 1

Abstract

Summary form only given. We obtained a low-threshold field emission from polished surface of metallic electrode which was covered by thin film of non-conjugated polymers such as: i) imide/siloxane copolymer; ii) aryl-polycarbonate; iii) Nylon 66. The films were prepared by deposition of a solution on the polished Mo or Nb electrodes. Then films were heated in air at a constant temperature to remove the major part of the polymer solvent. Field emission measurements were carried out in vacuum chamber at pressure of about 4 /spl times/ 10/sup -6/ Torr in construction with accelerating grid. We obtained a stable field emission at 4 kV/mm. However, for initial activation of the cathode, the threshold field should be 2.5-3 times more than 4 kV/mm. We observed a homogeneous fluorescence from the phosphorus glass anode with current-voltage characteristic corresponds to Fowler-Nordheim law at small electric fields but at high electric fields, there is deviation to smallest values of current. The field emission from polished metals we did not observe up to 25 kV/mm. Topography of the polymer film surfaces was analysed by an atomic force microscope before and after action of threshold field. Initially, polymers had smooth surfaces but after a threshold field emission, the surfaces were modified very strong: spikes were formed up to 400 nm high and its density was about 10 cm. Apart from conducting organic polymer such as poly (3-octylthiophene) where polymer bulk material emits electrons itself (I. Musa et al., 1998) in our case, there are two critical parameters where field emission effect exists: i) critical film thickness depending from polymer (about or less one micron) and ii) critical temperature of heat treatment for polymer film. We consider that polymer accepts the charge from metallic cathode due to relatively large effect of electrification (J. Lowell and A. C. Rose-Innes, 1980). Under the action of external electric field, the soft polymer surface was modified and polymer's needles emit electrons. We also discuss small electron affinity and field emission time stability. It should be also noted that there is correlation between field emission effect and conductivity effect that is spontaneously arisen when thin polymer films were placed between two metallic electrodes. For example, the imide/siloxane copolymer films exhibit high conductivity and supercurrents being placed between two normal metals and superconductors correspondingly (A. N. Ionov et al. 2003). There, it was also confirmed that the conductivity occurs through many channels orientated perpendicular to the polymer surfaces and connecting the two metallic electrodes. The cross-section of the conductive channels grows with increasing current as well as number of conductive path. The smallest observed value of the cross-section was less than 10/sup -10/ cm/sup 2/.
被聚合物绝缘体薄膜覆盖的金属的场发射
只提供摘要形式。我们从金属电极的抛光表面获得了低阈值场发射,表面覆盖有非共轭聚合物薄膜,如:i)亚胺/硅氧烷共聚物;(二)aryl-polycarbonate;iii)尼龙66。通过在抛光的Mo或Nb电极上沉积溶液来制备薄膜。然后在空气中恒温加热薄膜,以去除聚合物溶剂的主要部分。在加速栅格施工过程中,在压力约为4 /spl倍/ 10/sup -6/ Torr的真空室中进行了场发射测量。我们获得了稳定的4 kV/mm场发射。然而,对于阴极的初始活化,阈值场应大于4 kV/mm的2.5-3倍。我们观察到磷玻璃阳极在小电场下具有均匀的荧光,其电流-电压特性符合Fowler-Nordheim定律,但在高电场下,电流的最小值存在偏差。我们没有观察到抛光金属的场发射高达25千伏/毫米。用原子力显微镜对阈值场作用前后聚合物膜表面形貌进行了分析。最初,聚合物表面光滑,但在阈值场发射后,表面被修改得非常强:形成高达400nm高的尖峰,其密度约为10cm。在我们的案例中,除了导电有机聚合物(如聚(3-辛基噻吩),聚合物体材料本身会发射电子(i . Musa et al., 1998)之外,存在场发射效应的两个关键参数:i)取决于聚合物的临界膜厚度(约或小于1微米)和ii)聚合物膜的热处理临界温度。我们认为,由于电气化效应较大,聚合物接受来自金属阴极的电荷(J. Lowell和A. C. Rose-Innes, 1980)。在外加电场的作用下,柔软的聚合物表面被修饰,聚合物的针状结构发出电子。我们还讨论了小电子亲和力和场发射时间稳定性。还应注意的是,在两个金属电极之间放置聚合物薄膜时自发产生的场发射效应与电导率效应之间存在相关性。例如,亚胺/硅氧烷共聚物薄膜表现出高导电性,并相应地在两个正常金属和超导体之间放置超电流(A. N. Ionov etal . 2003)。在那里,还证实了电导率通过许多垂直于聚合物表面的通道发生,并连接两个金属电极。导电通道的横截面随着电流的增大和导电通道数量的增加而增大。截面最小观测值小于10/sup -10/ cm/sup 2/。
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