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    • 4. 发明授权
    • Process and apparatus for grain-sizing in alumina hydrate slurry
    • 在水合氧化铝浆料中的粒度调整方法和设备
    • US4816142A
    • 1989-03-28
    • US7122
    • 1987-01-27
    • Gyula OdorFrigyes CsapoBela SzaboLajos SzucsMihaly MartonJanso SteinerLaszlo ReveszFerenc TothFerenc Weiszengruber
    • Gyula OdorFrigyes CsapoBela SzaboLajos SzucsMihaly MartonJanso SteinerLaszlo ReveszFerenc TothFerenc Weiszengruber
    • B01D19/02B03B5/62C01F7/02C01F7/14C01F7/46
    • C01F7/46B01D19/02B03B5/623C01F7/021C01F7/148C01P2004/03C01P2004/51C01P2004/61
    • According to the invention, the grains of the hydrate slurry are separated by sedimentation where the dispersed bubbles of air are removed in course of the presizing, then a supplementary sizing is carried out. Preferably, a liquid free from hydrate grains is fed in to stream against the sinking grains. This liquid is advantageously the spent liquor of the hydrate filter. The apparatus according to the invention consists of a container with conical bottom, a feeding device, a slurry outlet stub and an overflow channel. The inlet stubs of the feeding device, however, are placed off-center and every stub is connected with a presizing equipment. This equipment is composed of a bundle of pipes and/or a pack of plates which are slop placed to geometrical axis: At the upper part of the presizing equipment there is a foam overflow apparatus. The bottom of each presizing equipment is connected with a common cone-frustum type deflector casing. The casing is concentric with the container. There is ring shape gap between the upper edge of the deflector casing and the cylinder jacket of the container. Under the deflector casing there is an upwards convex control cone. The control cone is vertically adjustable and concentric with the deflector casing.
    • 根据本发明,通过沉淀分离水合物浆料的颗粒,其中在预定过程中除去分散的空气气泡,然后进行补充施胶。 优选地,将不含水合物颗粒的液体加入到沉没颗粒中。 该液体有利地是水合物过滤器的废液。 根据本发明的装置由具有锥形底部的容器,进料装置,浆料出口短管和溢流通道组成。 然而,进料装置的入口短柱放置在偏心处,每个短截线与预设装置连接。 该设备由一排管道和/或一组板条组成,这些管道几何轴线是倾斜的:在预设设备的上部有一个泡沫溢流装置。 每个预设设备的底部与普通锥形截头锥型偏转器外壳连接。 外壳与容器同心。 在偏转器壳体的上边缘和容器的气缸套之间存在环形间隙。 在偏转器外壳下面有一个向上凸的控制锥。 控制锥体可垂直调节,与导流罩同心。
    • 5. 发明授权
    • Method for determining charged energy states of semiconductor or
insulator materials by using deep level transient spectroscopy, and an
apparatus for carrying out the method
    • 通过使用深层瞬态光谱法确定半导体或绝缘体材料的带电能态的方法,以及用于执行该方法的装置
    • US4571541A
    • 1986-02-18
    • US439226
    • 1982-11-04
    • Gyorgy FerencziJanos BodaFerenc TothPeter HorvathLaszlo BenkovicsLaszlo Dozsa
    • Gyorgy FerencziJanos BodaFerenc TothPeter HorvathLaszlo BenkovicsLaszlo Dozsa
    • G01N27/00G01R31/26G01R31/28H01L21/66
    • G01R31/2831
    • A method for determining charged energy states of a sample of a semiconductor or insulator material by using deep level transient spectroscopy. The method includes the steps of exciting the sample by application of periodical exciting pulses to change the initial charge state, detecting the transient response of the sample when it returns to the thermodynamical balance condition following the termination of each of the excitation pulses, blocking the detection during a blocking period defined as the combined existence of the exciting pulses and of a dead period including the recovery period of the means used for the detection, performing a weighted integration operation on a detected response signal by the application of a symmetrical square wave synchronizing pulse as a weighting function synchronized to the frequency of said exciting pulses, blocking the detection in each of said detecting periods for the duration of a further blocking period which begins in a moment defined between the starting moments of the two exciting pulses immediately preceding and following said detecting period and synchronizing the synchronizing pulses to terminating moments of said dead periods to have a period time which is equal to the period time of said periodical exciting pulses. Apparatus for carrying out the method is also disclosed.
    • 一种通过使用深层瞬态光谱法确定半导体或绝缘体材料样品的带电能态的方法。 该方法包括以下步骤:通过施加周期激励脉冲来激发样品以改变初始电荷状态,当样品在每个激发脉冲终止后返回到热力学平衡条件时检测样品的瞬态响应,阻止检测 在被定义为激励脉冲的组合存在和包括用于检测的装置的恢复周期的死区的阻塞期间中,通过应用对称的方波同步脉冲对检测到的响应信号执行加权积分运算 作为与所述激励脉冲的频率同步的加权函数,在每个所述检测周期内阻止在另一阻塞周期的持续时间内的检测,该进一步的阻塞周期从紧接在所述激励脉冲之前和之后的两个激励脉冲的起始时刻之间限定的时刻开始 检测周期并同步同步pu 导致所述死区的终止时刻具有等于所述周期激励脉冲的周期时间的周期时间。 还公开了用于执行该方法的装置。