会员体验
专利管家(专利管理)
工作空间(专利管理)
风险监控(情报监控)
数据分析(专利分析)
侵权分析(诉讼无效)
联系我们
交流群
官方交流:
QQ群: 891211   
微信请扫码    >>>
现在联系顾问~
热词
    • 3. 发明专利
    • QUANTUM WIRE WAVEGUIDE
    • JPH06275813A
    • 1994-09-30
    • JP6160693
    • 1993-03-22
    • HITACHI LTD
    • HARAGUCHI KEIICHIYAZAWA MASAMITSUKA KIRIN
    • H01L29/06H01L29/66
    • PURPOSE:To provide a waveguide electron waves which can be excelletly controlled without any influence of fluctuation of the boundaries and surfaces of crystals even when a quantum wire which is relatively larger than the conventional one is used. CONSTITUTION:The figure is a perspective view of a cylindrical quantum wire. The central part of the wire is constituted of a material having an electron affinity stronger than that of the semiconductor material constituting the outer part of the central part. The semiconductor material is doped with impurities so that the outer part can also work as a carrier supplying layer. The wave function 2 of the electron in the radial direction (kr) forms a standing wave by being confined by the side faces of a waveguide 1 for electron wave the waveguide. The wave function 3 in the side face direction (kphi) of the waveguide satisfies a periodic boundary condition, because the side faces of the waveguide form the side faces of an annulus, and also forms a standing wave. In the above-mentioned two directions, the wave number vector component of the electron becomes zero and a one-directional electron gas state in which electron wave propagates only in the axial direction of the cylinder is set. Therefore, a waveguide for electron wave can be realized even when the quantum has a relatively large size.
    • 4. 发明专利
    • MEMORY ELEMENT ULTRAHIGH IN DENSITY
    • JPH04152575A
    • 1992-05-26
    • JP27629190
    • 1990-10-17
    • HITACHI LTD
    • HARAGUCHI KEIICHIKATSUYAMA TOSHIO
    • H01L21/205H01L21/339H01L29/06H01L29/762H01L29/80
    • PURPOSE:To reduce the size of a memory and enable superhigh density by forming a cyclic potential well in the longitudinal direction of a semiconductor quantum fine line whose diameter is above a specified value, and storing electrons in the well within the range of one or several pieces. CONSTITUTION:Since the GaAs needle-shaped crystal is approximately 6mum, the Al0.1 Ga0.9As layer 3 is approximately 500Angstrom in well width, and the GaAs layer 4 is approximately 100Angstrom in well width, approximately one hundred electrodes can be attached. And electrodes 8 approximately 100Angstrom in diameter are attached to both ends of the needle-shaped crystal so that an electric field can be applied in the longitudinal direction of the quantum well fine line being the semiconductor 100Angstrom or less in diameter. Using the element being made this way as a memory element, the potential well with electrons, to 1, and the well without electrons, to 0, are made to correspond, and those are stored. The electrons are stored in the GaAs layer 4, and if one makes the insulating layer thin in advance, it is possible for the electrons to passes through it by the tunnel effect and reach the electrode 1 and to be sent to an electrode 2 and also sent in form the electrode 2. Furthermore, the electrode 8 can shift the electrons one by one from one quantum well to another quantum well by applying electric fields to both sides of the quantum fine line by a lead wire 5.
    • 10. 发明专利
    • OPTICAL SEMICONDUCTOR ELEMENT
    • JPH06252490A
    • 1994-09-09
    • JP3301793
    • 1993-02-23
    • HITACHI LTD
    • SATO TOSHIHIKOYAZAWA MASAMITSUHARAGUCHI KEIICHIUSAGAWA TOSHIYUKIHIRUMA TAKEYUKIKATSUYAMA TOSHIO
    • G02F1/37H01L21/20H01S3/109H01S5/00H01S5/026H01S3/18
    • PURPOSE:To obtain a wavelength conversion element having a high wavelength conversion efficiency, by providing an optically transparent region in the wavelength conversion element with respect to the shorter light wavelength than the one corresponding to the band gap of a semiconductor material in a bulk state. CONSTITUTION:In order that the second higher harmonic of a light is absorbed in a quantum box region 100 of a semiconductor material, it is required that the level in the conduction band of the material whereto electron in the valence band of the material is subjected to a transition by its resonant excitation is in an inoccupied state. In the conduction band laid in the quantum box, no electron level other than discrete levels 50, 51 exists, and therefore, such a transition as a transition 62 is not generated. Also, since the level 50 is occupied by electron in the conduction band, no transition to the level 50 is generated. Further, the level 51 has the height whereto no transition of electron can get even though electron in the conduction band is excited. Therefore, there is no level which resonates to the light having energy hnu in the quantum box 100. Further, no second higher harmonic is absorbed in a barrier region 101 since its band gap is larger than the energy hnu of the second higher harmonic.