JPH11290294A - Magnetic resonance imaging apparatus - Google Patents

Magnetic resonance imaging apparatus

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Publication number
JPH11290294A
JPH11290294A JP10112872A JP11287298A JPH11290294A JP H11290294 A JPH11290294 A JP H11290294A JP 10112872 A JP10112872 A JP 10112872A JP 11287298 A JP11287298 A JP 11287298A JP H11290294 A JPH11290294 A JP H11290294A
Authority
JP
Japan
Prior art keywords
magnetic field
frequency
magnetic resonance
subject
sequencer
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP10112872A
Other languages
Japanese (ja)
Inventor
Mutsumi Yoshikata
睦 善方
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Hitachi Healthcare Manufacturing Ltd
Original Assignee
Hitachi Medical Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Hitachi Medical Corp filed Critical Hitachi Medical Corp
Priority to JP10112872A priority Critical patent/JPH11290294A/en
Publication of JPH11290294A publication Critical patent/JPH11290294A/en
Pending legal-status Critical Current

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  • Magnetic Resonance Imaging Apparatus (AREA)

Abstract

PROBLEM TO BE SOLVED: To prevent degrading of the quality of a tomographic picture by reducing effect as caused by changes in the surrounding environment of a magnetic field of a magnetic field generation means. SOLUTION: A magnetic field sensor 21 is arranged near an electrostatic magnetic field generation magnet 2 to measure the environment F of a magnetic field. Any change in the environment F of the magnetic field is detected by a magnetic field sensor 21 and a detection signal is inputted into a sequencer 7 through an A/D converter 22. The sequencer 7 translates the change in the magnetic field into a frequency and outputs a frequency signal after the changes in the magnetic field to a transmitting system 4 and a receiving system 5. This eliminates the need for a correction magnetic field coil and a correction control circuit to cancel changes in the surrounding environment of the magnetic field thereby significantly improving installing availability and cost.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】核磁気共鳴(NMR)現象を
利用して被検体の検査部位の画像を得る磁気共鳴イメー
ジング装置に関し、特に磁場発生手段の周囲の磁場環境
変動による影響を低減して断層像の画質劣化を防止する
ことができるMRI装置に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnetic resonance imaging apparatus that obtains an image of an examination part of a subject by utilizing a nuclear magnetic resonance (NMR) phenomenon, and in particular, to reduce the influence of a magnetic field environment fluctuation around a magnetic field generating means and tomography The present invention relates to an MRI apparatus capable of preventing image quality deterioration.

【0002】[0002]

【従来の技術】従来のMRI装置は、その磁場発生手段
の周囲の磁場環境変動による影響を低減して断層像の画
質劣化を防止するため、当該装置全体の周囲六面をパー
マロイ,アモルファス金属等の高透磁率材料で囲んで磁
気シールドしていた。しかし、この方法では、一台のM
RI装置について、材料費及び工事費等が高額になると
共に、画質劣化の防止が完全とは言えなかった。
2. Description of the Related Art In a conventional MRI apparatus, six surfaces around the entire apparatus are made of permalloy, amorphous metal or the like in order to reduce the influence of magnetic field environment fluctuation around the magnetic field generating means and to prevent image quality deterioration of tomographic images. Magnetically shielded with a high permeability material. However, in this method, one M
Regarding the RI apparatus, the material cost and the construction cost are high, and the prevention of the image quality deterioration is not perfect.

