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    • 23. 发明申请
    • Antenna selection diversity apparatus and receiving method
    • 天线选择分集装置和接收方法
    • US20060234776A1
    • 2006-10-19
    • US10544388
    • 2004-11-04
    • Yoshiharu IshiharaYasushi IwataToshio Obara
    • Yoshiharu IshiharaYasushi IwataToshio Obara
    • H04B1/02H04M1/00H04B7/02
    • H04B7/0874
    • An antenna selection diversity apparatus capable of shortening, when antennas are switched in frame units, a measuring time of antennas and shortening the time of selecting an optimal antenna from among a plurality of antennas on standby. In this apparatus, an antenna selection section (109) selects one of three antennas as an antenna in actual use for a period of a plurality of frames consecutively according to selection priority stored in an antenna information storage section (108) and gives an instruction for selecting one of two antennas on standby as an antenna to be measured once at a period of a plurality of frames to an antenna selection switch (104). When the reception level of the antenna in actual use measured by a reception level measuring section (107) falls below the reception level of the antenna to be measured a predetermined number of times consecutively, the antenna selection section (109) gives an instruction for selecting the antenna to be measured as the antenna in actual use to the antenna selection switch (104).
    • 一种天线选择分集装置,其能够在天线以帧为单位进行切换时缩短天线的测量时​​间,并且缩短从待机状态的多个天线中选择最佳天线的时间。 在该装置中,天线选择部(109)根据存储在天线信息存储部(108)中的选择优先级,连续选择多个帧的周期的实际使用中的三个天线中的一个天线,并给出指令 选择待机状态下的两个天线中的一个天线作为在多个帧的周期被测量一次的天线到天线选择开关(104)。 当由接收电平测量部分(107)测量的实际使用的天线的接收电平连续地下降到预定次数以下的待测天线的接收电平时,天线选择部(109)给出选择指令 要测量的天线作为实际使用的天线到天线选择开关(104)。
    • 26. 发明申请
    • CRANKCASE FOR INTERNAL COMBUSTION ENGINE
    • 内燃机起动机构
    • US20090188478A1
    • 2009-07-30
    • US12358290
    • 2009-01-23
    • Tatsuhiro TERADAYasushi Iwata
    • Tatsuhiro TERADAYasushi Iwata
    • F02B25/06
    • F02M25/06Y02T10/121
    • A crankcase that is provided in an internal combustion engine, in which blow-by gas is returned to an intake passage via a gas outflow passage formed in a cylinder block so as to extend in a direction from an upper portion to a lower portion of the cylinder, includes: a partition wall extending in a direction from an upper portion to a lower portion of the crankcase and facing an inner side surface of a crankcase outer wall that also extends in the direction from the upper portion to the lower portion of the crankcase; an internal space that is formed between the partition wall and the inner side surface of the crankcase outer wall and connected to the gas outflow passage at an upper end of the internal space; and a window that is formed on the partition wall to communicate an inside and outside of the internal space.
    • 一种设置在内燃机中的曲轴箱,其中窜气通过形成在气缸体中的气体流出通道返回到进气通道,以便在从上部到下部的方向上延伸 气缸,包括:在从曲轴箱的上部到下部的方向上延伸并且面向曲轴箱外壁的内侧表面的分隔壁,其也在从曲轴箱的上部到下部的方向上延伸 ; 所述内部空间形成在所述分隔壁与所述曲轴箱外壁的内侧面之间,并且在所述内部空间的上端与所述气体流出通道连接; 以及窗口,其形成在所述分隔壁上以连通所述内部空间的内部和外部。
    • 27. 发明申请
    • CLUSTER FILM FORMATION SYSTEM AND FILM FORMATION METHOD, AND CLUSTER FORMATION SYSTEM AND FORMATION METHOD
    • 聚集体膜形成系统和膜形成方法,以及聚集体形成系统和形成方法
    • US20090114848A1
    • 2009-05-07
    • US12096703
    • 2006-12-07
    • Yasushi IwataToshio Takiya
    • Yasushi IwataToshio Takiya
    • A61N5/00
    • C23C14/28C23C14/228
    • The invention provides a cluster film formation system in which, in a cluster formation container 5, target 1 is irradiated with laser beams 2 to generate material vapor, which generates a shock wave 4 of an inert gas, and the shock wave 4 is reflected by a wall of the cluster formation container 5 to confine the material vapor having progressed in a particular region, and atoms or molecules of the material vapor and the inert gas collide with each other mutually to form groups of clusters, which are made to flow out through an outflow window 7, and sprayed deposited on a substrate 9 to form a cluster film 10. Corresponding to augmentation of energy strength of the laser beams 2, a cross section area of the laser beams 2 on the surface of the target is made large, thereby an increase in the amount of generation of the material vapor and efficient generation of the shock wave of the inert gas both are realized, and at the same time, the cluster formation container is enlarged so that the reflected wave of the shock wave meets conditions for confining the material vapor.
