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    • 84. 发明授权
    • Nuclear magnetic resonance imaging apparatus
    • 核磁共振成像装置
    • US4889127A
    • 1989-12-26
    • US37855
    • 1987-04-13
    • Ryuzaburo TakedaHideaki KoizumiYoshiyuki Miyamoto
    • Ryuzaburo TakedaHideaki KoizumiYoshiyuki Miyamoto
    • A61B10/00A61B5/055G01R33/48G01R33/563
    • G01R33/563
    • A nuclear magnetic resonance imaging apparatus for deriving a signal from a moving part of an object to be imaged, includes a gradient magnetic field generator for applying a gradient magnetic field to the object; and a radio frequency magnetic field generator for applying a radio frequency magnetic field to the object to present a nuclear magnetic resonance phenomenon. Pulses of a 180 degree pulse method are generated to remove an adverse effect of ununiformity of a static magnetic field; two gradient magnetic fields having the same amplitude and grading oppositely to each other are applied at a certain time interval therebetween to the moving part of the object in the direction of motion of the moving object; a radio frequency magnetic field is generated by applying a pulse in the pulses of the 180 degree pulse method succeeding a 180 degree pulse at the time corresponding to the center of an echo signal generated by the 180 degree pulse, the radio frequency magnetic field making a nuclear spin vector at the stationary part of the object in parallel to the static magnetic field; a resonance signal is detected which is produced from the object upon application of the radio frequency magnetic field; the above process is performed to further obtain another resonance signal, reversing the polarities of the gradient magnetic fields; and a difference between the two resonance signals is derived as a signal from the moving part of the object.
    • 用于从待成像对象的移动部分导出信号的核磁共振成像装置包括用于向对象施加梯度磁场的梯度磁场发生器; 以及用于对物体施加射频磁场以呈现核磁共振现象的射频磁场发生器。 产生180度脉冲方式的脉冲以消除静磁场不均匀性的不利影响; 以相对于彼此相反的幅度和等级的两个梯度磁场在其间的特定时间间隔被施加到物体的运动部分在运动物体的运动方向上; 通过在对应于由180度脉冲产生的回波信号的中心的时间的180度脉冲之后的180度脉冲方式的脉冲中施加脉冲,产生射频磁场来产生射频磁场, 核自旋矢量在物体的静止部分平行于静磁场; 检测在应用射频磁场时从物体产生的共振信号; 执行上述处理以进一步获得另一谐振信号,反转梯度磁场的极性; 并且导出两个谐振信号之间的差异作为来自物体的运动部分的信号。
    • 85. 发明授权
    • Light source for producing atomic spectral line
    • 用于生产原子光谱线的光源
    • US4562376A
    • 1985-12-31
    • US513316
    • 1983-07-13
    • Hideaki Koizumi
    • Hideaki Koizumi
    • H01J61/09G01N21/01H01J61/52H01J61/70
    • H01J61/523H01J61/70
    • Disclosed is a light source having an envelope containing therein an anode and a hollow cathode, in which the hollow cathode is supported by a hollow metal cylinder. The hollow cylinder externally extends out of the envelope and a plurality of radiation fins are attached on the outer wall of the externally extending portion of the cylinder. Meshes are provided on the inner wall of the hollow chamber of the cylinder. Water is sealed in the hollow chamber under a reduced pressure to facilitate evaporation. The condensed water is displaced toward a high temperature portion by capillarity. The water is evaporated at the high temperature portion while taking away the latent heat of evaporation. In such an arrangement, the cathode is maintained at a low temperature so that the self-absorption of the spectral line can be reduced.
    • 公开了一种光源,其具有包含阳极和中空阴极的外壳,其中空心阴极由中空金属圆筒支撑。 空心圆筒从外壳延伸出来,多个散热片安装在气缸外部延伸部分的外壁上。 网格设置在圆筒的中空室的内壁上。 水在减压下密封在中空室中以促进蒸发。 冷凝水通过毛细作用向高温部位移位。 在高温部分蒸发水分,同时消除蒸发潜热。 在这种布置中,阴极保持在低温,从而可以减小光谱线的自吸收。
    • 87. 发明授权
    • Flameless atomizer
    • 无焰雾化器
    • US4202628A
    • 1980-05-13
    • US781938
    • 1977-03-28
    • Hideaki KoizumiKazuo Moriya
    • Hideaki KoizumiKazuo Moriya
    • G01N21/31G01N21/74G01J3/30
    • G01N21/74G01N2021/151
    • A cuvette used in a flameless atomizer is hollow and includes an opening at both ends and a hole in a radial direction substantially at its central portion. The cuvette is made of a conductive material and Joule-heated by currents flowing therethrough. The interior of the cuvette is divided substantially into three sections: a sample mount section at which a sample introduced through the hole of the cuvette is disposed; a light beam path section through which light incident from the opening at one end of the cuvette passes and goes out of the opening at the other end; and an absorption cell section at which the light beam path section intersects with atomic vapors generated from the sample disposed at the sample mount section. The electric resistance of the cuvette is made smaller at the sample mount section than at a portion near the absorption cell section. This allows the higher temperature of the portions near the absorption cell section than that of the sample mount section. Therefore, almost all of the atomic vapors in the cuvette exist at the absorption cell portion, and the application of a magnetic field to the absorption cell section allows a great improvement in analysis precision and sensitivity of the flameless atomizer for atomic absorption analysis using a Zeeman effect.
    • 在无焰雾化器中使用的比色杯是中空的,并且包括在两端的开口和在径向方向上的大致在其中心部分的孔。 试管由导电材料制成,并由流过其中的电流进行焦耳加热。 试管的内部基本上分为三个部分:样品安装部分,其中设置通过反应杯的孔引入的样品; 光束路径部分,通过所述光束路径部分从所述反应杯的一端处的所述开口入射的光在所述另一端通过并离开所述开口; 以及吸收单元部分,光束路径部分与从设置在样品安装部分处的样品产生的原子蒸汽相交。 在样品安装部分,反应杯的电阻比吸收单元部分附近的电阻小。 这允许吸收单元部分附近的部分的温度高于样品安装部分的温度。 因此,比色皿中的几乎所有的原子蒸汽都存在于吸收单元部分,并且向吸收单元部分施加磁场允许使用塞曼对无焰雾化器进行原子吸收分析的分析精度和灵敏度大大提高 影响。