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    • 1. 发明公开
    • At cut quartz crystal resonator element
    • Schneidequarzkristall-Resonatorelement
    • EP2372908A1
    • 2011-10-05
    • EP11168046.8
    • 2007-08-07
    • Epson Toyocom Corporation
    • Naito, MatsutaroAoshima, YoshiyukiKomine, Kenji
    • H03H9/05H03H9/19
    • H03H9/177H03H3/04H03H9/02007H03H9/02102H03H9/0595H03H9/19Y10T29/42
    • An AT cut quartz crystal resonator element includes a quartz crystal element comprising a rectangular excitation part, which comprises AT cut quartz crystal and in which an X-axis direction of quartz crystal crystallization is a long side; and a reinforcing part, which is arranged at a periphery of the rectangular excitation part and whose thickness is thicker than that of the excitation part; and an excitation electrode, which is arranged on front and rear main surfaces of the excitation part, the excitation part being integrally coupled with the thick reinforcing part, by a coupling part whose thickness is thinner than that of the excitation part; and both side surfaces of the excitation part in a long side direction being respectively constituted by two faces, which are an m-face and a crystal face other than the m-face.
    • AT切割石英晶体振子元件包括石英晶体元件,其包括矩形激励部分,其包括AT切割石英晶体,并且其中石英晶体晶体的X轴方向为长边; 以及加强部,其配置在所述矩形激励部的周围,其厚度大于所述激励部的厚度; 以及激励电极,其被配置在所述激励部的前后主表面上,所述激励部通过厚度比所述激励部的厚度更薄的联接部与所述厚加强部一体地结合; 并且激励部的长边方向的两个侧面分别由m面以外的两个面和除了m面以外的结晶面构成。
    • 7. 发明公开
    • Optical path compensating device and optical pickup using the device
    • 为光路和光学读取头,使得平衡器装置
    • EP1736974A2
    • 2006-12-27
    • EP06012154.8
    • 2006-06-13
    • Epson Toyocom Corporation
    • Matsumoto, Hiroshi, c/o Epson Toyocom Corporation
    • G11B7/125G02B27/28G02B5/30
    • G11B7/1353G02B5/3083G02B27/283G11B7/1275G11B7/1369G11B2007/0006
    • An optical-path compensating device comprises: a first wavelength plate inputting linearly polarized light that includes three different wavelengths λ 1 , λ 2 and λ 3 of which polarized directions are the same and optical paths are in parallel; a first birefringent plate inputting the linearly polarized light including the three different wavelengths that were emitted from the first wavelength plate; a second wavelength plate inputting the linear polarized light including the three different wavelengths that transmitted through the first birefringent plate; a second birefringent plate inputting the linear polarized light including the three different wavelengths that were emitted from the second wavelength plate; a third wavelength plate inputting the linear polarized light including the three different wavelengths that transmitted through the second birefringent plate. The first wavelength plate gives a phase difference 2πm 1 to the linearly polarized light including the wavelength λ 1 , a phase difference π(2n 1 -1) to the linearly polarized light including the wavelength λ 2 and a phase difference 2πq 1 to the linearly polarized light including the wavelength λ 3 respectively ( m 1 , n 1 and q 1 are integers). The first birefringent plate is arranged so as to make the linear polarized light including the wavelength λ 2 be an ordinary ray and the linear polarized light including the wavelengths λ 1 and λ 3 be an extraordinary ray, when these linear polarized light are emitted from the first wavelength plate along the optical axis of the first birefringent plate. The following equation is satisfied: t 1 = d 1 ⋅ n ⁢ 0 2 ⋅ tan θ + n ⁢ e 2 / n ⁢ 0 2 − n ⁢ e 2 ⋅ tan θ ,
      where a distance for compensating an optical path is d 1 a refractive index of the birefringent plate to an ordinary ray is n0,a refractive index of the birefringent plate to an extraordinary ray is ne, an angle between an optical axis and a normal line to a main plane of the birefringent plate is θ and the thickness of the birefringent plate is ti.