    • 本发明提供一种簇成膜系统,其中在簇形成容器5中,用激光束2照射靶1以产生材料蒸汽,其产生惰性气体的冲击波4,并且冲击波4被反射 簇形成容器5的壁,用于限制在特定区域中进行的材料蒸气,以及材料蒸气和惰性气体的原子或分子彼此相互碰撞,以形成一组簇,其被排出通过 流出窗口7,并喷涂在基板9上以形成簇膜10.对应于激光束2的能量强度的增加,激光束2在目标表面上的横截面面积变大, 从而实现了材料蒸气的产生量的增加,并且实现了惰性气体的冲击波的有效产生,并且同时使集束形成容器扩大,使得 冲击波的反射波符合限制材料蒸气的条件。
    • 28. 发明授权
    • Storage device
    • 储存设备
    • US07137438B2
    • 2006-11-21
    • US10499678
    • 2002-12-27
    • Satoshi NomuraYuuichi MinamiyamaIchiro FurihataKenji KunoYasushi Iwata
    • Satoshi NomuraYuuichi MinamiyamaIchiro FurihataKenji KunoYasushi Iwata
    • A47F3/04
    • F25D25/02A47F3/0443A47F2003/046F25D2317/0665
    • A storage apparatus is provided that comprises a display case part with an inside thereof being dividable into a plurality of zones, a supply duct that is connected to supply openings for supplying conditioning air for controlling environmental conditions to the plurality of zones respectively, and an exhaust duct that is connected to exhaust openings for taking in air from the plurality of zones. In this storage apparatus, conditioning air such as cold air or hot air is circulated in the respective zones, and the environmental conditions can be adjusted efficiently in zone basis. Therefore, in a storage apparatus equipped with an open-type display case part, it is possible to dispense with an air curtain covering the entire open side, so that a storage apparatus with a high storage capacity is provided.
    • 一种存储装置,包括:显示壳体部分,其内部可分为多个区域;供应管道,连接到供应开口,分别用于向多个区域提供用于控制环境条件的调节空气;排气口 管道,其连接到用于从多个区域吸入空气的排气口。 在这种存储装置中,诸如冷空气或热空气的调节空气在各个区域中循环,并且可以基于区域有效地调整环境条件。 因此,在具有开放式显示壳体部件的存储装置中,可以省略覆盖整个开放侧的气幕,从而提供具有高存储容量的存储装置。
    • 29. 发明授权
    • Automatic gain control method and device
    • 自动增益控制方法及装置
    • US06745016B2
    • 2004-06-01
    • US10357744
    • 2003-02-04
    • Yasushi IwataYasufumi Ichikawa
    • Yasushi IwataYasufumi Ichikawa
    • H04B106
    • H03G3/3078H03G3/30H03G3/3052
    • A constant output signal can be achieved by controlling a gain variable amplifier 2 based on a level of an output signal which is derived by variably amplifying a receiving signal S1 (input signal). An AGC output signal S11 is detected by a detector circuit 3. Then, a CPU 5 generates a control signal S8 based on a detected voltage signal S7. An RSSI detector portion 9 detects an RSSI signal S10 corresponding to a transmitting signal level from the receiving signal S1. The transmitting signal level is compared to a preceding transmitting signal level. The control signal from a preceding execution of the gain control is output if the present control signal is lower than the preceding control signal and the present transmitting signal level is reduced below the preceding transmitting signal level.
    • 可以通过基于通过可变地放大接收信号S1(输入信号)导出的输出信号的电平来控制增益可变放大器2来实现恒定输出信号。 AGC输出信号S11由检测器电路3检测。然后,CPU 5基于检测到的电压信号S7产生控制信号S8。 RSSI检测部9从接收信号S1检测与发送信号电平对应的RSSI信号S10。 将发送信号电平与先前的发送信号电平进行比较。 如果当前控制信号低于先前控制信号并且当前发送信号电平降低到先前发送信号电平以下,则输出来自执行增益控制的控制信号。
    • 30. 发明授权
    • Particle selection method and a time-of flight mass spectrometer
    • 粒子选择方法和飞行时间质谱仪
    • US5962849A
    • 1999-10-05
    • US826311
    • 1997-03-25
    • Naoaki SaitoMitsumori TanimotoKazuyoshi KoyamaYasushi Iwata
    • Naoaki SaitoMitsumori TanimotoKazuyoshi KoyamaYasushi Iwata
    • G01N27/62H01J49/40G01D59/44H01J49/00
    • H01J49/40
    • In the time-of-flight mass spectrometer, the mass spectrometer with high resolution is provided which defines the initial position and the initial velocity of the charged particles and selects only the stable charged particles to measure.First, all of the charged particles Pe are accelerated to one direction in a homogeneous or spatially uniform electric field during a common finite period of time, and then all of the charged particles Pe are accelerated to the opposite direction of the former in a homogeneous or spatially uniform electric field during a common finite period of time and given the same momentum in the opposite direction of the former. Two kind of particle selection method can be adopted. Only the charged particles Pe passing through a predetermined position at a predetermined time are selected by the selector. The charged particles Pe passing through the selector are defected by the first and second deflectors and then only the charged particles passing through a predetermined point of the slit are selected and reach the ion detector. Finally, the mass spectrum is obtained by measuring the time-of-flight of the particles using the ion detector.
    • 在飞行时间质谱仪中,提供了具有高分辨率的质谱仪,其定义了带电粒子的初始位置和初始速度,并且仅选择稳定的带电粒子进行测量。 首先,在均匀或空间均匀的电场中,所有带电粒子Pe在均匀或空间均匀的电场中被加速到一个方向,然后所有带电粒子Pe被加速到前者的相反方向, 在相同的有限时间段内空间均匀的电场,并给出与前者相反方向相同的动量。 可采用两种粒子选择方法。 选择器仅选择在预定时间内通过预定位置的带电粒子Pe。 穿过选择器的带电粒子Pe被第一和第二偏转器缺陷,然后仅选择通过狭缝的预定点的带电粒子并到达离子检测器。 最后,通过使用离子检测器测量颗粒的飞行时间来获得质谱。