【0003】これに対して、近年、特開平2−4503
5号公報に記載されているようなMRI装置が提案され
ている。すなわち、磁場発生手段の周囲の磁場環境変動
を磁場センサで検出し、この磁場センサで検出した出力
波形を増幅器で増幅し、この出力信号に応じて補正磁場
コイル電源で補正電流を生成し、この補正電流を静磁場
発生の磁気回路の内部に上下に対向して平行に設けられ
たループ状の補正磁場コイルに流し、これによって上記
磁場環境変動と逆向きの補正磁場を発生させ、この補正
磁場により、上記磁場環境変動を打ち消すものである。
On the other hand, in recent years, Japanese Patent Laid-Open Publication No.
An MRI apparatus as described in Japanese Patent Laid-Open Publication No. 5 has been proposed. That is, a magnetic field environment fluctuation around the magnetic field generating means is detected by a magnetic field sensor, an output waveform detected by the magnetic field sensor is amplified by an amplifier, and a correction current is generated by a correction magnetic field coil power supply according to the output signal. The correction current is caused to flow through a loop-shaped correction magnetic field coil provided in parallel in a magnetic circuit for generating a static magnetic field so as to be vertically opposed to each other, thereby generating a correction magnetic field in a direction opposite to the above-described magnetic field environment fluctuation. This cancels out the magnetic field environment fluctuation.

【0004】[0004]

【発明が解決しようとする課題】従来のMRI装置にお
いては、磁場センサの他に、補正制御回路,補正磁場コ
イルが必要であった。また、近年のオープン型MRI装
置においては、ガントリー構造が複雑になり、補正磁場
コイルを機外に設置する方法も提案されているが、補正
磁場コイルを機外に設置すると、その補正磁場の影響
で、磁場センサの設置場所に制限を受けて、補正を正確
に行うことが困難であるという問題があった。
In the conventional MRI apparatus, a correction control circuit and a correction magnetic field coil are required in addition to the magnetic field sensor. In recent years, in open MRI apparatuses, the gantry structure has become complicated, and a method of installing a correction magnetic field coil outside the apparatus has been proposed. Thus, there is a problem in that it is difficult to accurately perform the correction due to the restriction on the installation location of the magnetic field sensor.

【0005】そこで、本発明は、上記問題点を解決し
て、外来磁場の影響による画質低下をきたさないMRI
装置を提供することを目的とするため、磁場センサから
の信号を基に、被検体に核磁気共鳴を起こさせるための
照射電磁波及び、被検体の核磁気共鳴により放出される
電磁波を収集する受信系の検波器16の周波数を、磁場
環境変動により共鳴周波数が変化した分だけシフトさせ
ることにより、画像劣化を防止する。
Accordingly, the present invention solves the above-mentioned problems, and prevents MRI from deteriorating the image quality due to the influence of an external magnetic field.
In order to provide an apparatus, an irradiation electromagnetic wave for causing nuclear magnetic resonance in a subject and a reception for collecting electromagnetic waves emitted by nuclear magnetic resonance of the subject based on a signal from a magnetic field sensor are provided. The image deterioration is prevented by shifting the frequency of the detector 16 of the system by an amount corresponding to the change of the resonance frequency due to the magnetic field environment fluctuation.

【0006】[0006]

【課題を解決するための手段】上記目的を達成するため
に、本発明によるMRI装置は、被検体に静磁場及び傾
斜磁場を与える磁場発生手段と,上記被検体の生体組織
を構成する原子の原子核に核磁気共鳴を起こさせるため
に電磁波を照射する送信系と,上記の核磁気共鳴により
放出される電磁波を検出する受信系と,この受信系で検
出した電磁波の信号を用いて画像再構成演算を行う信号
処理系と,上記磁場発生手段の周囲の磁場環境変動を検
出する磁場センサと,を備えて成る磁気共鳴イメージン
グ装置において、上記磁場センサからの信号をもとに、
上記送信系から出力される照射電磁波の周波数と,受信
系の検波周波数とを同一となるように制御する手段を設
けたものである。
In order to achieve the above object, an MRI apparatus according to the present invention comprises: a magnetic field generating means for applying a static magnetic field and a gradient magnetic field to a subject; A transmission system that irradiates an electromagnetic wave to cause nuclear magnetic resonance in a nucleus, a reception system that detects an electromagnetic wave emitted by the above-described nuclear magnetic resonance, and an image reconstruction using a signal of the electromagnetic wave detected by the reception system In a magnetic resonance imaging apparatus including a signal processing system for performing an operation and a magnetic field sensor for detecting a change in a magnetic field environment around the magnetic field generating means, based on a signal from the magnetic field sensor,
Means is provided for controlling the frequency of the irradiation electromagnetic wave output from the transmission system and the detection frequency of the reception system to be the same.

