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    • 2. 发明授权
    • Differentially pumped optical amplifer and mopa device
    • 差分泵浦光学放大器和mopa器件
    • US5539571A
    • 1996-07-23
    • US202359
    • 1994-02-28
    • David F. WelchDonald R. ScifresRobert G. WaartsDavid G. MehuysAmos A. HardyRoss A. Parke
    • David F. WelchDonald R. ScifresRobert G. WaartsDavid G. MehuysAmos A. HardyRoss A. Parke
    • H01S5/026H01S5/042H01S5/062H01S5/10H01S5/12H01S5/125H01S5/16H01S5/187H01S5/20H01S5/50H01S3/00
    • H01S5/0425H01S5/026H01S5/20H01S5/50H01S2301/163H01S2301/166H01S5/0267H01S5/0422H01S5/06243H01S5/1014H01S5/1053H01S5/1064H01S5/1085H01S5/12H01S5/125H01S5/16H01S5/187H01S5/2036H01S5/5018
    • An optical amplifier semiconductor device which is differentially pumped and a master oscillator power amplifier (MOPA) device employing such an amplifier. The amplifier allows the light propagating therein to diverge along at least part of its length, and may be a flared amplifier having a gain region that increases in width toward its output at a rate that equals or exceeds the divergence of the light. The amplifier is pumped with a current density at its input end which is smaller than the current density used to pump the output end for maintaining coherence of the beam to high power levels. Differential pumping may be both longitudinal and lateral within the amplifier. A single mode preamplifier section may be optically coupled to the input end of the amplifier. The amplifier input may have a width which is the same as or wider than that of the preamplifier output. The preamplifier may have a constant mode width or may be tapered to alter the divergence of the beams provided to the amplifier section. The laser oscillator in the MOPA device may be a single mode DBR laser diode monolithically integrated on the same substrate as the optical amplifier. Laser sources external to an amplifier chip may also be used. The input portion of the amplifier or the preamplifier section, if present, may be modulated. The laser oscillator might also be modulated if it has a high Q cavity. Tunable laser oscillators are also disclosed.
    • 差分泵浦的光放大器半导体器件和采用这种放大器的主振荡器功率放大器(MOPA)器件。 放大器允许其中传播的光沿其长度的至少一部分发散,并且可以是具有增益区域的扩张放大器,该增益区域以等于或超过光的发散度的速率朝向其输出增加。 放大器在其输入端以电流密度泵送,该电流密度小于用于泵浦输出端的电流密度,以将光束的相干性保持在高功率水平。 差分泵浦可以在放大器内部纵向和横向两者。 单模前置放大器部分可以光耦合到放大器的输入端。 放大器输入可以具有与前置放大器输出的宽度相同或更宽的宽度。 前置放大器可以具有恒定的模式宽度,或者可以是锥形的,以改变提供给放大器部分的光束的发散度。 MOPA器件中的激光振荡器可以是单模DBR激光二极管,其单片集成在与光放大器相同的衬底上。 还可以使用放大器芯片外部的激光源。 放大器或前置放大器部分的输入部分(如果存在)可以被调制。 如果激光振荡器具有高Q腔,则也可能会被调制。 还公开了可调谐激光振荡器。
    • 9. 发明授权
    • III-V arsenide-nitride semiconductor
    • III-V族砷化物半导体
    • US6100546A
    • 2000-08-08
    • US908766
    • 1997-08-07
    • Jo S. MajorDavid F. WelchDonald R. Scifres
    • Jo S. MajorDavid F. WelchDonald R. Scifres
    • C23C16/30H01L33/32H01S5/323H01L33/00H01L31/0304
    • H01S5/3235C23C16/303C30B25/02C30B29/40H01L33/32H01S5/32H01S5/323H01S5/32341H01S5/32366H01S5/32375
    • III-V arsenide-nitride semiconductor are disclosed. Group III elements are combined with group V elements, including at least nitrogen and arsenic, in concentrations chosen to lattice match commercially available crystalline substrates. Epitaxial growth of these III-V crystals results in direct bandgap materials, which can be used in applications such as light emitting diodes and lasers. Varying the concentrations of the elements in the III-V materials varies the bandgaps, such that materials emitting light spanning the visible spectra, as well as mid-IR and near-UV emitters, can be created. Conversely, such material can be used to create devices that acquire light and convert the light to electricity, for applications such as full color photodetectors and solar energy collectors. The growth of the III-V material can be accomplished by growing thin layers of elements or compounds in sequences that result in the overall lattice match and bandgap desired.
    • 公开了III-V族氮化物半导体。 III族元素与V族元素组合,包括至少氮和砷,其浓度选择为与市售的晶体基质匹配。 这些III-V晶体的外延生长导致直接的带隙材料,其可以用于诸如发光二极管和激光器的应用中。 改变III-V材料中元素的浓度会改变带隙,从而可以产生跨越可见光谱的光以及中红外和近紫外线发射体的材料。 相反,这种材料可用于产生获得光并将光转换成电的装置,用于诸如全色光电检测器和太阳能收集器的应用。 III-V材料的生长可以通过在导致总体晶格匹配和带隙期望的序列中生长薄层的元素或化合物来实现。
    • 10. 发明授权
    • Methods for forming group III-V arsenide-nitride semiconductor materials
    • 形成III-V族氮化镓半导体材料的方法
    • US6130147A
    • 2000-10-10
    • US820727
    • 1997-03-18
    • Jo S. MajorDavid F. WelchDonald R. Scifres
    • Jo S. MajorDavid F. WelchDonald R. Scifres
    • H01L33/32H01S5/323H01L21/28
    • H01S5/3235H01L33/32H01S5/32H01S5/32341H01S5/32366H01S5/32375
    • Methods are disclosed for forming Group III--arsenide-nitride semiconductor materials. Group III elements are combined with group V elements, including at least nitrogen and arsenic, in concentrations chosen to lattice match commercially available crystalline substrates. Epitaxial growth of these III-V crystals results in direct bandgap materials, which can be used in applications such as light emitting diodes and lasers. Varying the concentrations of the elements in the III-V crystals varies the bandgaps, such that materials emitting light spanning the visible spectra, as well as mid-IR and near-UV emitters, can be created. Conversely, such material can be used to create devices that acquire light and convert the light to electricity, for applications such as full color photodetectors and solar energy collectors. The growth of the III-V crystals can be accomplished by growing thin layers of elements or compounds in sequences that result in the overall lattice match and bandgap desired.
    • 公开了用于形成III族 - 氮化物 - 氮化物半导体材料的方法。 III族元素与V族元素组合,包括至少氮和砷,其浓度选择为与市售的晶体基质匹配。 这些III-V晶体的外延生长导致直接的带隙材料,其可以用于诸如发光二极管和激光器的应用中。 改变III-V晶体中元素的浓度会改变带隙,从而可以产生跨越可见光谱的光的材料,以及中红外和近紫外线发射器。 相反,这种材料可用于产生获得光并将光转换成电的装置,用于诸如全色光电检测器和太阳能收集器的应用。 III-V晶体的生长可以通过在导致总体晶格匹配和带隙期望的序列中生长薄层的元素或化合物来实现。