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    • 2. 发明专利
    • MAGNETIC RESONANCE IMAGING METHOD
    • JPH0788103A
    • 1995-04-04
    • JP17070494
    • 1994-07-22
    • HITACHI LTDHITACHI MEDICAL CORP
    • HIRATA TOMOTSUGUBITO YOSHITAKAYAMAMOTO ETSUJI
    • G01R33/32A61B5/055G01R33/48
    • PURPOSE:To provide the magnetic resonance imaging method by which the spatial resolution and the spectral band can be set independently. CONSTITUTION:To a pre-stage of the sequence of a high speed MRSI method (magnetic resonance spectroscopic imaging method), a first to a third steps are added, and with regard to substance A, B whose chemical shifts are different from each other, an excitation of a nuclear spin and a measurement of a magnetic resonance signal are executed, and at the time of single echo train signal measurement, a spectral band is narrowed. In a first stage, a high frequency magnetic field of a center frequency (fa) (the frequency band is (fb-fa), and (fa) and (fb) denote resonance frequencies of A and B) and a slice selection gradient magnetic field Gz are applied simultaneously, and the unclear spin of A in a slice, and the unclear spin of B outside of the slice are excited. In a second stage, the high frequency magnetic field whose phase is inverted by 180 deg.C, and the Gz whose gradient polarity is inverted are applied simultaneously, the unclear spin in the slice is restored forcibly to its original thermal equilibrium state, and the unclear spin of B outside of the slice is set to an exciting state. In a third stage, spoil gradient magnetic fields Gz, Gx and Gy are applied simultaneously, and the unclear spin of B being in an exciting state is set to a pseudo-saturated state. In such a way, chemical shift information is obtained by a high speed high resolution.
    • 5. 发明专利
    • FLOW RATE IMAGING METHOD BY MRI DEVICE
    • JPH0947439A
    • 1997-02-18
    • JP20065995
    • 1995-08-07
    • HITACHI LTDHITACHI MEDICAL CORP
    • TAKEUCHI FUMIYATANIGUCHI AKIRABITO YOSHITAKAYAMAMOTO ETSUJIOKAJIMA KENICHI
    • G01P5/20A61B5/055
    • PROBLEM TO BE SOLVED: To reduce artifact and measure flow rate accurately and in a short time, by constituting images of echo signals including and not-including phase modulation of magnetization due to flow, and by determining phase and arithmetically operating. SOLUTION: An echo signal which is generated by inverting polarity of amplitude of a lead-out gradient magnetic field is measured and complex images Ie 1, Ic 1 are obtained from an echo signal line Se 1 which includes phase modulation or magnetization due to flow and from the echo signal line Sc 1 which does not includes that. Secondly, the echo signal line which is generated by inverting polarity or amplitude of a lead-out gradient magnetic field is measured so as to invert the direction of phase modulation due to flow, and the complex images Ie 2, Ie 2 are obtained from both the echo signal line Se 2 which includes phase modulation of magnetization due to flow and from the echo signal line Sc 2 which does not includes that. Lastly, a complex differential image Id 1 between Ie 1 and Ic 1 and the complex differential image Id 2 between Ie 2 and Id 2 are obtained. The phase of the obtained complex differential images between Id 1 and Id 2 are further reduced with each other, and the phase differential image is determined. The phase differential image is converted into a flow rate image, thereby flow rate is obtained.
