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    • 44. 发明专利
    • NMR IMAGING APPARATUS
    • JPS61148357A
    • 1986-07-07
    • JP27040584
    • 1984-12-21
    • HITACHI LTD
    • TSUDA MUNETAKAHIGUCHI KAZUTOSHI
    • A61B10/00A61B5/055G01R33/48G01R33/50G01R33/54
    • PURPOSE:To relieve a person to be inspected of a pain with the reduced inspection time of a sample, by applying a series of continuous high frequency magnetic field pulses containing a gradient magnetic field sequentially to the sample to take a plurality of NMR images simultaneously. CONSTITUTION:A system control section 11 is connected to a frequency synthesizer 9 to allow the application of a frequency control signal thereto for the generation of pulse trains as illustrated. Then, a pi pulse is applied with the resonance frequency of 6.375MHz corresponding to the first slicing position. A pi pulse is applied with the resonance frequency of 6.3763MHz corresponding to the second slicing position. Likewise, a pi pulse is applied with the resonance frequency of 6.3776MHz corresponding to the third slicing position and a pipulse done with the resonance frequency of 6.3789MHz corresponding to the fourth slicing position. In this manner, high frequency magnetic field pulses are applied sequentially to take a plurality of NMR images simultaneously thereby relieving a person to be inspected of a pain with a reduced inspection time of the sample.
    • 47. 发明专利
    • NMR IMAGING APPARATUS
    • JPS60149953A
    • 1985-08-07
    • JP481684
    • 1984-01-17
    • HITACHI LTD
    • MATSUI SHIGERUYAMAMOTO ETSUJISHIONO HIDEKIKOUNO HIDEKI
    • A61B10/00A61B5/055G01N24/08G01R33/50
    • PURPOSE:To make it possible to perform the measurement and imaging of a transverse relaxation time (T2) value in a good SN ratio, by using a steady state free precession (SSFP) method. CONSTITUTION:A high frequency pulse with intensity H1 and a width tau is continuously applied to a spin system at time intervals T sufficiently shorter than T1 but about 1/4 times of T2. In this case, for example, in order to selectively obtain only the signal in a plane of Z=Z0, a vibration magnetic field gradient G is applied in a Z-direction as shown by the drawing (d) and, in order to further obtain the projected image of the intra-plane signal selected as shown by the drawing (c) toward various directions in an XY-plane, a rotary magnetic field gradient GXY is applied in the XY-plane. At this time, a signals appearing steadily directly after and before the high frequency pulse are independently added at a high speed and data processing such as Fourier conversion or reverse projection is performed. If the ratio of two obtained images is taken, because T is known, the image of a T2-value can be obtained by using formula (wherein S+ and S- are signals similar directly after and before the high frequency pulse).
    • 48. 发明专利
    • INSPECTION METHOD AND APPARATUS BY NUCLEAR MAGNETIC RESONANCE
    • JPS59231438A
    • 1984-12-26
    • JP10578483
    • 1983-06-15
    • YOKOGAWA HOKUSHIN ELECTRIC
    • IWAOKA HIDETOSUGIYAMA SUNAOMATSUURA HIROYUKI
    • A61B10/00A61B5/055G01R33/48G01R33/50G01R33/561G01N24/08
    • PURPOSE:To calculate transition times T1 and T2 simply with the magnetization M forcibly turned in the Z' direction by determining at least one 2-D and/or 3-D image of a spin-lattice transition time T1, a spin-spin transition time T2 and a nuclear density from intensity values of a plurality of nuclear magnetic resonance signals through an inter-image computation. CONSTITUTION:A control circuit 2 of a static magnetic field coil 1 contains, for example, a DC stabilization power source. A grade magnetic field coil 3 contains a Z grade magnetic field coil 31, (y) grade magnetic field coils 32 and 33 and an (x) grade magnetic field coil which is the same in the shape as (y) grade magnetic field coils 32 and 33 not illustrated and set turned by 90 deg.. This grade magnetic field coil generates a magnetic field having straight grade respectively in the (x), (y) and (z) axis directions by a magnetism in the same direction as an even static magnetic field H0. Numeral 60 indicates the controller of a control circuit 4. An excitation coil 5 gives a body to be inspected an RF pulse of a fine frequency spectrum (f) as an electromagnetic wave. A detection coil 7 for detecting an NMR resonance signal in the body being detected is the same as the excitation coil and is set turned by 90 deg. with respect to the excitation coil 5. Thus, when energization is forcibly returned to the normal using a pulse series after applied, the transition times T1 and T2 and the proton density M can be determined simply by a computation observing the current intensity of the NMR signal.