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    • 1. 发明专利
    • Component concentration measuring apparatus and component concentration measuring method
    • 组件浓度测量装置和组件浓度测量方法
    • JP2013224838A
    • 2013-10-31
    • JP2012096316
    • 2012-04-20
    • Seiko Epson Corpセイコーエプソン株式会社Hokkaido Univ国立大学法人北海道大学
    • NISHIDA KAZUHIROSHIMIZU KOICHI
    • G01N21/17A61B5/1455
    • PROBLEM TO BE SOLVED: To provide a novel technique for acquiring a time resolution waveform of scattered light with high resolution and a high S/N ratio, and a technique for measuring the concentration of a component that an analyte includes on the basis of the time resolution waveform with high accuracy.SOLUTION: A component concentration measuring apparatus includes an irradiation section 303, a light condensation section 304, a detection section 313 which detects light intensity, a light reception gain variable section 308 which varies the level of a signal of the light intensity detected by the detection section 313, a gate light guide section 309 which is configured to vary the length of an optical path where gate light comprising pulse light synchronized with measurement light is guided, an optical driving shutter section 311 which transmits light condensed by the light condensation section 304 toward the detection section 313 on the basis of the gate light that the gate light guide section 309 guides, an optical path length control section which varies and controls the optical path length of the gate light guide section 309, and a calculation section which calculates the concentration of a component included in an analyte by finding the time resolution waveform from the detection result of the detection section 313 at the optical path length varied by the optical path length control section.
    • 要解决的问题:提供一种用于获取具有高分辨率和高S / N比的散射光的时间分辨率波形的新技术,以及用于基于时间测量分析物包含的分量的浓度的技术 分辨率波形。解决方案:组分浓度测量装置包括照射部分303,光凝结部分304,检测光强度的检测部分313,光接收增益变量部分308,其改变信号的水平 由检测部313检测出的光强度;门导光部309,被配置为改变包括与测量光同步的脉冲光的栅极光的光路的长度;光学驱动快门部311, 光凝结部304基于栅极光gu的栅极光朝向检测部313 ide部分309引导,改变并控制栅极光导部分309的光程长度的光程长度控制部分,以及计算部分,该计算部分通过从 光路长度由光程长度控制部变化的检测部313的检测结果。
    • 2. 发明专利
    • Concentration determining device, optical absorption coefficient calculating method, concentration determining method, program for performing calculation of optical absorption coefficient and program for performing calculation of concentration
    • 浓度测定装置,光学吸收系数计算方法,浓度测定方法,用于执行光吸收系数计算的程序和执行浓度计算的程序
    • JP2013072736A
    • 2013-04-22
    • JP2011211688
    • 2011-09-27
    • Seiko Epson Corpセイコーエプソン株式会社Hokkaido Univ国立大学法人北海道大学
    • NISHIDA KAZUHIROSHIMIZU KOICHIKATO YUJI
    • G01N21/35A61B5/1455G01N21/3577G01N21/359
    • PROBLEM TO BE SOLVED: To provide a concentration determining device reducing influence of noise due to a layer other than a target layer.SOLUTION: The concentration determining device includes: optical path length distribution storage means 102; time-resolved waveform storage means 103; optical path length variation storage means 104; irradiating means 105; light receiving means 106; optical intensity acquiring means 107; optical path length acquiring means 109; optical intensity model acquiring means 110; optical absorption coefficient calculating means 111 for calculating an optical absorption coefficient of any layer on the basis of optical intensity acquired by the optical intensity acquiring means 107, an optical path length of each layer of a plurality of light scattering medium layers acquired by the optical path length acquiring means 109, an optical intensity model acquired by the optical intensity model acquiring means 110 and optical path length variations of each layer of the plurality of light scattering medium layers stored in the optical path length variation storage means 104; and concentration calculating means 113 for calculating a concentration of a target component in any layer on the basis of the optical absorption coefficient calculated by the optical absorption coefficient calculating means 111.