【0007】[0007]

【発明の実施の形態】以下、本発明の実施の形態を図面
を用いて説明する。図1は、本発明によるMRI装置の
実施例を示す全体構成のブロック図である。このMRI
装置は、核磁気共鳴現象を利用して、被検体の断層像を
得るもので、図1に示すように、静磁場発生磁石2と,
磁場勾配発生系(9,10)と,送信系4と,受信系5
と,信号処理系6と,シーケンサ7と,中央処理装置
(CPU)8と,磁場センサ21とを備えて成る。
Embodiments of the present invention will be described below with reference to the drawings. FIG. 1 is a block diagram of an overall configuration showing an embodiment of an MRI apparatus according to the present invention. This MRI
The apparatus obtains a tomographic image of a subject by using a nuclear magnetic resonance phenomenon. As shown in FIG.
Magnetic field gradient generating system (9, 10), transmitting system 4, and receiving system 5
, A signal processing system 6, a sequencer 7, a central processing unit (CPU) 8, and a magnetic field sensor 21.

【0008】上記静磁場発生磁石2は、被検体1の周り
にその体軸方向(水平方向)または体軸と直交する方向
(垂直方向)に均一な静磁場を発生させるもので、上記
被検体の1の周りのある広がりをもった空間に永久磁石
方式または常電導方式あるいは超電導方式の磁場発生手
段によって静磁場を発生させる。なお、図1では、上記
静磁場の方向を図中の矢印Aの向きで示している。磁場
勾配発生系は、X,Y,Zの三軸方向に巻かれた傾斜磁
場コイル9と,それぞれのコイルを駆動する傾斜磁場電
源10とから成り、上記シーケンサ7からの命令に従っ
てそれぞれのコイルの傾斜磁場電源10を駆動すること
により、X,Y,Zの三軸方向の傾斜磁場Gx,Gy,
Gzを被検体1に印加するようになっている。この傾斜
磁場の加え方により、被検体1に対するスライス面を設
定することができる。
The static magnetic field generating magnet 2 generates a uniform static magnetic field around the subject 1 in the body axis direction (horizontal direction) or the direction perpendicular to the body axis (vertical direction). A static magnetic field is generated by a permanent magnet type, a normal conduction type, or a superconducting type magnetic field generating means in a space having a certain extent around the above 1. In FIG. 1, the direction of the static magnetic field is indicated by the direction of arrow A in the figure. The magnetic field gradient generating system includes a gradient magnetic field coil 9 wound in three directions of X, Y, and Z, and a gradient magnetic field power supply 10 for driving each coil. By driving the gradient magnetic field power supply 10, gradient magnetic fields Gx, Gy,
Gz is applied to the subject 1. The slice plane with respect to the subject 1 can be set by the method of applying the gradient magnetic field.

【0009】送信系4は、被検体1の生体組織を構成す
る原子の原子核に核磁気共鳴を起こさせるために電磁波
を照射するもので、高周波発振器11と変調器12と高
周波増幅器13とを送信側の高周波コイル14aとから
成り、上記高周波発振器11から出力された高周波パル
スをシーケンサ7の命令に従って変調器12で振幅変調
し、この振幅変調された高周波パルスを高周波増幅器1
3で増幅した後に被検体1に近接して配置された高周波
コイル14aに供給することにより、電磁波が上記被検
体1に照射されるようになっている。
The transmission system 4 irradiates an electromagnetic wave to cause nuclear magnetic resonance to the nuclei of the atoms constituting the living tissue of the subject 1. The transmission system 4 transmits a high-frequency oscillator 11, a modulator 12, and a high-frequency amplifier 13. A high-frequency pulse output from the high-frequency oscillator 11 is amplitude-modulated by the modulator 12 in accordance with a command from the sequencer 7 and the high-frequency pulse is output from the high-frequency amplifier 1.
After being amplified by 3 and supplied to the high-frequency coil 14a arranged close to the subject 1, the subject 1 is irradiated with electromagnetic waves.

