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    • 5. 发明申请
    • PLASMA GENERATOR
    • 等离子发生器
    • US20110042008A1
    • 2011-02-24
    • US12735807
    • 2009-02-20
    • Masaru HoriHiroyuki KanoKazuo AmanoTetsuya KoikeNaofumi YoshidaToshiyuki Ikedo
    • Masaru HoriHiroyuki KanoKazuo AmanoTetsuya KoikeNaofumi YoshidaToshiyuki Ikedo
    • C23F1/08H05H1/48
    • H05H1/48H01J37/3244H01J37/32449H01J37/32467H01J37/3255
    • To provide a plasma generator having a plasma-generating zone of an increased volume.A plasma generator 100 has a casing 10 made of a sintered ceramic produced from alumina (Al2O3) as a raw material. The casing 10 has a slit-like gas intake section 12, and a gas discharge section 20 in which a plurality of holes are disposed in a line. From the gas intake section 12 to the top of a plasma-generating zone P, the slits have a width of 1 mm. There is provided a second gas discharge section 22 including holes 24 which have a diameter of 0.5 mm and a length of 16 mm and which are arranged in a line along the longitudinal axis of the plasma-generating zone P. The plasma-generating zone P has a cross-section which is a rectangle having a side of 2 to 5 mm. Electrodes 2a, 2b are provided with hollow portions on the surfaces thereof facing each other. A power sources supplies about 9 kV, which is obtained by boosting 100 V (60 Hz) and is applied to the electrodes 2a, 2b with a current of 20 mA. When argon gas is supplied through a gas intake section 12, a plasma was generated, even when the electrodes 2a, 2b were separated at a maximum spacing of 4 cm. No electric discharge was generated between the tips of the holes 24 and a treatment object.
    • 提供具有增加体积的等离子体产生区域的等离子体发生器。 等离子体发生器100具有由作为原料的氧化铝(Al 2 O 3)制成的烧结陶瓷制成的壳体10。 壳体10具有狭缝状的气体吸入部12和排列在多个孔中的气体排出部20。 从气体吸入部12到等离子体产生区P的顶部,狭缝的宽度为1mm。 设置有第二气体排出部22,该第二气体排出部22具有直径为0.5mm,长度为16mm的孔24,沿着等离子体产生区P的纵轴线排列。等离子体产生区P 具有侧面为2〜5mm的矩形的截面。 电极2a,2b在其彼此面对的表面上设置有中空部分。 电源提供约9kV,其通过升压100V(60Hz)而获得,并以20mA的电流施加到电极2a,2b。 当通过气体进入部分12供应氩气时,即使电极2a,2b以4cm的最大间距分离,也产生等离子体。 在孔24的尖端和处理对象物之间不产生放电。
    • 7. 发明申请
    • Discharge Light Source
    • 放电光源
    • US20090140651A1
    • 2009-06-04
    • US12227434
    • 2007-05-21
    • Masaru HoriHiroyuki Kano
    • Masaru HoriHiroyuki Kano
    • H01J17/26H01J61/16H01J61/06
    • H01J61/86H01J61/0732H01J61/16H01J61/28
    • [Problem]To provide a light-emitting device as a point light source having a broad emission spectrum by a safe and simple process.[Means for Solving the Problem]The discharge light source shown in FIG. 1 is composed of an insulated pipe 30 and electrodes 31a and 31b. Projections 32a and 32b extend from the electrodes 31a and 31b. When a voltage is applied to the electrodes 31a and 31b in an argon gas flow through the insulated pipe 30 passing between the projections 32a and 32b, a glow discharge is generated thereby emitting light in the area between the projections 32a and 32b. The interval between the projections 32a and 32b is so narrow that the emitting area is small, and thus the light source serves as a point light source. The emission intensity increases with an increase of the gas flow rate, whereby a continuous broad emission spectrum is produced over the ultraviolet to visible region.
