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    • 2. 发明授权
    • Optically controlled resonant tunneling electronic devices
    • 光控谐振隧道电子器件
    • US5047810A
    • 1991-09-10
    • US294225
    • 1989-01-09
    • Daniel S. ChemlaDavid A. B. MillerStephan Schmitt-Rink
    • Daniel S. ChemlaDavid A. B. MillerStephan Schmitt-Rink
    • H01L31/10H01L29/88H01L31/0352
    • B82Y10/00H01L31/0352
    • Resonant tunneling devices having an improved device switching speed are realized by including an optical control element rather than an electrical control element for switching the device from one stable state to the other. The resulting optoelectronic device including at least one double barrier quantum well semiconductor heterostructure is controllably switched from an active state to an inactive state and vice versa by impinging optical signals from an optical control element having a mean photon energy less than the bandgap energy of the double barrier quantum well semiconductor heterostructure, wherein the active state of the device exhibits conduction of charge carriers by resonant tunneling. Improvement in the switching speed occurs because the optical processes initiated by the optical control element are condsiderably faster than the electronic processes induced by prior art electrical control elements.
    • 具有改进的器件切换速度的谐振隧道装置通过包括光学控制元件而不是将器件从一个稳定状态切换到另一个的电子控制元件来实现。 所产生的包括至少一个双重势垒量子阱半导体异质结构的光电子器件可从可激活的状态切换到非活动状态,反之亦然,通过从具有小于双重能带隙能量的平均光子能量的光学控制元件入射光学信号 势阱量子阱半导体异质结构,其中器件的活性状态通过谐振隧穿显示出电荷载流子的传导。 由于由光学控制元件启动的光学处理比由现有技术的电气控制元件引起的电子处理更加明显地更快地发生开关速度的改善。
    • 3. 发明授权
    • Optical reading of quantum well device
    • 量子阱器件的光学读数
    • US4761620A
    • 1988-08-02
    • US937387
    • 1986-12-03
    • Israel Bar-JosephTao-Yuan ChangDaniel S. ChemlaDavid A. B. Miller
    • Israel Bar-JosephTao-Yuan ChangDaniel S. ChemlaDavid A. B. Miller
    • H01L27/10G02F1/015G02F1/017H01L21/338H01L29/778H01L29/812H01L31/10H01L31/14
    • B82Y20/00G02F1/017
    • Optical apparatus is disclosed wherein narrow line width light from a source is directed through the substrate of a semiconductor structure and reflected from the gate electrode of a field effect transistor element fabricated on the surface of the semiconductor structure. A quantum well layer serves as the current channel for the field effect transistor, and charge carries from a doped semiconductor layer provide high mobility carriers in the quantum well layer. Changes in the potential between the gate and source electrodes of the field effect transistor causes the normal pinchoff of carriers in the quantum well layer thereby causing changes in the absorption characteristic presented by the quantum well layer. By directing light from the source at the gate electrode through the substrate of the semiconductor structure, a photodetector can be positioned so as to detect a change in light which has passed twice through the quantum well layer, thereby detecting a change in the electrical state of the field effect transistor.
    • 公开了一种光学装置,其中来自源极的窄线宽度光被引导通过半导体结构的衬底,并且从制造在半导体结构的表面上的场效应晶体管元件的栅电极反射。 量子阱层用作场效应晶体管的电流通道,并且来自掺杂半导体层的电荷携带在量子阱层中提供高迁移率载流子。 场效应晶体管的栅极和源极之间的电势的变化导致量子阱层中载流子的正常尖峰,从而引起量子阱层所呈现的吸收特性的变化。 通过将来自栅极的光源通过半导体结构的基板引导,可以将光电检测器定位以便检测已经通过量子阱层的两次的光的变化,从而检测电子状态的变化 场效应晶体管。
    • 5. 发明授权
    • Nonlinear optical apparatus
    • 非线性光学仪器
    • US4597638A
    • 1986-07-01
    • US566968
    • 1983-12-30
    • Daniel S. ChemlaDavid A. B. MillerPeter W. Smith
    • Daniel S. ChemlaDavid A. B. MillerPeter W. Smith
    • G02F1/017G02F1/21G02F1/313G02F1/35G02F1/355G02F3/02G02F1/015
    • B82Y20/00G02F1/017G02F1/01716G02F1/218G02F1/3556G02F3/024G02F1/3137G02F1/3515
    • A nonlinear optical apparatus is provided with a multiple layer heterostructure made from alternate layers of a charge carrier semiconductor material having a narrow bandgap energy, and a charge barrier material having a wider bandgap energy than the charge carrier material. The layers are deposited one upon the other in substantially flat planes forming a series of potential barriers. The potential barriers are capable of confining charge carriers which arise within the layers of the charge carrier semiconductor material to remain substantially therein. The optical absorption coefficient of the multiple layer heterostructure exhibits at least one sharp resonant optical absorption peak near the semiconductor material bandgap absorption. A light source is restricted to provide a beam of light photons of energy near the energy of the sharp resonant optical absorption peak for promoting production of charge carriers within the charge carrier semiconductor material. The light photons are directed into the multiple layer heterostructure so that the light photons may saturate the optical absorption coefficient and thereby cause the index of refraction of the multiple layer heterostructure to vary with incident light intensity.