    • 要解决的问题:提供浓度测定装置,减小由于除了目标层以外的层引起的噪声的影响。 浓度测定装置包括:光路长度分布存储装置102; 时间分辨波形存储装置103; 光路长度变化存储装置104; 照射装置105; 光接收装置106; 光强度获取装置107; 光路长度获取装置109; 光强度模型获取装置110; 光吸收系数计算装置111,用于基于由光强度获取装置107获取的光强度计算任何层的光吸收系数,通过光路获取的多个光散射介质层的每一层的光路长度 长度获取装置109,由光强度模型获取装置110获取的光强度模型和存储在光路长度变化存储装置104中的多个光散射介质层的每一层的光程长度变化; 和浓度计算装置113,用于根据由光吸收系数计算装置111计算出的光吸收系数计算任何层中的目标成分的浓度。(C)2013,JPO&INPIT
    • 3. 发明专利
    • Projector
    • 投影机
    • JP2011008150A
    • 2011-01-13
    • JP2009153416
    • 2009-06-29
    • Seiko Epson Corpセイコーエプソン株式会社
    • NISHIDA KAZUHIROFUJIMAKI OSAMUTANAKA KATSUMI
    • G03B21/00G02F1/13G02F1/13357G03B21/16
    • G02B13/16G02B5/005
    • PROBLEM TO BE SOLVED: To provide a projector that prevents light rays from being incident on a projection optical system at unnecessary angles to suppress heating of the projection optical system and focus shift.SOLUTION: The dimming mechanism drive part 93 of a control unit 90 changes the open/close state of the dimming mechanism 80 in accordance with the F number of the projection optical system 70. This operation allows illumination light having the angular distribution corresponding to the F number of the projection system 70 to be incident on the projection system 70 and prevents the illumination light from being blocked by a lens barrel, a diaphragm, or any other similar component in the projection optical system 70. The light blockage prevents the projection optical system 70 from being heated unnecessarily, focus shift of the lens in the projection optical system 70 is prevented and fuzziness is eliminated without changing the luminance of the illuminator 10 itself.
    • 要解决的问题:提供一种防止光线以不必要的角度入射到投影光学系统上的投影仪,以抑制投影光学系统的加热和聚焦偏移。解决方案:控制单元90的调光机构驱动部分93改变 根据投影光学系统70的F数,调光机构80的打开/关闭状态。该操作允许具有与投影系统70的F数相对应的角度分布的照明光入射到投影系统70上 并且防止照明光被投影光学系统70中的镜筒,隔膜或任何其它类似部件阻挡。遮光防止投影光学系统70不必要地被加热,镜片在投影中的焦点偏移 防止光学系统70并消除模糊性,而不改变照明器10本身的亮度。
    • 4. 发明专利
    • Projector
    • 投影机
    • JP2009175570A
    • 2009-08-06
    • JP2008015878
    • 2008-01-28
    • Seiko Epson Corpセイコーエプソン株式会社
    • NISHIDA KAZUHIRO
    • G03B21/00G02B3/00G02F1/13
    • PROBLEM TO BE SOLVED: To provide a projector for improving contrast of a liquid crystal panel by adjusting illuminating direction.
      SOLUTION: Distances D1 and D1' from the center point O of a second lens array 21e to the outer circumference in a first characteristic up, down, right, and left directions are larger than a distance D2 from the center point O of a second lens array 21e to the outer circumference in a second characteristic direction tilted at an angle of 45°. Therefore, as for the high contrast direction of a first liquid crystal panel 25a, an illumination light can be made incident on the first liquid crystal panel 25a at a comparatively large incident angle, and as for the low contrast direction of the first liquid crystal panel 25a, an illumination light can be made incident on the first liquid crystal panel 25a at a comparatively small incident angle. Thereby, the contrast of an image projected by a projection lens 29 on a screen can be improved as a whole.
      COPYRIGHT: (C)2009,JPO&INPIT
    • 解决的问题:提供一种通过调节照明方向来提高液晶面板的对比度的投影仪。 解决方案:从第二透镜阵列21e的中心点O到第一特征上,下,右和左方向的外圆的距离D1和D1'大于距离中心点O的距离D2 第二透镜阵列21e以第二特征方向以45°的角度向外周延伸。 因此,对于第一液晶面板25a的高对比度方向,能够以比较大的入射角使照明光入射到第一液晶面板25a上,对于第一液晶面板的低对比度方向 如图25a所示,能够以比较小的入射角使照明光入射到第一液晶面板25a上。 由此,整体上可以提高由投影透镜29投影在屏幕上的图像的对比度。 版权所有(C)2009,JPO&INPIT
    • 5. 发明专利
    • Projector
    • 投影机
    • JP2008165136A
    • 2008-07-17
    • JP2007000438
    • 2007-01-05
    • Seiko Epson Corpセイコーエプソン株式会社
    • ISHIBASHI OSAMUNISHIDA KAZUHIRO
    • G03B21/00G02F1/13
    • G02B27/149G02B27/1046G02B27/145G02B27/28H04N9/3105H04N9/3152
