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    • 2. 发明授权
    • Process for producing single-crystal semiconductor and apparatus for producing single-crystal semiconductor
    • 单晶半导体的制造方法及单晶半导体的制造装置
    • US07235128B2
    • 2007-06-26
    • US11005180
    • 2004-12-06
    • Susumu MaedaHiroshi InagakiShigeki KawashimaShoei KurosakaKozo Nakamura
    • Susumu MaedaHiroshi InagakiShigeki KawashimaShoei KurosakaKozo Nakamura
    • C30B15/20
    • C30B29/06C30B15/20C30B15/22C30B15/36Y10S117/90Y10T117/1004
    • A process for producing a single-crystal semiconductor and an apparatus therefor. A single-crystal semiconductor of large diameter and large weight can be lifted with the use of existing equipment not having any substantial change thereto while not influencing the oxygen concentration of single-crystal semiconductor and the temperature of melt and while not unduly raising the temperature of seed crystal. In particular, the relationship (L1, L2, L3) between the allowable temperature difference (ΔT) and the diameter (D) of seed crystal (14) is preset so that the temperature difference between the seed crystal (14) at the time the seed crystal (14) is immersed in the melt and the melt (5) falls within the allowable temperature difference (ΔT) at which dislocations are not introduced into the seed crystal (14). In accordance with the relationship (L1, L2, L3), the allowable temperature difference (ΔT) corresponding to the diameter (D) of seed crystal (14) to be immersed in the melt is determined. Temperature control is conducted so that at the time the seed crystal (14) is immersed in the melt (5) the temperature difference between the seed crystal (14) and the melt (5) falls within the determined allowable temperature difference (ΔT).
    • 一种单晶半导体的制造方法及其装置。 可以使用不具有任何显着变化的现有设备来提升大直径和大重量的单晶半导体,同时不影响单晶半导体的氧浓度和熔体的温度,同时不会过度地提高温度 晶种。 特别地,预设晶种(14)的允许温差(DeltaT)和直径(D)之间的关系(L 1,L 2,L 3),使得晶种(14)在 籽晶(14)浸入熔体中的时间和熔体(5)落入未被引入到晶种(14)中的位错的允许温度差(DeltaT)之内。 根据关系(L 1,L 2,L 3),确定与浸入熔体中的晶种(14)的直径(D)相对应的容许温度差(DeltaT)。 进行温度控制,使晶种(14)浸入熔融物(5)中时晶种(14)和熔体(5)之间的温度差落在确定的允许温差(DeltaT)之内。
    • 3. 发明申请
    • Method for producing silicon wafer
    • 硅晶片的制造方法
    • US20060005762A1
    • 2006-01-12
    • US10533147
    • 2003-10-31
    • Susumu MaedaHiroshi InagakiShigeki KawashimaShoei KurosakaKozo Nakamura
    • Susumu MaedaHiroshi InagakiShigeki KawashimaShoei KurosakaKozo Nakamura
    • C30B15/00C30B21/06C30B23/00C30B30/04C30B27/02
    • C30B29/06C30B15/203
    • The present invention is to produce a silicon crystal wherein the boron concentration in the silicon crystal and the growth condition V/G are controlled so that the boron concentration in the silicon crystal is no less than 1×1018 atoms/cm3 and the growth condition V/G falls within the epitaxial defect-free region α2 whose lower limit line LN1 is the line indicating that the growth rate V gradually drops as the boron concentration increases. Further, the present invention is to produce a silicon wafer wherein the boron concentration in the silicon crystal and the growth condition V/G are controlled so as to include at least the epitaxial defect region β1, and the heat treatment condition of the silicon crystal and the oxygen concentration in the silicon crystal are controlled so that no OSF nuclei grow to OSFs. Moreover, the present invention is to produce a silicon crystal wherein the boron concentration in the silicon crystal and the growth condition V/G are controlled so that they fall in the vicinity of the lower limit line LN3 within the epitaxial defect-free region α1.
