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    • 3. 发明专利
    • Optical isolator
    • 光学隔离器
    • JPS6157922A
    • 1986-03-25
    • JP17987584
    • 1984-08-29
    • Fujitsu Ltd
    • MASUDA SHIGEFUMI
    • G02F1/09G02B6/42G02B27/28
    • G02B6/4209
    • PURPOSE:To increase the isolation of the optical isolator by providing a polarization splitting mirror group as a polarizer on both sides of a Faraday rotation element. CONSTITUTION:Projection light from a laser diode 11 consists of, for example, vertical polarized light and is converted by a lens 12 into a parallel light beam, which is incident on the polarization splitting mirror group 13. Vertical polarized light projected from the polarization splitting mirror group is incident on the Faraday rotation element 14 to have its polarization direction turned by 45 deg., made incident on a polarization splitting mirror group 15, and converged on a point A through a lens 16. Light traveling from a point in the opposite direction passes through the lens 16 and polarization splitting mirror group 15 and projected having the direction rotated by 45 deg. through the Faraday rotation element 14; and the projection light is horizontally polarized light and perpendicular to the propagation direction of the polarization splitting mirror 13 and the light is all reflected in a direction Px. Therefore, there is no light returning to the laser light dd through the lens 12, and the function of the optical isolator is realized.
    • 目的:通过在法拉第旋转元件的两侧提供偏振分光镜组作为偏振片来增加光隔离器的隔离度。 构成:来自激光二极管11的投影光由例如垂直偏振光构成,并由透镜12转换成入射在偏振光分离镜组13上的平行光束。从偏振分束投射的垂直偏振光 反射镜组入射在法拉第旋转元件14上以使其偏振方向转动45度,入射到偏振分束镜组15上,并通过透镜16会聚在点A.从相对的点移动的光 方向通过透镜16和偏振分束镜组15并且投影方向旋转45度。 通过法拉第旋转元件14; 并且投影光是水平偏振光并且垂直于偏振分束镜13的传播方向,并且光全部在方向Px上反射。 因此,没有光通过透镜12返回到激光dd,并且实现了光隔离器的功能。
    • 4. 发明专利
    • Optical isolator
    • 光学隔离器
    • JPS59119316A
    • 1984-07-10
    • JP22844982
    • 1982-12-27
    • Fuji Elelctrochem Co Ltd
    • NAKANO TAKAYUKI
    • G02B6/42G02B27/28G02F1/09
    • G02F1/093G02B6/4209
    • PURPOSE:To attain a small-size and light weight further reduce cost, of a device by combining one polarizer with a magnetooptic element which provides polarization on a slanting surface arranged at the complementary angle of a Brewster angle to an optical axis. CONSTITUTION:Light L12 reflected by an end surface of an optical fiber 5 passes through the polarizer 1 in the opposite direction as shown by B to enter the transmission surface 13 of the magnetooptic element 10. The light is influenced therein by an external magnetic field H and its plane of polarization rotates counterclockwise in regard to its optical axis; and the light propagates while reflected repeatedly by a reflecting film 14. Linear polarized light reaching the slanting surface 12 while the plane of polarization rotates by 45 deg. has the plane of polarization rotated by 90 deg. as compared with light in the forward direction shown by A and is reflected by the slanting surface 12 which provides polarization, so almost no light returns to a semiconductor laser 4. This constitution reduces the size, weight and cost of the optical isolator.