    • PROBLEM TO BE SOLVED: To provide a projector increasing the F-number of an illumination optical system, without enlarging the illumination optical system, etc. SOLUTION: A coupling lens 43a cooperating with a superimposed lens 35 is provided only in a first section between a first dichroic mirror 41a and a reflecting mirror for red 42a being a bending mirror, in a first optical path OP1 from the superimposed lens 35 to a first liquid crystal display panel 61r. Thus, the F-number of the illumination optical system 30 for blue can be adjusted with a high degree of freedom and the increase in the number of lenses constituting a color separation light guide optical system 40 and the illumination optical system 30 can be prevented. Furthermore, illumination light can be prevented from entering with a large incident angle around the first liquid crystal display panel 61r and the telecentric properties of the illumination optical system 30 for blue can be secured. COPYRIGHT: (C)2008,JPO&INPIT
    • 要解决的问题:提供增加照明光学系统的F数的投影仪,而不会放大照明光学系统等。解决方案:仅提供与重叠透镜35配合的耦合透镜43a 在从重叠透镜35到第一液晶显示面板61r的第一光路OP1中,在第一分色镜41a和红色42a的反射镜之间的第一部分是弯曲镜。 因此,可以高度自由地调节用于蓝色的照明光学系统30的F数,并且可以防止构成分色导光系统40和照明光学系统30的透镜数量的增加。 此外,可以防止照明光在第一液晶显示面板61r周围以大的入射角进入,并且可以确保用于蓝色的照明光学系统30的远心特性。 版权所有(C)2008,JPO&INPIT
    • 6. 发明专利
    • Projector
    • 投影机
    • JP2007298804A
    • 2007-11-15
    • JP2006127413
    • 2006-05-01
    • Seiko Epson Corpセイコーエプソン株式会社
    • NISHIDA KAZUHIROUEHARA KATSUYUKI
    • G03B21/14G02F1/13G02F1/1335G03B21/00H04N5/74
    • G03B21/208G02B27/102G02B27/141G03B21/2066G03B33/12
    • PROBLEM TO BE SOLVED: To provide a projector where more accurate correction of chromatic aberration is performed, thereby restraining the occurrence of irregularity and blurring in an image, and making high efficiency of using light. SOLUTION: The incident surface of a first dichroic mirror 31 is arranged at an angle larger than 45° by a very small angle with respect to an illumination optical axis OA so that the reflection angle of R light on the first dichroic mirror 31 may be smaller than 45° by the very small angle, that is, a bending angle α in the optical axis direction of a first optical path OP1 may be smaller than 90°. Thus, the length of the first optical path OP1 is made somewhat longer than the length of the second optical path OP2, and the correction more corresponding to the chromatic aberration is performed than in the conventional projector. COPYRIGHT: (C)2008,JPO&INPIT
    • 要解决的问题:提供一种执行更精确的色差校正的投影仪,从而抑制图像中的不规则和模糊的发生,并且提高使用光的效率。 解决方案:第一分色镜31的入射表面相对于照明光轴OA以非常小的角度布置成大于45°的角度,使得R光在第一分色镜31上的反射角 可以以非常小的角度小于45°,即第一光路OP1的光轴方向上的弯曲角度α可以小于90°。 因此,使第一光路OP1的长度比第二光路OP2的长度稍长,并且比现有的投影仪更多地对应于色像差的校正。 版权所有(C)2008,JPO&INPIT
    • 7. 发明专利
    • Illumination optical device and projector
    • 照明光学设备和投影仪
    • JP2006106205A
    • 2006-04-20
    • JP2004290527
    • 2004-10-01
    • Seiko Epson Corpセイコーエプソン株式会社
    • NISHIDA KAZUHIRO
    • G03B21/00G02B19/00G02F1/13
    • PROBLEM TO BE SOLVED: To provide an illumination optical device capable of making a light source image at a part near an illumination optical axis out of light source images formed on a light condensing element very small, and to provide a projector.
      SOLUTION: In the illumination optical device 2, an optical device 20 is arranged between a 1st lens array 412 and a light source device 411. The optical device 20 is equipped with an optical device main body 21 whose luminous flux emitting side surface is a concave surface 212, and an optical device main body 22 whose luminous flux incident surface is a convex surface 221. The concave surface 212 is curved and recessed from a center point 212A toward an outer circumference edge. The convex surface 221 has shape corresponding to the concave surface 212.