    • 非线性光学装置设置有由具有窄带隙能的电荷载体半导体材料的交替层制成的多层异质结构和具有比电荷载体材料更宽的带隙能量的电荷阻挡材料。 这些层在形成一系列势垒的基本平坦的平面中彼此沉积。 势垒能够限制出现在电荷载体半导体材料的层内的电荷载体基本保持在其中。 多层异质结构的光吸收系数在半导体材料带隙吸收附近表现出至少一个锐利的共振光吸收峰。 光源被限制为在尖锐的共振光吸收峰的能量附近提供能量光束,以促进电荷载流子半导体材料内的电荷载体的产生。 光子被引导到多层异质结构中,使得光子可以饱和光吸收系数,从而导致多层异质结构的折射率随入射光强度而变化。
    • 6. 发明授权
    • Laser controlled by a multiple-layer heterostructure
    • 激光由多层异质结构控制
    • US4860296A
    • 1989-08-22
    • US53498
    • 1987-05-14
    • Daniel S. ChemlaDavid A. B. MillerPeter W. Smith
    • Daniel S. ChemlaDavid A. B. MillerPeter W. Smith
    • G02F1/017H01S3/106H01S3/113H01S5/065H01S5/14
    • B82Y20/00G02F1/017H01S3/1061H01S3/113H01S5/065H01S5/14
    • The invention is a controlled laser having an optical resonator, a laser gain medium placed inside the optical resonator, the laser gain medium being capable of emitting light and of lasing with the light, a multiple layer heterostructure placed inside the optical resonator, and means for varying an optical absorption of the multiple layer heterostructure for the light in order to control an optical gain of the optical resonator, and thereby control lasing of the laser gain medium. Passive mode locking is achieved by the light emitted by the gain medium controlling the optical absorption of the multiple layer heterostructure. Active mode locking and modulation are achieved by controlling the optical absorption of the multiple layer heterostructure by applying an electric field to the multiple layer heterostructure. Control of laser gain by an external light source is achieved by controlling the optical absorption of the multiple layer heterostructure by illuminating it with light from the external light source. An embodiment of the multiple layer heterostructure fabricated as a GaAs-AlGaAs multiple quantum well with a Type I superlattice band structure is a passive mode locker for a semiconductor diode laser.
