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
    • 11. 发明授权
    • Optical amplifier with complementary modulation signal inputs
    • 具有互补调制信号输入的光放大器
    • US5657153A
    • 1997-08-12
    • US408030
    • 1995-03-21
    • John EndrizDavid F. WelchRobert G. WaartsSteven SandersDonald R. Scifres
    • John EndrizDavid F. WelchRobert G. WaartsSteven SandersDonald R. Scifres
    • H04B10/17H01S3/00H04B10/04
    • H04B10/291H04B10/2912H01S3/005H01S3/06712H01S3/06754H01S3/10015H01S3/2383H01S5/06216H01S5/4087
    • In an optical transmission medium, such as a fiber amplifier, two optically distinguishable signals with complementary modulation are both inputted into the amplifying medium for encoding information, particularly a serial stream of digital data, or alternatively, redundant encoding of pulses. The gain profile in the medium is preferably maintained approximately constant at all times, so that whichever amplified signal is used as the primary information carrier, its output intensity will be substantially stable from pulse to pulse, independent of recent pulse history. The two complementary signals may have different orthogonal linear polarizations or wavelengths with the same stimulated emission cross-section, so that the population inversion profile stays constant, whichever signal happens to be on at a given moment. The two signals may be derived from separate intensity modulated laser diode signal sources, from a single laser diode signal source switched between two emission wavelengths, or from a single laser diode with constant emission coupled to a directional coupler directing two complementary polarized light signals into the fiber amplifying medium.
    • 在诸如光纤放大器的光传输介质中,具有互补调制的两个光学可区分信号都被输入到用于对信息进行编码的放大媒体,特别是串行数字数据流,或备选地,脉冲的冗余编码。 介质中的增益分布优选总是保持近似恒定,因此无论使用哪个放大信号作为主信息载体,其输出强度将基本上与脉冲相比稳定,与最近的脉冲历史无关。 两个互补信号可以具有不同的具有相同受激发射横截面的正交线性偏振或波长,使得群体反转谱保持恒定,无论哪个信号在给定时刻发生什么信号。 两个信号可以从单独的强度调制的激光二极管信号源获得,来自在两个发射波长之间切换的单个激光二极管信号源,或者来自具有恒定发射的单个激光二极管耦合到定向耦合器,其将两个互补偏振光信号引入到 光纤放大介质。
    • 12. 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。
    • 13. 发明授权
    • Antiguided semiconductor laser array with edge reflectors
    • 具有边缘反射器的反射半导体激光器阵列
    • US5159604A
    • 1992-10-27
    • US737463
    • 1991-07-29
    • David G. MehuysAmos A. HardyDavid F. WelchRobert G. WaartsDonald R. Scifres
    • David G. MehuysAmos A. HardyDavid F. WelchRobert G. WaartsDonald R. Scifres
    • H01S5/40
    • H01S5/4031
    • In a semiconductor laser array structure in which antiguided regions between high effective refractive index waveguide regions experience greater gain then the waveguide regions, structures introduced at the sides of the array, next to the edgemost waveguides and not on the array period, reflect laterally transmitted radiation back toward the center of the array. The edge reflecting structures may be waveguide regions having widths of (m'+1/2) half-wavelengths, where "m'" is zero or a positive integer, compared to array waveguides with width m, where "m" is an integer not necessarily equal to "m'". The edge reflecting structures may also be stacks of such waveguides, where the regions between the edge waveguides are of a width substantially equal to (n'+1/2) half-wavelengths, compared to antiguide element widths of n half-wavelengths. The two integers n and n' may be, but are not necessarily, equal. Alternatively, the edge reflectors can be mirrors fabricated at the side edges of the array or by disordering the active region beyond the edgemost waveguides to form a refractive index step. The mirrors should be positioned a distance substantially a/2 from the edgemost emitters, where "a" is the array period.
    • 在半导体激光器阵列结构中,其中高有效折射率波导区域之间的防护区域具有更大的增益,然后波导区域,引导在阵列侧面的结构,在边缘波导旁边,而不是阵列周期,反射横向透射辐射 回到阵列的中心。 与具有宽度m的阵列波导相比,边缘反射结构可以是宽度为(m'+ 1/2)半波长的波导区域,其中“m”为零或正整数,其中“m”为整数 不一定等于“m”。 边缘反射结构也可以是这样的波导的堆叠,其中边缘波导之间的区域的宽度基本上等于(n'+ 1/2)个半波长,与n个半波长的防卫元件宽度相比。 两个整数n和n'可以是但并不一定相等。 或者,边缘反射器可以是在阵列的侧边缘处制造的反射镜,或者通过使有源区域超出边缘波导的方式来形成折射率步骤。 镜子应该与edgemost发射器的距离基本上为1/2,其中“a”是阵列周期。
    • 14. 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。
    • 16. 发明授权
    • Methods for forming group III-arsenide-nitride semiconductor materials
    • 形成III族砷化物 - 氮化物半导体材料的方法
    • US06342405B1
    • 2002-01-29
    • US09576746
    • 2000-05-23
    • Jo S. MajorDavid F. WelchDonald R. Scifres
    • Jo S. MajorDavid F. WelchDonald R. Scifres
    • H01L2100
    • H01S5/3235C23C16/303C30B25/02C30B29/40H01L33/32H01S5/32H01S5/323H01S5/32341H01S5/32366H01S5/32375
    • 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。