      COPYRIGHT: (C)2006,JPO&NCIPI
    • 解决的问题:提供一种照明光学装置,其能够使形成在聚光元件上的光源图像非常小的照明光轴附近的部分处的光源图像,并且提供投影仪。 解决方案:在照明光学装置2中,光学装置20布置在第一透镜阵列412和光源装置411之间。光学装置20装备有光学装置主体21,其光束发射侧表面 是凹面212,光束入射面为凸面221的光学元件主体22.凹面212从中心点212A向外周缘弯曲并凹陷。 凸面221具有与凹面212对应的形状。(C)2006,JPO&NCIPI
    • 9. 发明专利
    • Light absorption coefficient calculation device, concentration determination device, light absorption coefficient calculation method, concentration determination method, program for calculating light absorption coefficient, and program for calculating concentration
    • 光吸收系数计算装置,浓度测定装置,光吸收系数计算方法,浓度测定方法,计算光吸收系数的程序和计算浓度的程序
    • JP2014006063A
    • 2014-01-16
    • JP2012139831
    • 2012-06-21
    • Seiko Epson Corpセイコーエプソン株式会社Hokkaido Univ国立大学法人北海道大学
    • NISHIDA KAZUHIROSHIMIZU KOICHI
    • G01N21/17A61B5/1455
    • PROBLEM TO BE SOLVED: To provide a light absorption coefficient calculation device for reducing an effect of noise generated by a layer other than a target layer, a concentration determination device, a light absorption coefficient calculation method, a concentration determination method, a program for calculating a light absorption coefficient, and a program for calculating a concentration.SOLUTION: The light absorption coefficient calculation device includes: irradiation means 102; light receiving means 103; optical intensity acquisition means 104; and light absorption coefficient calculation means 106 for obtaining a calibration curve created based optical intensity at a predetermined time of a time resolution waveform of short-time pulse light in a plurality of observation target models, optical intensity at non-absorption time at the predetermined time of the time resolution waveform of the short-time pulse light in the plurality of observation target models, and a model value of the light absorption coefficient of each of a plurality of layers of light scattering media set in each of the plurality of observation target models, and collating the optical intensity obtained by the optical intensity acquisition means 104 with the calibration curve to calculate a light absorption coefficient on an arbitrary layer.
    • 要解决的问题:提供一种减少由目标层以外的层产生的噪声的影响的光吸收系数计算装置,浓度确定装置,光吸收系数计算方法,浓度确定方法,计算程序 光吸收系数和计算浓度的程序。解光:光吸收系数计算装置包括:照射装置102; 光接收装置103; 光强度获取装置104; 以及光吸收系数计算装置106,用于获得在多个观察目标模型中的短时间脉冲光的时间分辨率波形的预定时间基于光强度产生的校准曲线,在预定时间的非吸收时间的光强度 多个观察对象模型中的短时间脉冲光的时间分辨率波形的模型值,以及在多个观察对象模型中的每一个中设置的多层光散射介质中的每一个的光吸收系数的模型值 并且将由光强度获取装置104获得的光强度与校准曲线进行比较,以计算任意层上的光吸收系数。
    • 10. 发明专利
    • Component concentration measuring apparatus and component concentration measuring method
    • 组件浓度测量装置和组件浓度测量方法
    • JP2013088244A
    • 2013-05-13
    • JP2011227932
    • 2011-10-17
    • Seiko Epson Corpセイコーエプソン株式会社Hokkaido Univ国立大学法人北海道大学
    • NISHIDA KAZUHIROSHIMIZU KOICHI
    • G01N21/27A61B5/1455
    • G01N21/4738A61B5/1455A61B5/7282G01N2201/0697
    • PROBLEM TO BE SOLVED: To propose a novel approach for acquiring a temporally decomposed waveform of scattering light with a high resolution, and to propose an approach for measuring the concentration of a component contained in an examinee with high accuracy.SOLUTION: Light-source beams from a light source 301 are split by a splitter 302, and an examinee is irradiated with one of the light beams as measuring light by an irradiator 303. Light emitted from the examinee is converged by a convergence section 304 and relayed to an optical converter 307 by a relay 305. On the other hand, the other beam split by the splitter 302 is guided to an optically driven shutter 311 as gate light. In this event, an optical path length of the gate light is changed by a gate light guide 309 and gate light of a different optical path length is guided to a Kerr substance 311A. Then, a temporally decomposed waveform is determined from the result of detecting the intensity of light in the changed optical path length, and the concentration of a component contained in the examinee is calculated.
    • 要解决的问题:提出一种用于以高分辨率获取时间分解的散射光波形的新颖方法,并且提出一种用于以高精度测量受检者中包含的成分的浓度的方法。 解决方案:来自光源301的光源光束被分离器302分离,并且被照射器303照射作为测量光的一个光束的被检体。从被检体发出的光被会聚 并通过继电器305中继到光学转换器307.另一方面,由分离器302分流的另一个光束被引导到作为栅极光的光学驱动的光阀311。 在这种情况下,栅极光的光路长度由栅极光导30改变,并且不同光程长度的栅极光被引导到克尔物质311A。 然后,根据在改变的光路长度中检测光的强度的结果来确定时间上分解的波形,并且计算包含在受检者中的成分的浓度。 版权所有(C)2013,JPO&INPIT