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    • 9. 发明申请
    • Optoelectronic device with controlled temperature dependence of the emission wavelength and method of making same
    • 具有受控温度依赖性的发光波长的光电器件及其制造方法
    • US20120105932A1
    • 2012-05-03
    • US12925707
    • 2010-10-28
    • Nikolay Ledentsov
    • Nikolay Ledentsov
    • G02F1/017H01S3/063G02F1/01H01S3/13B82Y20/00
    • H01S5/1028H01S3/109H01S5/0651H01S5/0654H01S5/12H01S5/14H01S5/18302H01S5/18308H01S5/2027H01S5/2031H01S5/423
    • A device representing a reflector, for example an evanescent reflector or a multilayer interference reflector, with at least one reflectivity stopband is disclosed. A medium with means of generating optical gain is introduced into the layer or several layers of the reflector. The optical gain spectrum preferably overlaps with the spectral range of the reflectivity stopband. This reflector is attached to multilayer passive cavity structure made of semiconducting, and/or dielectric, and/or metallic materials with the inserted tools of achieving wavelength selection of the optical modes. For example, volume Bragg gratings, distributed feedback gratings or patterns, using of vertical optical cavities surrounded by multilayer Bragg reflectors can be applied. The optical modes of the passive optical cavity partially penetrate into the gain region of the reflector. As a result of the interaction of the gain medium in the reflector region and the passive cavity modes, photons are generated or amplified in the passive cavity at wavelengths defined by the passive cavity modes. The materials selected for the passive cavity layers are chosen to provide the necessary temperature dependence of the effective index of refraction of the related optical modes of the passive cavity and serve as a tool to achieve the controlled temperature dependence of the wavelength of the emitted photons. In particular a complete suppression of the wavelength to temperature variations can be achieved. In another case a strong shift of the resonant wavelength or wavelengths with temperature may be realized. Thus the structure represents an optoelectronic device with controlled temperature dependence of the emission wavelength.
    • 公开了一种表示具有至少一个反射阻挡带的反射器,例如ev逝反射器或多层干涉反射器的装置。 具有产生光学增益的方法的介质被引入反射器的层或几层中。 光学增益谱优选与反射阻挡带的光谱范围重叠。 该反射器附接到由半导体和/或电介质和/或金属材料制成的多层无源腔结构,其中插入的工具实现光学模式的波长选择。 例如,可以应用使用由多层布拉格反射器包围的垂直光学腔的体积布拉格光栅,分布式反馈光栅或图案。 无源光学腔的光学模式部分地进入反射器的增益区域。 作为反射器区域中的增益介质与无源腔模式的相互作用的结果,在被动空腔模式定义的波长下,在无源腔中产生或放大光子。 选择用于无源腔层的材料被选择为提供无源腔的相关光学模式的有效折射率所需的温度依赖性,并且作为实现所发射光子的波长的受控温度依赖性的工具。 特别地,可以实现波长对温度变化的完全抑制。 在另一种情况下,可以实现谐振波长或波长随温度的强烈偏移。 因此,该结构表示具有受控于发射波长的温度依赖性的光电子器件。