      The second wavelength plate gives a phase difference π(2m 2 -1) to the linearly polarized light including the wavelength λ 1 , a phase difference 2πn 2 to the linearly polarized light including the wavelength λ 2 and a phase difference 2πq 2 to the linearly polarized light including the wavelength λ 3 respectively ( m 2 , n 2 and q 2 are integers). The second birefringent plate is arranged so as to make the linear polarized light including the wavelengths λ 1 and λ 2 be an extraordinary ray and the linear polarized light including the wavelength λ 3 be an ordinary ray, where these linear polarized light are emitted from the first wavelength plate along the optical axis of the second birefringent plate. The following equation is satisfied: t 2 = d 2 ⋅ n ⁢ 0 2 ⋅ tan θ + n ⁢ e 2 / n ⁢ 0 2 − n ⁢ e 2 ⋅ tan θ ,
      where a distance for compensating an optical path is d 2 a refractive index of the birefringent plate to an ordinary ray is n0,a refractive index of the birefringent plate to an extraordinary ray is ne, an angle between an optical axis and a normal line to a main plane of the birefringent plate is θ and the thickness of the birefringent plate is t 2 .
      The third wavelength plate gives a phase difference π(2m 3 -1) to the linearly polarized light including the wavelength λ 1 , a phase difference π(2n 3 -1) to the linearly polarized light including the wavelength λ 2 and a phase difference 2πq 3 to the linearly polarized light including the wavelength λ 3 respectively ( m 3 , n 3 and q 3 are integers).
    • 光路补偿装置包括:第一波长板输入直线偏振光,其包括三个不同的波长“1,” 2和“哪个偏振方向的3相同和光路是并联; 第一双折射板输入的直线偏振光包括3个不同的波长与第一波长板发射的thatwere; 的第二波长板输入的直线偏振光包括3个不同的波长没有反式通过第一双折射板mitted; 的第二双折射板输入的直线偏振光包括3个不同的波长从第二波长板发射的thatwere; 通过第二双折射板的第三波长板输入的直线偏振光包括3个不同的波长并反mitted。 第一波长板给出了相位差2AM 1到的直线偏振光,包括波长“1,相位差A(2N 1 -1)到直线偏振光波长包括” 2和相位差2AQ 1到线性 偏振光分别包括波长“3(M 1,N 1和q 1为整数)。 第一双折射板被设置成使线偏振光包括波长“2是一个普通的射线和线性偏振光包括波长” 1和“3中可以非常光线,当合成线性偏振光从所发射的 沿着第一双折射板的光轴的第一波长板。 下面的等式被满足:T 1 = D 1
    • 8. 发明公开
    • Highly stable piezoelectric oscillator
    • Hochstabiler压电式振荡器
    • EP1708357A1
    • 2006-10-04
    • EP06006380.7
    • 2006-03-28
    • Epson Toyocom Corporation
    • Satoh, Tomio, c/o Epson Toyocom Corporation
    • H03B5/32
    • H05K1/141H03B5/32H05K3/366H05K2201/048H05K2201/09181H05K2201/10068H05K2201/10166H05K2201/10515
    • A highly stable piezoelectric oscillator includes a heat-generating component mounted on a base printed circuit board; an erected printed circuit board placed upright on the base printed circuit board by fitting a fitting end part in a fitting slit that is formed to penetrate the base printed circuit board; a piezoelectric resonator which is disposed horizontally and directly on the heat-generating component on the base printed circuit board and whose lead electrode part is connected and fixed on the erected printed circuit board; and an oscillation circuit component to obtain an oscillation output using the piezoelectric resonator as a frequency source. Further, connection pads are arranged opposite from each other on surfaces of the base printed circuit board along both opposing end edges of the fitting slit; arc-shaped side through holes are provided on the inner walls of the fitting slit that correspond to each of the connection pads; and lead pads are arranged so as to have positional relations to their respective connection pads on both surfaces of the fitting end part of the erected printed circuit board; and each connection pad having the side through hole is soldered to each lead pad of the fitting end part.
    • 高度稳定的压电振荡器包括安装在基底印刷电路板上的发热元件; 通过将配合端部嵌合在形成为穿过基底印刷电路板的配合狭缝中而直立放置在基板印刷电路板上的直立印刷电路板; 压电谐振器,其水平地并且直接放置在基板印刷电路板上的发热部件上,其引线电极部分连接固定在竖立的印刷电路板上; 以及使用压电谐振器作为频率源获得振荡输出的振荡电路部件。 此外,连接焊盘沿着配合狭缝的两个相对的端部边缘彼此相对布置在基底印刷电路板的表面上; 弧形侧通孔设置在与每个连接垫对应的装配狭缝的内壁上; 并且引线焊盘被布置成与竖立的印刷电路板的装配端部的两个表面上的各自的连接焊盘具有位置关系; 并且具有侧通孔的每个连接垫焊接到装配端部的每个引线焊盘。