    • 目的:为了实现小尺寸和轻量化,通过将一个偏振器与磁光元件组合来进一步降低成本,该光学元件在布鲁斯特角的互补角度与光轴布置的倾斜表面上提供极化。 构成:由光纤5的端面反射的光L12沿着与B所示相反的方向穿过偏振器1,进入磁光元件10的透射面13.光受到外部磁场H 并且其偏振面相对于其光轴反时针旋转; 并且光在反射膜14反复反射的同时传播。偏振平面旋转45度时到达倾斜面12的直线偏振光。 具有偏振面旋转90度。 与A所示的向前方向的光相比,被倾斜面12反射,倾斜面12提供极化,所以几乎没有光返回到半导体激光器4.这种结构减小了光隔离器的尺寸,重量和成本。
    • 6. 发明专利
    • Optical device
    • 光学装置
    • JP2014163993A
    • 2014-09-08
    • JP2013032404
    • 2013-02-21
    • Sumitomo Osaka Cement Co Ltd住友大阪セメント株式会社
    • OKAMURA MIKIHARA NORITAKA
    • G02B6/122G02B6/42
    • G02B6/327G02B6/122G02B6/30G02B6/4209G02B2006/12147G02F2001/212G02F2201/06G02F2202/20
    • PROBLEM TO BE SOLVED: To provide an optical device capable of suitably maintaining the amount of light to be outputted to the outside.SOLUTION: In an optical modulator 1, positions of emission ends of two waveguides 42b and 42c can be shifted from each other in a direction A which is an extension direction of the waveguides and is a propagation direction of light emitted from the waveguides, by setting an angle θ formed between an emission end surface 41b of a waveguide substrate 41 and the direction A to less than 0° and more than 90°. On the other hand, a distance between the two waveguides 42b and 42c and a distance between condenser elements 6a and 6b of a light condensing member 6 having the condenser elements 6a and 6b formed on an element installation surface 60b can be adjusted by adjusting an attachment position of the light condensing member 6, whereby the amount of light to be outputted to the outside can be suitably maintained.
    • 要解决的问题:提供能够适当地保持输出到外部的光量的光学装置。解决方案:在光学调制器1中,两个波导42b和42c的发射端的位置可以彼此偏移 作为波导的延伸方向的方向A,并且是通过设定角度而从波导发射的光的传播方向; 形成在波导基板41的发射端面41b与方向A之间,小于0°且大于90°。 另一方面,两个波导42b和42c之间的距离以及形成在元件安装表面60b上的具有聚光元件6a和6b的聚光部件6的聚光元件6a和6b之间的距离可以通过调节附件 聚光部件6的位置,能够适当地保持输出到外部的光量。
    • 9. 发明专利
    • Optical isolator
    • 光学隔离器
    • JPS6120016A
    • 1986-01-28
    • JP14107884
    • 1984-07-06
    • Fujitsu Ltd
    • WATANABE SHIGEKIOKUJIMA HIROKIOKAMOTO AKIRACHIKAMA TERUMI
    • G02F1/09G02B6/42G02B27/28
    • G02B6/4209
    • PURPOSE:To prevent incident light and emission light from deviating in axis and simplify optical system constitution by arranging the 1st and the 2nd prisms at both sides of a Faraday rotating element, and making the shape of its cross section trapezoid. CONSTITUTION:The 2nd prisms 3 are arranged upside down at both sides of the Faraday rotating element 1. When the vertical angle and refractive index of the prism are selected properly, light emitted by a light source 6, i.e. incident light 4 is made incident on the 1st prism 2 in the forward direction and deflected, and reflected rotally by a flank of the Faraday rotating element 1, so that the emission light 5 and incident light 4 do not deviate in axis in parallel and the emission light is in the same direction with the incident light 4. The incident light 4 made incident in the opposite direction, i.e. from the side of the 2nd prism 2 is zero-deflected by the 1st prism 2 when (e)-polarized to generate projected light 8 or (e)-polarized by the 1st prism 2 when zero-polarized to generate emission light 9. Namely, return light in the opposite direction is separated with high performance and never fed back to the light source 6.
    • 目的:通过在法拉第旋转元件的两侧布置第一和第二棱镜,并使其横截面梯形形状,防止入射光和发射光偏离轴,简化光学系统构成。 构成:第二棱镜3在法拉第旋转元件1的两侧被倒置放置。当正确选择棱镜的垂直角度和折射率时,由光源6发射的光即入射光4入射到 第一棱镜2在正向上被偏转,并被法拉第旋转元件1的侧面旋转地反射,使得发射光5和入射光4在轴上不平行偏离,并且发射光在相同方向 当(e)偏振以产生投射光8时,入射光4在相反方向(即从第二棱镜2的一侧入射)被第一棱镜2零偏转,或(e) 当零极化以产生发射光9时被第一棱镜2偏振。即,相反方向的返回光以高性能分离,并且不会反馈到光源6。