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    • 73. 发明授权
    • Optical directional coupler with amplification
    • 光放大定向耦合器
    • US4717228A
    • 1988-01-05
    • US882932
    • 1986-06-27
    • Lars Helge Thylen
    • Lars Helge Thylen
    • G02B6/12G02F1/025G02F1/313G02F1/35H01S3/063G02F1/00
    • H01S3/063G02F1/3133G02F2201/125G02F2202/101
    • An optical directional coupler with amplification having first, second and third waveguides respectively intended for incoming light for bar coupling of light from the first waveguide and for cross coupling of light from the first waveguide. The waveguides are transparent to the wave length of the incoming light and have a characteristic refractive index in the coupling area. The coupler also includes waveguide sections constituting coupling elements for the first, second and third waveguides as well as electrodes. An arrangement is provided for achieving optical amplification of light passing through the first and the second waveguide in the bar coupling state of the directional coupler and amplification of the light passing through the first and the third waveguides in the cross coupling state of the directional coupler by feeding a current to the electrodes according to which coupling state is desired.
    • PCT No.PCT / SE85 / 00462 Sec。 371日期1986年6月27日第 102(e)日期1986年6月27日PCT提交1985年11月18日PCT公布。 公开号WO86 / 03306 PCT 日期:1986年6月5日。一种具有放大的光学定向耦合器,其具有分别用于入射光的第一,第二和第三波导,用于光耦合来自第一波导的光并用于来自第一波导的光的交叉耦合。 波导对入射光的波长是透明的,并且在耦合区域中具有特征折射率。 耦合器还包括构成用于第一,第二和第三波导以及电极的耦合元件的波导部分。 提供了一种布置,用于在定向耦合器的条形耦合状态下实现通过第一和第二波导的光的光学放大,并且通过定向耦合器的交叉耦合状态的通过第一和第三波导的光的放大, 根据期望的耦合状态向电极供电。
    • 75. 发明授权
    • Coupling device for coupling of two waveguides
    • 用于耦合两个波导的耦合装置
    • US4278322A
    • 1981-07-14
    • US45946
    • 1979-06-06
    • Hans F. Mahlein
    • Hans F. Mahlein
    • G02B6/26G02B6/42H01S3/063G02B5/14
    • H01S3/0632G02B6/26G02B6/42G02B6/4206H01S3/0941
    • A coupling device for coupling two waveguides having different cross sections, for example a layer conductor or laser element to a strip conductor, characterized by a telescopic system, which narrows the beam cross section of the larger of these two waveguides and directs it onto a large cross-sectional end of a tapering waveguide, which tapers down to the cross section of the other waveguide or conductor. The telescopic system can be composed of one conical gradient lens, two coaxial gradient lenses, or a gradient lens coaxially arranged with a conical gradient lens. The tapering waveguide preferably is integral with the strip waveguide or conductor and is of the same type.
    • 用于将具有不同横截面的两个波导(例如层导体或激光元件)耦合到带状导体的耦合装置,其特征在于伸缩系统,其缩小这两个波导中较大者的束横截面并将其引导到大的 锥形波导的横截面端,其逐渐变细到另一个波导或导体的横截面。 伸缩系统可以由一个锥形梯度透镜,两个同轴梯度透镜或与锥形梯度透镜同轴布置的梯度透镜组成。 锥形波导优选地与带状波导或导体成一体,并且是相同类型的。
    • 79. 发明授权
    • Gaseous thin film acoustically tuned laser
    • 气体薄膜声学调谐激光
    • US4087764A
    • 1978-05-02
    • US675165
    • 1976-04-08
    • Robert A. Young
    • Robert A. Young
    • H01S3/063H01S3/097H01S3/102H01S3/10
    • H01S3/097H01S3/0632H01S3/102
    • A thin film laser typcially operating in the region of 1,000 to 10,000 A. First and second electrodes are mounted in a fluid container in spaced relation with a dielectric block in the gap between the electrodes and fixed to the first electrode. A voltage pulse applied to the electrodes produces an electric field between the electrodes with a discharge occurring in the thin film of fluid between the dielectric and second electrode. The current discharge excites the fluid, forming simple excited molecules which may have a bound upper state and a dissociative lower state connected by an optical transition. The surfaces of the block and second electrode may form an active optical wave guide for the excited molecules, in which lasing occurs. The laser may be tuned by an acoustic wave produced at the surface of the dielectric block which causes distributed feedback in the active region recycling potential laser emission through the active medium and turning the laser to a wavelength that matches the wavelength of the acoustic surface wave.
    • 一种在1000至10,000A范围内经常工作的薄膜激光器。第一和第二电极以与电极间的间隙中的介电块隔开的关系安装在流体容器中并固定到第一电极。 施加到电极的电压脉冲在电极之间产生电场,在电介质和第二电极之间的流体薄膜中发生放电。 电流放电激发流体,形成可能具有结合的上部状态的简单的激发分子和通过光学转变连接的解离的下部状态。 块和第二电极的表面可以形成用于发生激光的激发分子的有源光波导。 可以通过在介质块的表面处产生的声波来调谐激光器,其在有源区域中产生分布式反馈,通过有源介质再循环潜在的激光发射,并将激光器转换成与声表面波的波长匹配的波长。
    • 80. 发明授权
    • Leaky corrugated optical waveguide device
    • 泄漏波纹光波导器件
    • US3898585A
    • 1975-08-05
    • US43292674
    • 1974-01-14
    • IBM
    • HEIDRICH PAUL FZORY JR PETER STEPHEN
    • G02B6/34G02B6/124G02F1/295H01S3/02H01S3/063H01S3/101H01S3/20H01S3/00
    • H01S3/0635G02B6/124G02F1/2955G02F2201/302H01S3/022H01S3/20
    • Diffracted leaky optical waves are coupled out of a thin film optical waveguide device having one surface which is periodically thickness-modulated or corrugated to form an optical diffraction grating. The waveguide device is constructed such that the average thickness of the waveguide in the complex refractive index of the waveguide or one of the layers surrounding the waveguide is varied when an external power source applied to the device is varied and thereby, a parameter of the leaky wave in accordance with the variable power source. In one embodiment, the waveguide is made of light amplifying material which is suitably excited to produce lasing action and cause an optical wave to propagate in the waveguide. The variable parameter in this case is the wavelength of the leaky wave, and the leaky wave is always normal to the plane of the diffraction grating. Consequently, a tunable laser is provided. In a second embodiment, no lasing occurs, but instead, an external light source is used to cause an optical wave to propagate in the waveguide. The parameter which is varied is the angle between the leaky wave and the normal to the diffraction grating, the wavelength of the leaky wave remaining constant.
    • 衍射泄漏的光波从具有周期性厚度调制或波纹状的一个表面的薄膜光波导器件耦合,以形成光学衍射光栅。 波导器件被构造成使得当施加到器件的外部电源变化时波导的平均厚度在波导的复合折射率或围绕波导的一个层之间变化,并且因此,泄漏的参数 按照可变电源波。 在一个实施例中,波导由光放大材料制成,其被适当地激发以产生激光作用并且使光波在波导中传播。 这种情况下的可变参数是泄漏波的波长,漏波总是垂直于衍射光栅的平面。 因此,提供可调谐激光器。 在第二实施例中,不发生激光,而是使用外部光源使光波在波导中传播。 变化的参数是漏波与衍射光栅的法线之间的角度,漏波的波长保持不变。