    • 通过安全且简单的工艺,提供具有宽发射光谱的点光源的发光装置。 解决问题的手段图1所示的放电光源 1由绝缘管30和电极31a和31b组成。 突起32a和32b从电极31a和31b延伸。 当通过穿过突起32a和32b之间的绝缘管30的氩气流中向电极31a和31b施加电压时,产生辉光放电,从而在突起32a和32b之间的区域中发光。 突起32a和32b之间的间隔非常窄,使得发射面积小,因此光源用作点光源。 发射强度随着气体流量的增加而增加,从而在紫外到可见光区域产生连续的宽发射光谱。
    • 8. 发明授权
    • Light source
    • 光源
    • US08310673B2
    • 2012-11-13
    • US12450402
    • 2008-03-24
    • Masaru HoriHiroyuki KanoShoji Den
    • Masaru HoriHiroyuki KanoShoji Den
    • G01J3/30
    • H05H1/0025G01N21/15G01N21/3103G01N2021/158G01N2201/023G01N2201/0233G01N2201/061
    • To provide a light source which realizes accurate determination of the particle density of a plasma atmosphere without disturbing the state of the plasma atmosphere.The light source of the invention includes a tubular casing 12; a cooling medium passage 30 for causing a cooling medium to flow therethrough, the passage being provided along the inner wall of the casing; a lens 50 provided at a tip end of the casing; a first electrode 44 and a second electrode 45 which are provided in the casing and before the lens so as to be vertical to the axis of the casing and parallel to each other; and an insulating spacer 46 provided between the first electrode and the second electrode. The light source further includes a hole 47 axially penetrating the center portions of the first electrode, the insulating spacer, and the second electrode; and an electric discharge gas passage for introducing an electric discharge gas, along the inner wall of the cooling medium passage, to the back surface of the lens so that the electric discharge gas is reflected by thepslens and flows through the hole.
    • 提供一种实现等离子体气氛的粒子密度的精确测定而不干扰等离子体气氛的状态的光源。 本发明的光源包括管状壳体12; 用于使冷却介质流过其中的冷却介质通道30,所述通道沿着所述壳体的内壁设置; 设置在所述壳体的前端的透镜50; 第一电极44和第二电极45,其设置在壳体内并且在透镜之前垂直于壳体的轴线并且彼此平行; 以及设置在第一电极和第二电极之间的绝缘间隔件46。 光源还包括轴向穿过第一电极,绝缘间隔物和第二电极的中心部分的孔47; 以及放电气体通道,用于沿着冷却介质通道的内壁将放电气体引导到透镜的背面,使得放电气体被透镜反射并流过孔。
    • 10. 发明申请
    • Spectroscopy Method and Spectroscope
    • 光谱法和光谱仪
    • US20090122317A1
    • 2009-05-14
    • US11991542
    • 2006-09-06
    • Masafumi ItoNorihiko NishizawaMasaru HoriToshio GotoHiroyuki Kano
    • Masafumi ItoNorihiko NishizawaMasaru HoriToshio GotoHiroyuki Kano
    • G01N21/31G02B6/26
    • G01N21/39G01J3/02G01J3/0218G01J3/0224G01J3/10G01J3/42G01J2001/4242G01N2201/0697G02B6/2861
    • To achieve an apparatus capable of measuring a light absorption coefficient f a sample with high sensitivity. A ring down spectroscope uses a wavelength-variable femtosecond soliton pulse light source 1. Pulse light is input to a loop optical fiber 6 through a first light waveguide 4 and a wavelength selective switch 5. Ring down pulse light is input to a homodyne detector through the wavelength selective switch 5. On the other hand, pulse light propagating in the first light waveguide 4 is split and input to light waveguides constituting a second light waveguide 20 through an optical directional coupler 8 and a first optical switching element 12. The pulse light propagating in the second light waveguide 20 is input to the homodyne detector as reference light and used for synchronous detection. The plural light waveguides constituting the second light waveguide 20 differ in optical length in accordance with the length of the optical fiber 6, and can slightly change the optical length.
    • 实现能够以高灵敏度测量样品的光吸收系数f的装置。 环形光谱仪使用波长可变飞秒激光脉冲光源1.脉冲光通过第一光波导4和波长选择开关5输入到环形光纤6中。环形脉冲光通过 波长选择开关5.另一方面,在第一光波导4中传播的脉冲光通过光学定向耦合器8和第一光开关元件12被分离并输入到构成第二光波导20的光波导上。脉冲光 在第二光波导20中传播的信号被输入到零差检测器作为参考光,并用于同步检测。 构成第二光波导路20的多个光波导根据光纤6的长度的光学长度不同,并且可以稍微改变光学长度。