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    • 4. 发明申请
    • Optical Fiber and Optical Transmission Medium
    • 光纤和光传输介质
    • US20080124036A1
    • 2008-05-29
    • US11791855
    • 2006-09-13
    • Ryo MiyabeYu Mimura
    • Ryo MiyabeYu Mimura
    • G02B6/036G02B6/032
    • G02B6/03638G02B6/02333G02B6/02347G02B6/02357G02B6/02361G02B6/02376G02B6/02385G02B6/03622
    • The present invention can easily realize an optical fiber and an optical transmission line that can propagate a light in a single mode while lowering a macro-bending loss against a small-diameter bending. An optical fiber 1 according to the present invention includes a first cladding region 3 having a refractive index lower than a refractive index of a core region 2 on outer circumference of the core region 2. Sub-medium regions 5a to 5f, 6a to 6f are arranged in multilayer in the first cladding region 3, which have a refractive index lower than a refractive index of a main-medium region of the first cladding region 3. The sub-medium regions 5a to 5f having a circular shape with a lateral cross section of a diameter d1 is arranged in an inner cladding area 3a of the first cladding region 3, and the sub-medium regions 6a to 6f having a circular shape with a lateral cross section of a diameter d2 (>d1) is arranged in an outer cladding area 3b of the first cladding region 3.
    • 本发明可以容易地实现能够以单一模式传播光的光纤和光传输线,同时降低针对小直径弯曲的宏观弯曲损耗。 根据本发明的光纤1包括折射率低于芯区域2的外周上的芯区域2的折射率的第一包层区域3。 副介质区域5a至5f,6a至6f在第一包层区3中以折射率低于第一包层区3的主介质区域的折射率的方式布置成多层。 具有横截面为直径d 1的圆形的副介质区域5a至5f布置在第一包层区域3的内包层区域3a中,并且子介质区域6a至6 具有直径d 2(> d 1)的横截面的圆形的f布置在第一包层区域3的外包层区域3b中。
    • 7. 发明授权
    • Stokes parameter measurement device and method
    • 斯托克斯参数测量装置及方法
    • US07679744B2
    • 2010-03-16
    • US11987714
    • 2007-12-04
    • Mieko YamagakiYu MimuraKazuyou MizunoTakeshi Takagi
    • Mieko YamagakiYu MimuraKazuyou MizunoTakeshi Takagi
    • G01J4/00
    • G01J4/00
    • The invention provides a Stokes parameter measurement device and Stokes parameter measurement method that enable high-precision measurement. The Stokes parameter measurement device comprises a polarization splitting device which comprises an optical element formed of a birefringent crystal material and which, by means of the optical element, splits signal light to be measured into a plurality of polarized light beams and adjusts the polarization state of one or more among the plurality of polarized light beams, and a light-receiving portion for performing photoelectric conversion of an optical component of the signal light split by and emitted from the polarization splitting device.
    • 本发明提供了能够进行高精度测量的斯托克斯参数测量装置和斯托克斯参数测量方法。 斯托克斯参数测量装置包括偏振分离装置,其包括由双折射晶体材料形成的光学元件,并且通过光学元件将待测量的信号光分解为多个偏振光束并调节偏振态 多个偏振光束中的一个或多个,以及用于对由偏振分离装置分离和发射的信号光的光学分量执行光电转换的光接收部分。
    • 9. 发明授权
    • Optical filter and method of manufacturing the same
    • 光学滤波器及其制造方法
    • US06933001B2
    • 2005-08-23
    • US10047459
    • 2002-01-14
    • Abe HiroyukiYu MimuraKazuyou Mizuno
    • Abe HiroyukiYu MimuraKazuyou Mizuno
    • C23C14/54G02B1/10G02B1/11G02B5/28C23C16/52G02B5/20
    • G02B1/10C23C14/547G02B5/285
    • The optical thickness of a film formed on a substrate is controlled precisely to manufacture an optical filter having an accurate optical thickness. Time is counted during a film being formed on a substrate to note time points t with respect to a reference time set in advance. At least one of two optical characteristics of energy transmittance and energy reflectance when the film being formed on the substrate is irradiated with monitoring light is expressed by a function f(t) of the time points t based on a theoretical formula of the optical characteristic. The optical characteristic is measured by irradiating the film with the monitoring light at the time points t. A designed thickness achieving time at which the optical thickness of the film designed thickness is predicted. The film formation is stopped at the designed thickness achieving time, thereby obtaining the optical filter.
    • 精确地控制形成在基板上的膜的光学厚度,以制造具有精确的光学厚度的滤光器。 在基板上形成胶片期间计数时间,以便相对于预先设定的参考时间来记录时间点t。 基于光学特性的理论公式,通过用监视光照射在基板上形成的膜的能量透射率和能量反射率的两个光学特性中的至少一个由时间点t的函数f(t)表示。 通过在时间点t用监测光照射膜来测量光学特性。 预测薄膜设计厚度的光学厚度的设计厚度实现时间。 在设计的厚度实现时间停止成膜,从而获得滤光器。