    • 本发明是为了制造硅晶体,其中硅晶体中的硼浓度和生长条件V / G被控制,使得硅晶体中的硼浓度不低于1×10 18原子/ cm 3,并且生长条件V / G落在外延无缺陷区域α2N中,其下限线LN1是表示生长速率V逐渐下降的线 硼浓度增加。 此外,本发明是为了制造硅晶片,其中硅晶体中的硼浓度和生长条件V / G被控制为至少包括外延缺陷区β1,并且 控制硅晶体的热处理条件和硅晶体中的氧浓度,使得OSF核不生长到OSF。 此外,本发明是为了制造硅晶体,其中硅晶体中的硼浓度和生长条件V / G被控制为使得它们落入外延缺陷区域内的下限线LN3附近, SUB> 1
    • 4. 发明申请
    • Process for producing single-crystal semiconductor and apparatus for producing single-crystal semiconductor
    • 单晶半导体的制造方法及单晶半导体的制造装置
    • US20050139149A1
    • 2005-06-30
    • US11005180
    • 2004-12-06
    • Susumu MaedaHiroshi InagakiShigeki KawashimaShoei KurosakaKozo Nakamura
    • Susumu MaedaHiroshi InagakiShigeki KawashimaShoei KurosakaKozo Nakamura
    • C30B15/00C30B15/20C30B15/22C30B15/36C30B29/06C30B21/06C30B27/02C30B28/10C30B30/04
    • C30B29/06C30B15/20C30B15/22C30B15/36Y10S117/90Y10T117/1004
    • A process for producing a single-crystal semiconductor and an apparatus therefor. A single-crystal semiconductor of large diameter and large weight can be lifted with the use of existing equipment not having any substantial change thereto while not influencing the oxygen concentration of single-crystal semiconductor and the temperature of melt and while not unduly raising the temperature of seed crystal. In particular, the relationship (L1, L2, L3) between the allowable temperature difference (ΔT) and the diameter (D) of seed crystal (14) is preset so that the temperature difference between the seed crystal (14) at the time the seed crystal (14) is immersed in the melt and the melt (5) falls within the allowable temperature difference (ΔT) at which dislocations are not introduced into the seed crystal (14). In accordance with the relationship (L1, L2, L3), the allowable temperature difference (ΔT) corresponding to the diameter (D) of seed crystal (14) to be immersed in the melt is determined. Temperature control is conducted so that at the time the seed crystal (14) is immersed in the melt (5) the temperature difference between the seed crystal (14) and the melt (5) falls within the determined allowable temperature difference (ΔT).
    • 一种单晶半导体的制造方法及其装置。 可以使用不具有任何显着变化的现有设备来提升大直径和大重量的单晶半导体,同时不影响单晶半导体的氧浓度和熔体的温度,同时不会过度地提高温度 晶种。 特别地,预设晶种(14)的允许温差(DeltaT)和直径(D)之间的关系(L 1,L 2,L 3),使得晶种(14)在 籽晶(14)浸入熔体中的时间和熔体(5)落入未被引入到晶种(14)中的位错的允许温度差(DeltaT)之内。 根据关系(L 1,L 2,L 3),确定与浸入熔体中的晶种(14)的直径(D)相对应的允许温度差(DeltaT)。 进行温度控制,使晶种(14)浸入熔融物(5)中时晶种(14)和熔体(5)之间的温度差落在确定的允许温差(DeltaT)之内。
    • 7. 发明申请
    • STATOR WINDING OF ELECTRICAL ROTATING MACHINE
    • 电动旋转机定子绕组
    • US20140346914A1
    • 2014-11-27
    • US14372226
    • 2012-04-19
    • Yoichi FunasakiKiyonori KogaSusumu Maeda
    • Yoichi FunasakiKiyonori KogaSusumu Maeda
    • H02K3/28
    • H02K3/28
    • In a three-phase, four-pole, four-parallel-circuit stator winding of an electrical rotating machine, each of two sets of U-phase output terminals U1, U2 is formed of two sets of parallel circuits each formed of windings having a same pitch (one is formed of first and second winding circuits 1, 2 and the other is formed of third and fourth winding circuits 3, 4). The winding of each winding circuit is formed of two serially-connected coil phase bands (coil phase bands a and b form the first winding circuit 1 and coil phase bands c and d, coil phase bands e and f, and coil phase bands g and h form the second, third, and fourth winding circuits 2, 3, 4, respectively). A voltage vector phase difference and a voltage difference between the winding circuits can be eliminated without providing a jumper wire to winding end portions.
    • 在旋转电机的三相四极并联电路定子绕组中,两组U相输出端子U1,U2中的每一组由两组并联电路组成,每组由具有 相同的间距(一个由第一和第二绕组电路1,2形成,另一个由第三和第四绕组电路3,4组成)。 每个绕组电路的绕组由两个串联的线圈相位带(线圈相位带a和b形成第一绕组电路1和线圈相位带c和d,线圈相位​​带e和f以及线圈相位带g和 h分别形成第二,第三和第四绕组电路2,3,4)。 可以消除绕组电路之间的电压矢量相位差和电压差,而不向绕组端部提供跨接线。