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    • 42. 发明授权
    • Apparatus for manufacturing single crystal of silicon
    • 用于制造单晶硅的装置
    • US5968266A
    • 1999-10-19
    • US822088
    • 1997-03-20
    • Eiichi IinoMasanori KimuraShozo Muraoka
    • Eiichi IinoMasanori KimuraShozo Muraoka
    • C30B15/14C30B29/06C30B33/04H01L21/208C30B35/00
    • C30B15/14Y10S117/917Y10T117/1068Y10T117/1088
    • An apparatus for manufacturing a single crystal of silicon includes a crucible, a heater, electrodes, and a magnet. In addition to a plurality of heat generating portions and two main electrode portions, the heater has two or more auxiliary electrode portions. Two or more heater support members having an insulating property are further provided so as to support the heater through the auxiliary electrode portions. The number of heat generating portions which may be present between a heater support member and an electrode and between heater support members if adjacent to each other is equal to or less than 4. Each generating portion of the heater has a thickness of 25 mm or more. This structure makes it possible to produce a single crystal of silicon without causing breakage of a heater, even if a large electric current flows through the heater, even if a magnetic field of a high intensity is applied to a silicon melt in the crucible, and even if the heater has a large diameter.
    • 用于制造单晶硅的装置包括坩埚,加热器,电极和磁体。 除了多个发热部和两个主电极部之外,加热器还具有两个以上的辅助电极部。 进一步提供具有绝缘性能的两个或更多个加热器支撑构件,以便通过辅助电极部分支撑加热器。 可以存在于加热器支撑构件和电极之间以及加热器支撑构件之间的彼此相邻的发热部分的数量等于或小于4.加热器的每个产生部分的厚度为25mm以上 。 即使在坩埚中的硅熔体上施加高强度的磁场,即使大的电流流过加热器,也能够制造单晶硅,而不会导致加热器的断裂,并且 即使加热器具有大的直径。
    • 47. 发明授权
    • Display and its driving method
    • 显示及其驱动方法
    • US07499115B2
    • 2009-03-03
    • US10398385
    • 2001-10-04
    • Katsuhiko KumagawaHiroyuki YamakitaMasanori KimuraAkio Takimoto
    • Katsuhiko KumagawaHiroyuki YamakitaMasanori KimuraAkio Takimoto
    • G02F1/141G02F1/133G02F1/1343
    • G02F1/134363G02F2001/134345G09G3/3614G09G2300/0434G09G2320/0247
    • An array substrate (10) is provided with a pixel electrode (3) disposed in a region defined by two adjacent gate wirings (1) and two adjacent source wirings (2), a switching element (5) for switching a voltage applied to the pixel electrode (3) from the source wiring (2) based on a signal voltage supplied from the gate wiring (1), a common wiring (8) arranged between the two adjacent gate wirings (1) and a common electrode (4) being electrically connected to the common wiring (8) and generating an electric field between the pixel electrode (3) whereto a voltage is applied, wherein the pixel electrode (1) comprises a first pixel electrode (1a) and a second pixel electrode (2a), and the opposing electrode (2) comprises a first opposing electrode (1b) and a second opposing electrode (2b), wherein a first region generates an electric field between the first pixel electrode (1a) and the first opposing electrode (2a) whose light transmittance is lower than that of the first pixel electrode (1a) and a second region generates an electric field between the second pixel electrode (1b) and the second opposing electrode (2b) whose light transmittance is higher than that of the second pixel electrode (1b) are formed.
    • 阵列基板(10)设置有设置在由两个相邻的栅极布线(1)和两个相邻的源极布线(2)限定的区域中的像素电极(3),用于切换施加到 基于从栅极布线(1)提供的信号电压,源极布线(2)的像素电极(3),布置在两个相邻的栅极布线(1)和公共电极(4)之间的公共布线(8) 电连接到公共布线(8)并在施加电压的像素电极(3)之间产生电场,其中像素电极(1)包括第一像素电极(1a)和第二像素电极(2a) ,相对电极(2)包括第一相对电极(1b)和第二相对电极(2b),其中第一区域在第一像素电极(1a)和第一相对电极(2a)之间产生电场, 透光率比第一像素电极的透光率低 1a)和第二区域在第二像素电极(1b)和第二相对电极(2b)之间产生其透光率高于第二像素电极(1b)的电场。
    • 48. 发明申请
    • Method for driving plasma display panel
    • 驱动等离子体显示面板的方法
    • US20070097031A1
    • 2007-05-03
    • US10559728
    • 2005-05-24
    • Kunihiro MimaMasanori KimuraTeiichi Kimura
    • Kunihiro MimaMasanori KimuraTeiichi Kimura
    • G09G3/28
    • G09G3/294G09G3/2965G09G2310/066G09G2320/0233
    • A method for driving a plasma display panel is disclosed in which generation of a region having brightness non-uniformity can be reduced over an entire screen without changing the voltage and pulse width of sustain pulses thus enabling suppression of an increase in power consumption. This method for driving a plasma display panel comprises an initialization period for forming a discharge cell at an intersection where scan electrode and sustain electrode meet data electrode and generating initialization discharge in the cell, a writing period for generating writing discharge in the discharge cell, and a sustain period for generating sustain discharge by alternately applying sustain pulses to the scan electrode and sustain electrode of the discharge cell, and rise time of the sustain pulses to be applied to the scan electrode and sustain electrode during the sustain period is shortened at a frequency of once every several times.
    • 公开了一种用于驱动等离子体显示面板的方法,其中可以在整个屏幕上减少具有亮度不均匀性的区域的生成,而不改变维持脉冲的电压和脉冲宽度,从而能够抑制功耗的增加。 用于驱动等离子体显示面板的方法包括用于在扫描电极和维持电极与数据电极相交并在单元中产生初始化放电的交叉处形成放电单元的初始化时段,用于在放电单元中产生写入放电的写入周期,以及 用于通过对维持周期的扫描电极和维持电极交替施加维持脉冲而产生维持放电的维持周期,并且在维持周期期间将被施加到扫描电极和维持电极的维持脉冲的上升时间缩短为频率 每隔几次。
    • 50. 发明授权
    • Liquid crystal display device
    • 液晶显示装置
    • US06816208B2
    • 2004-11-09
    • US09911305
    • 2001-07-23
    • Tetsuo FukamiKatsuhiko KumagawaMasanori Kimura
    • Tetsuo FukamiKatsuhiko KumagawaMasanori Kimura
    • G02F11368
    • G02F1/134363G02F1/136213
    • This is an active matrix liquid crystal display device comprising a capacitive accumulation portion formed by overlapping a pixel electrode, an insulating layer and a common electrode for each pixel area, and a non-electrode area in a part of the pixel area which is not covered with a pixel electrode, wherein a peripheral shape of said capacitive accumulation portion on a side contacting said non-electrode area is substantially the same between the respective pixels, and a value of a storage capacity in said capacitive accumulation portion differs on a feeding side and on a termination side, the value on the feeding side being larger than the value on the termination side. Thereby, a constant aperture ratio can be maintained by changing the storage capacity value for each pixel. Furthermore, by using a lateral electric field method liquid crystal display device, the storage capacity value can be changed while maintaining the aperture ratio of the pixel constant, and the electric fields applied to the liquid crystal layer in the display portion can be kept evenly. As a result, deterioration and unevenness of display characteristics do not occur. Moreover, even in the case of using a light shield film to improve contrast and so forth, a light shield film with a narrower width than that in a conventional configuration can be used, so that the aperture ratio does not drop drastically.