Abstract:
An electron emission device includes a number of electron emission units spaced from each other, wherein each of the number of electron emission units includes a first electrode, a semiconductor layer, an insulating layer, and a second electrode stacked with each other, the first electrode includes a carbon nanotube layer, a number of holes defines in the semiconductor layer, and a portion of the carbon nanotube layer suspended on the number of holes.
Abstract:
A semiconductor photocathode includes an AlXGa1-XN layer (0≦X
Abstract translation:半导体光电阴极包括通过SiO 2层和形成在AlXGa1-XN层上的含碱金属的层结合到玻璃基板上的Al x Ga 1-x N层(0&lt; nlE; X <1)。 AlXGa1-XN层包括第一区域,第二区域,第一区域和第二区域之间的中间区域。 第二区域具有通过交替层叠阻挡层和阱层而形成的半导体超晶格结构,中间区域具有通过交替层压阻挡层和阱层而形成的半导体超晶格结构。 当一对相邻的阻挡层和阱层被定义为单位部分时,单位部分中Al的组成比X的平均值随着距离第二区域和SiO 2层之间的界面位置的距离而至少在 中间区域。
Abstract:
The present invention relates to a diamond n-type semiconductor in which the amount of change in carrier concentration is fully reduced in a wide temperature range. The diamond n-type semiconductor comprises a diamond substrate, and a diamond semiconductor formed on a main surface thereof and turned out to be n-type. The diamond semiconductor exhibits a carrier concentration (electron concentration) negatively correlated with temperature in a part of a temperature region in which it is turned out to be n-type, and a Hall coefficient positively correlated with temperature. The diamond n-type semiconductor having such a characteristic is obtained, for example, by forming a diamond semiconductor doped with a large amount of a donor element while introducing an impurity other than the donor element onto the diamond substrate.
Abstract:
A display device and a flat lamp that have simple structures and can be fabricated using simple fabricating processes, and a method of fabricating the display device and the flat lamp. The display device includes: a first substrate and a second substrate facing each other across a predetermined distance; barrier ribs defining light emitting cells with the first substrate and the second substrate; an anode electrode disposed in the light emitting cell; a conductive silicon layer disposed on an inner surface of one of the first and second substrates; an oxidized porous silicon layer, at least a part of which is disposed on the conductive silicon layer; and a gas contained in the light emitting cell. The fabrication method includes doping part of a silicon layer on the inner surface of the first or second substrate and changing another part of the silicon layer to an oxidized porous silicon layer.
Abstract:
An n-GaN layer is provided as an emitter layer for supplying electrons. A non-doped (intrinsic) AlxGa1−xN layer (0≦x≦1) having a compositionally graded Al content ratio x is provided as an electron transfer layer for transferring electrons toward the surface. A non-doped AlN layer having a negative electron affinity (NEA) is provided as a surface layer. Above the AlN layer, a control electrode and a collecting electrode are provided. An insulating layer formed of a material having a larger electron affinity than that of the AlN layer is interposed between the control electrode and the collecting electrode. This provides a junction transistor which allows electrons injected from the AlN layer to conduct through the conduction band of the insulating layer and then reach the collecting electrode.
Abstract:
A cold electron emitter may include a heavily nnull doped wide band gap (WBG) substrate, a p-doped WBG region, and a low work function metallic layer (nnull-p-M structure). A modification of this structure includes heavily pnull doped region between p region and M metallic layer (nnull-p-pnull-M structure). These structures make it possible to combine high current emission with stable (durable) operation. The high current density is possible because the p-doped (or pnull heavily doped) WBG region acts as a negative electron affinity material when in contact with low work function metals. The injection emitters with the nnull-p-M and nnull-p-pnull-M structures are stable since the emitters make use of relatively low extracting electric field and are not affected by contamination and/or absorption from accelerated ions. In addition, the structures may be fabricated with current state-of-the-art technology.