    • 6. 发明专利
    • MAGNETIC RESONANCE IMAGING METHOD
    • JPH07289534A
    • 1995-11-07
    • JP8616594
    • 1994-04-25
    • HITACHI LTDHITACHI MEDICAL CORP
    • HIRATA TOMOTSUGUBITO YOSHITAKAYAMAMOTO ETSUJI
    • A61B5/055G01R33/48
    • PURPOSE:To erase a signal from an unrequired substance and to easily detect a signal from a small quantity of metabolite by using plural high-frequency pulses provided with different flip angles and gradient magnetic fields for spoil. CONSTITUTION:A second high-frequency pulse RF2 in which the flip angle of nuclear spin provided with magnetization to which erasure is insufficiently applied is adjusted so as to be 90 deg. (or odd number times of 90 deg.) is irradiated. Either of gradient magnetic fields Gx, Gy and Gz is applied as a second gradient magnetic field Gs2 for spoil immediately after irradiation, and the magnetization of the nuclear spin can be erased. When the magnetization for which the erasure is insufficiently performed even by applying the high-frequency pulse RF2 and the second gradient magnetic field Gs2. for spoil exists, third, fourth,... n-th high-frequency pulses and gradient magnetic fields for spoil are applied repeatedly until the erasure of the magnetization can be sufficiently performed. After the erasure of the magnetization is sufficiently performed, either of a magnetic resonance spectrum, a magnetic resonance spectrum image and a magnetic resonance image is measured.
    • 7. 发明专利
    • DIFFUSION COEFFICIENT MEASURING METHOD IN NUCLEAR MAGNETIC RESONANCE APPARATUS
    • JPH0767849A
    • 1995-03-14
    • JP21858393
    • 1993-09-02
    • HITACHI LTDHITACHI MEDICAL CORP
    • BITO YOSHITAKAHIRATA TOMOTSUGUYAMAMOTO ETSUJI
    • A61B5/055G01R33/48
    • PURPOSE:To eliminate an error of a diffusion coefficient caused by ununiformity of a magnetic field, and to obtain an exact diffusion coefficient by calculating a gradient magnetic field factor from magnetic field ununiformity data and an impressed gradient magnetic field used for obtaining diffusion coefficient measured data, and calculating the diffusion coefficient by using the gradient magnetic field factor. CONSTITUTION:In the nuclear magnetic resonance apparatus provided with a magnet 1 for generating a static magnetic field, a coil 3 for generating a high frequency magnetic field and detecting a signal generated from an object body 2, and gradient magnetic field generating coils 4-6 for generating a gradient magnetic field in the X-Z directions, respectively, the influence of ununiformity of the magnetic field is eliminated by using a gradient magnetic field factor which becomes a function of a place for calculating a diffusion coefficient in accordance with ununiformity of the magnetic field, at the time of measuring the diffusion coefficient. That is, first of all, by considering both of the ununiformity of the magnetic field and the impressed gradient magnetic field at the time of measuring the diffusion coefficient, the gradient magnetic field factor is calculated. Subsequently, data is obtained by using the same diffusion measuring method as a conventional one, and from the obtained data, the diffusion coefficient is calculated by using the gradient magnetic field factor being the function of the place.
    • 8. 发明专利
    • SPECTRUM ANALYZING METHOD
    • JPH0755905A
    • 1995-03-03
    • JP19815593
    • 1993-08-10
    • HITACHI LTDHITACHI MEDICAL CORP
    • BITO YOSHITAKAYAMAMOTO ETSUJITAKEDA RYUSABUROWATARI HIROSHI
    • A61B5/055G01N30/86G01R33/32
    • PURPOSE:To rapidly resolve a spectrum by resolving a single spectrum disposed at one end side of an observing area to a symmetrical waveform and the other waveform at a peak position of the single spectrum as a center. CONSTITUTION:An observation spectrum is obtained from a nuclear magnetic resonance apparatus, various analyzer such as an X-ray diffraction, etc., or an inspecting unit. Number and spectral peak position of a single spectrum (spectrum regarding a component included in a sample to be inspected) included in an observing spectrum are calculated based on observing spectral data. The single spectrum disposed at the spectral peak position is calculated from one end of the observing area of the spectrum, and resolved from an superposed spectrum (observing spectrum). The calculation of the single spectrum is conducted by resolving the single spectrum to a symmetrical waveform and an asymmetrical waveform at the peak value of the single spectrum as a center, and counting the symmetrical waveform as the single spectrum. This step is repeated times of number of the single spectra, and the resolving of the spectrum is completed.