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    • 4. 发明授权
    • Magnetic resonance imaging system
    • 磁共振成像系统
    • US5343149A
    • 1994-08-30
    • US94916
    • 1993-07-22
    • Masatoshi Hanawa
    • Masatoshi Hanawa
    • A61B5/055G01R33/36G01R33/46G01R33/58G01V3/00
    • G01R33/583
    • In a magnetic resonance imaging system having an automatic power control function for adjusting the transmission power of an RF pulse so as to set a desired flip angle of a spin, in an automatic power control mode, a plane including only a portion of an object to be examined in an imaging region having a uniform field intensity, e.g., a transaxial plane or a plane slightly inclined from the transaxial plane is excited by a gradient magnetic field Gz in the direction of the body axis of the object as a slice gradient magnetic field regardless of a plane to be imaged. The peak values of MR echo signals are detected while the transmission power of the RF pulse is changed. An RF pulse transmission power at which the maximum peak value appears is detected from these detection values. The transmission power of the RF pulse in imaging, i.e., the output of an RF oscillator having a predetermined frequency, is attenuated on the basis of the relationship between the transmission power and the maximum peak value, thereby adjusting the attenuation amount of an attenuator for supplying a current to an RF coil.
    • 在具有自动功率控制功能的磁共振成像系统中,在自动功率控制模式中,用于调整RF脉冲的发射功率以便设定期望的旋转翻转角度,将仅包括对象的一部分的平面 在具有均匀场强的成像区域中进行检查,例如横轴平面或从轴向平面稍微倾斜的平面被作为切片梯度磁场的物体的轴线方向上的梯度磁场Gz激发 不管要成像的飞机。 当RF脉冲的发送功率改变时,检测MR回波信号的峰值。 从这些检测值检测出出最大峰值的RF脉冲发送功率。 基于发送功率和最大峰值之间的关系,成像中的RF脉冲的发送功率,即具有预定频率的RF振荡器的输出被衰减,从而调整衰减器的衰减量 向RF线圈提供电流。
    • 5. 发明授权
    • Coil system for magnetic resonance imaging
    • 用于磁共振成像的线圈系统
    • US4767993A
    • 1988-08-30
    • US75758
    • 1987-07-20
    • Masatoshi Hanawa
    • Masatoshi Hanawa
    • A61B5/055G01R33/341G01R33/36G01R33/56G01R33/20
    • G01R33/3678G01R33/56
    • A coil system for magnetic resonance imaging in a magnetic resonance imaging system, used to transmit the excitation pulse and to receive the magnetic resonance signals, includes a first coil for transmitting a predetermined high-frequency pulse, second and third coils, arranged on a propagation path of the magnetic resonance signal at a position closer to the object to be examined than the first coil in directions orthogonal to each other, for receiving the magnetic resonance signals, and a pair of tuning elements, respectively provided in association with the second and third coils, for tuning the second and third coils to predetermined magnetic resonance signals. The tuning elements tune the second and third coils slightly offset from accurate tuning points so that voltage phases of the magnetic resonance signals received through the second and third coils coincide with each other.
    • 用于磁共振成像系统中用于发射激励脉冲并接收磁共振信号的磁共振成像用线圈系统包括用于传输预定的高频脉冲,第二和第三线圈的第一线圈,布置在传播 在与第一线圈相对的方向上相对于被检查物体的位置处的磁共振信号的路径相对于彼此正交的方向,用于接收磁共振信号;以及一对调谐元件,分别与第二和第三 线圈,用于将第二和第三线圈调谐到预定的磁共振信号。 调谐元件调谐第二和第三线圈稍微偏离精确的调谐点,使得通过第二和第三线圈接收的磁共振信号的电压相位彼此一致。
    • 9. 发明授权
    • MR imaging using mutual interaction between different kinds of pools of
nuclear spins
    • MR成像使用不同种类的核旋转池之间的相互作用
    • US6023634A
    • 2000-02-08
    • US618859
    • 1996-03-20
    • Masatoshi HanawaMitsue MiyazakiYoshimori Kassai
    • Masatoshi HanawaMitsue MiyazakiYoshimori Kassai
    • G01R33/54A61B5/055
    • G01R33/54
    • In addition to the known MT (magnetization transfer) effect, an RMT (reverse MT) is newly found, which increases a detected MR signal strength. Both the MT and RMT effects can be explained with mutual interaction, such as phenomena of chemical exchange and/or cross relaxation, acted between a pool of water proton spins and another pool of macromolecule proton spins, for example, within an object. In order to enhance the MT or RMT effect, the frequency bandwidths of RF pulses, such as a 90.degree. RF exciting pulse in a SE or FSE method, an inversion pulse in a FLAIR or fast FLAIR method, and others, are controlled. To enhance the MT effect, the bandwidth is controlled into a wider value (approx. more than 1250 Hz) than the normally (conventionally) used bandwidth, while to obtain the RMT effect, the bandwidth is controlled into a narrower value (approx. less than 1000 Hz) than the normally used bandwidth. Actively controlling the MT or RMT effect permits changed image contrast in MR imaging.
    • 除了已知的MT(磁化传递)效应之外,新发现RMT(反向MT),这增加了检测到的MR信号强度。 MT和RMT效应都可以通过相互作用(例如化学交换和/或交叉松弛的现象)来解释,这些现象在水质子旋转池和另一个大分子质子自旋池之间起作用,例如在物体内。 为了提高MT或RMT效应,可以控制RF脉冲的频率带宽,例如SE或FSE方法中的90°RF激励脉冲,FLAIR或快速FLAIR方法中的反转脉冲等。 为了提高MT效应,带宽被控制在比正常(常规)使用的带宽更宽的值(大于1250Hz)的同时,为了获得RMT效应,带宽被控制在较小的值(大约少于 超过1000 Hz)比正常使用的带宽。 积极控制MT或RMT效果可以改善MR成像中的图像对比度。
    • 10. 发明授权
    • Magnetic resonance imaging system
    • 磁共振成像系统
    • US5051699A
    • 1991-09-24
    • US400059
    • 1989-08-29
    • Masatoshi HanawaKazuto Nakabayashi
    • Masatoshi HanawaKazuto Nakabayashi
    • G01R33/485G01R33/565
    • G01R33/56527G01R33/485
    • A magnetic resonance imaging system includes a static magnetic field generating section, a gradient magnetic field applying section, an RF pulse applying section, a sequence control section, a receiving section, and an imaging processing section. The sequence control section causes an RF pulse to excite magnetic resonance, causes at least one of the RF pulse and the gradient field to produce an initial magnetic resonance echo, applies a read gradient field to the imaging volume upon reception of the magnetic resonance echo, and inverts the read gradient field at least once to produce at least one magnetic resonance echo in addition to the initial magnetic resonance echo. The receiving section adds and averages data of a plurality of such magnetic resonance echoes or performs an addition or subtraction of the magnetic resonance echoes.
    • 磁共振成像系统包括静磁场产生部分,梯度磁场施加部分,RF脉冲施加部分,序列控制部分,接收部分和成像处理部分。 序列控制部分使RF脉冲激发磁共振,使RF脉冲和梯度场中的至少一个产生初始磁共振回波,在接收到磁共振回波时将读取的梯度场应用于成像体积, 并且将读取的梯度场反转至少一次以产生除了初始磁共振回波之外的至少一个磁共振回波。 接收部分添加并平均多个这样的磁共振回波的数据,或执行磁共振回波的加法或减法。