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    • 1. 发明授权
    • High performance light-emitting devices
    • 高性能发光装置
    • US07863632B2
    • 2011-01-04
    • US11573774
    • 2004-08-23
    • Li LiJerzy DobrowolskiDaniel Poitras
    • Li LiJerzy DobrowolskiDaniel Poitras
    • H01L33/00H01L21/00
    • H01L51/5265H01L51/0059H01L51/0078H01L51/0081
    • An organic light emitting device consists of a layered structure including a top multilayer stack, a bottom multilayer stack, a cavity layer between the top multilayer stack and the bottom multilayer stack, and an organic light emitting region within the cavity layer. The layered structure is constructed such that the product of phase factors ξ1 and ξ2 is. greater than 80% at the center of at least one emitting wavelength region and for a normal viewing angle, wherein where Ra− and Rb+ are the reflectance of the top and bottom multilayer stacks respectively, φa− and φb+ are the phase changes on reflection for the top and bottom multilayer stacks respectively, α1 β1 are respectively the real and imaginary parts of the phase thickness of the cavity layer, α2 and β2 are respectively the real and imaginary parts of the phase thickness of the light-emitting region at the operating wavelength of the device, x is the mean distance of light emitting region from the bottom multilayer stack, n and k are the refractive index and absorption coefficient of the cavity layer, θcavity is the emitting angle inside the cavity layer, and d is the physical thickness of said cavity layer. This condition improves the light output efficiency of the device.
    • 有机发光器件由包括顶层多层堆叠,底层多层堆叠,顶层多层叠层和底层多层堆叠之间的空腔层以及空腔层内的有机发光区域的分层结构组成。 构造层状结构,使得相位因子&xgr1和xgr2的乘积为。 在至少一个发射波长区域的中心处大于80%,并且对于正常视角,其中其中R a和R b +分别是顶部和底部多层叠层的反射率,并且&phgr; b +是相位 分别为顶层和底层多层堆叠的反射变化,α1和bgr1分别是空腔层相位厚度的实部和虚部,α2和&bgr; 2分别是相位厚度的实部和虚部 在器件的工作波长处的发光区域,x是发光区域与底部多层堆叠体的平均距离,n和k是空腔层的折射率和吸收系数,腔体是内部的发射角 空腔层,d是所述腔层的物理厚度。 该条件提高了器件的光输出效率。
    • 3. 发明申请
    • High Performance Light-Emitting Devices
    • 高性能发光器件
    • US20070246705A1
    • 2007-10-25
    • US11573774
    • 2004-08-23
    • Li LiJerzy DobrowolskiDaniel Poitras
    • Li LiJerzy DobrowolskiDaniel Poitras
    • H01L51/00H01L21/00
    • H01L51/5265H01L51/0059H01L51/0078H01L51/0081
    • An organic light emitting device consists of a layered structure including a top multilayer stack, a bottom multilayer stack, a cavity layer between the top multilayer stack and the bottom multilayer stack, and an organic light emitting region within the cavity layer. The layered structure is constructed such that the product of phase factors ξ1 and ξ2 is. greater than 80% at the center of at least one emitting wavelength region and for a normal viewing angle, wherein where Ra− and Rb+ are the reflectance of the top and bottom multilayer stacks respectively, φa− and φb+ are the phase changes on reflection for the top and bottom multilayer stacks respectively, α1 β1 are respectively the real and imaginary parts of the phase thickness of the cavity layer, α2 and β2 are respectively the real and imaginary parts of the phase thickness of the light-emitting region at the operating wavelength of the device, x is the mean distance of light emitting region from the bottom multilayer stack, n and k are the refractive index and absorption coefficient of the cavity layer, θcavity is the emitting angle inside the cavity layer, and d is the physical thickness of said cavity layer. This condition improves the light output efficiency of the device.
    • 有机发光器件由包括顶层多层堆叠,底层多层堆叠,顶层多层叠层和底层多层堆叠之间的空腔层以及空腔层内的有机发光区域的分层结构组成。 层状结构被构造成使得相位因子x 1和x 2 2的乘积是。 在至少一个发射波长区域的中心处大于80%,并且具有正常的视角,其中R a a和 - 分别是顶部和底部多层叠层的反射率,分别为phi< SUB>和< b>< +分别为顶层和底层多层叠层反射的相变,α1β1分别为相厚度的实部和虚部 腔层,α2和β2分别是器件的工作波长处的发光区域的相位厚度的实部和虚部,x是 距离底层多层堆叠的发光区域的平均距离,n和k是空腔层的折射率和吸收系数,θ是空腔层内的发射角,d是物理层的物理 所述腔层的厚度。 该条件提高了器件的光输出效率。
    • 5. 发明授权
    • Multi-band multiwavelength quantum dot mode-locked lasers
    • 多波段多波长量子点锁模激光器
    • US07991023B2
    • 2011-08-02
    • US12585830
    • 2009-09-25
    • Jiaren LiuZhenguo LuSylvain RaymondPhilip PoolePedro BarriosDaniel Poitras
    • Jiaren LiuZhenguo LuSylvain RaymondPhilip PoolePedro BarriosDaniel Poitras
    • H01S3/89H01S3/10
    • H01S5/065B82Y20/00H01S5/0657H01S5/3412
    • A multi-band (multi-color) multiwavelength mode locked laser diode is provided by dynamic phase compensation of a quantum dot active medium. The laser diode is provided with a PIN diode structure where the active medium consists of a plurality of layers of quantum dots such as those produced by self-assembly from known chemical beam epitaxy methods. The multiplicity of bands may be produced by AC Stark splitting, frequency selective attenuation, or by the inclusion of multiple different layers having different, respective, peak ASE emissions. Dispersion compensation within laser facets, waveguides, and the optically active media permit the selection of a fixed dispersion within the cavity. A dynamic group phase change induced by the AC Stark effect permits compensation of the fixed dispersion sufficiently to produce an intraband mode-locked laser. Even interband mode locking was observed.
    • 通过量子点活性介质的动态相位补偿提供多波段(多色)多波长锁模激光二极管。 激光二极管设置有PIN二极管结构,其中活性介质由多个量子点层组成,例如通过已知化学束外延方法通过自组装产生的量子点。 频带的多样性可以通过AC Stark分裂,频率选择性衰减或包含具有不同的相应峰值ASE发射的多个不同的层来产生。 激光小平面,波导和光学活性介质内的色散补偿允许选择腔内的固定分散体。 由AC Stark效应引起的动态组相变使得可以充分补偿固定分散体,以产生嵌入式锁模激光器。 观察到甚至带间模式锁定。