    • 本发明是一种受控激光器,其具有光学谐振器,放置在光学谐振器内部的激光增益介质,激光增益介质能够发光并与光发射激光,多层异质结构位于光学谐振器内部,以及用于 改变光的多层异质结构的光吸收,以便控制光学谐振器的光学增益,从而控制激光增益介质的激光。 无源模式锁定是由控制多层异质结构光吸收的增益介质发出的光来实现的。 通过对多层异质结构施加电场来控制多层异质结构的光吸收来实现主动模式锁定和调制。 通过外部光源的光照射来控制多层异质结构的光吸收来实现对外部光源的激光增益的控制。 作为具有I型超晶格带结构的GaAs-AlGaAs多量子阱制造的多层异质结构的实施例是用于半导体二极管激光器的无源模式锁存器。
    • 8. 发明授权
    • High speed light modulator using multiple quantum well structures
    • 使用多个量子阱结构的高速光调制器
    • US4525687A
    • 1985-06-25
    • US558545
    • 1983-12-02
    • Daniel S. ChemlaTheodoor C. DamenArthur C. GossardDavid A. B. MillerThomas H. Wood
    • Daniel S. ChemlaTheodoor C. DamenArthur C. GossardDavid A. B. MillerThomas H. Wood
    • G02F1/017H01S5/34G02B5/14
    • B82Y20/00G02F1/017H01S5/34
    • A semiconductor apparatus is provided. The apparatus has a multiple layer heterostructure having first and second material layers having first and second bandgaps, respectively and a semiconductor layer of a third bandgap being fabricated between said material layers, the bottom of the conduction band of said semiconductor layer is below the bottom of the conduction band of said material layers, and the top of the valence band of said semiconductor layer is above the top of the valence band of said material layers, the thickness of said semiconductor layer is chosen sufficient for carrier confinement effects within said semiconductor layer to influence the optical properties of said multiple layer heterostructure, and means for applying an electric field to the multiple layer heterostructure in order to vary an optical absorption coefficient and an index of refraction of the multiple layer heterostructure in response to the electric field. The apparatus is adapted for use as an optical absorption modulator or optical phase modulator, or as an electrically tuned Fabry-Perot cavity or as a polarization modulator, or as a nonlinear or bistable apparatus in which the operating point is varied by application of an electric field.
    • 提供一种半导体装置。 该装置具有多层异质结构,其具有分别具有第一和第二带隙的第一和第二材料层,并且在所述材料层之间制造第三带隙的半导体层,所述半导体层的导带的底部低于 所述材料层的导带和所述半导体层的价带的顶部高于所述材料层的价带的顶部,所述半导体层的厚度被选择为足以用于在所述半导体层内的载流子约束效应 影响所述多层异质结构的光学性质,以及用于向多层异质结构施加电场以便响应于电场改变多层异质结构的光吸收系数和折射率的装置。 该装置适合用作光吸收调制器或光相位调制器,或用作电调制的法布里 - 珀罗腔或作为偏振调制器,或者用作非线性或双稳态装置,其中工作点通过施加电 领域。
    • 9. 发明授权
    • Semiconductor device including cascaded modulation-doped quantum well
heterostructures
    • 包括级联调制掺杂量子阱异质结构的半导体器件
    • US5008717A
    • 1991-04-16
    • US322958
    • 1989-03-03
    • Israel Bar-JosephTao-Yuan ChangDaniel S. Chemla
    • Israel Bar-JosephTao-Yuan ChangDaniel S. Chemla
    • G02F1/015G02F1/017H01S5/00
    • B82Y20/00G02F1/01725G02F1/01708G02F2001/0175
    • Modulation-doped quantum well heterostructures are cascaded in a semiconductor device to achieve high speed operation while obtaining large index of refraction or absorption coefficient changes for modulating lightwave signals without significant increases in the operating potentials over prior quantum well structures. Each modulation-doped quantum well heterostructure exhibits substantially equal boundary conditions in an unbiased condition for efficient cascading or stacking. Each quantum well has associated with it a barrier layer to minimize leakage current. As a result, each quantum well has associated with it a separate charge reservoir. This aspect contributes to the speed of the cascaded structure. When incorporated within a waveguide structure, cascaded modulation-doped quantum well heterostructures can act as an external modulator, or as an intra-cavity wavelength tuning element, or as an intra-cavity modulator, or even as an optically-pumped laser.
    • 调制掺杂的量子阱异质结构在半导体器件中级联以实现高速操作,同时获得大的折射率或用于调制光波信号的吸收系数变化,而不会超过现有量子阱结构的操作电位的显着增加。 每个调制掺杂的量子阱异质结构在无偏置条件下表现出基本相等的边界条件,用于有效的级联或堆叠。 每个量子阱与其相关联的阻挡层以最小化泄漏电流。 因此,每个量子阱都与一个单独的电荷储层相关联。 这个方面有助于级联结构的速度。 当结合在波导结构中时,级联调制掺杂的量子阱异质结构可以用作外部调制器,或者作为腔内波长调谐元件,或作为腔内调制器,或者甚至作为光泵浦激光器。