【0010】また、受信系5は、被検体1の生体組織の
原子核の核磁気共鳴により放出される電磁波(NMR信
号)を検出するもので、受信側の高周波コイル14bと
増幅器15と直交位相検波器16とA/D変換器17と
を有して成り、上記送信側の高周波コイル14aから照
射された電磁波による被検体1の応答の電磁波(NMR
信号)は被検体1に近接して配置された高周波コイル1
4bで検出され、増幅器15及び直交位相検波器16を
介してA/D変換器17に入力してディジタル量に変換
され、さらにシーケンサ7からの命令によるタイミング
で直交位相検波器16によりサンプリングされた二系列
の収集データとされ、その信号が信号処理系6に送られ
るようになっている。
The receiving system 5 detects electromagnetic waves (NMR signals) emitted by nuclear magnetic resonance of atomic nuclei of the living tissue of the subject 1. The receiving system 5 includes a high-frequency coil 14b on the receiving side, an amplifier 15, and a quadrature phase detector. An electromagnetic wave (NMR) of a response of the subject 1 due to an electromagnetic wave emitted from the high-frequency coil 14a on the transmitting side.
Signal) is a high-frequency coil 1 disposed close to the subject 1
4b, input to the A / D converter 17 via the amplifier 15 and the quadrature detector 16 and converted into a digital quantity, and further sampled by the quadrature detector 16 at a timing according to a command from the sequencer 7. The collected data is two-series data, and the signal is sent to the signal processing system 6.

【0011】この信号処理系6は、CPU8と,磁気デ
ィスク18及び磁気テープ19等の記録装置と,CRT
等のディスプレイ20とから成り、上記CPU8でフー
リエ変換,補正係数計算,画像再構成等の処理を行い、
任意断面の信号強度分布あるいは複数の信号に適当な演
算を行って得られた分布を画像化してディスプレイ20
に断層像として表示するようになっている。
The signal processing system 6 includes a CPU 8, a recording device such as a magnetic disk 18 and a magnetic tape 19, and a CRT.
The CPU 8 performs processing such as Fourier transform, correction coefficient calculation, image reconstruction, and the like.
The signal intensity distribution at an arbitrary cross section or the distribution obtained by performing an appropriate operation on a plurality of signals is imaged and displayed on the display 20.
Is displayed as a tomographic image.

【0012】シーケンサ7は、CPU8の制御で動作
し、被検体1の断層像のデータ収集に必要な種々の命令
を送信系4及び磁場勾配発生系(9,10)並びに受信
系5に送り、上記NMR信号を計測するシーケンスを発
生する手段となるものである。なお、図1において、送
信側の高周波コイル14a及び受信側の高周波コイル1
4b並びに傾斜磁場コイル9,9は、被検体1の周りの
空間に配置された静磁場発生磁石2の磁場空間内に配置
されている。
The sequencer 7 operates under the control of the CPU 8 and sends various commands necessary for collecting data of tomographic images of the subject 1 to the transmission system 4, the magnetic field gradient generation systems (9, 10) and the reception system 5, This is a means for generating a sequence for measuring the NMR signal. In FIG. 1, the high-frequency coil 14a on the transmitting side and the high-frequency coil 1 on the receiving side
4 b and the gradient magnetic field coils 9, 9 are arranged in the magnetic field space of the static magnetic field generating magnet 2 arranged in the space around the subject 1.

【0013】磁場センサ21は、前記静磁場発生磁石2
の周囲において、静磁場方向(矢印Aの方向)の磁石環
境(磁場変動)Fを検出するものである。A/D変換器
22は、磁石センサ21からの検出信号を変換し、シー
ケンサ7に送る。
The magnetic field sensor 21 includes the static magnetic field generating magnet 2
, A magnet environment (magnetic field fluctuation) F in the static magnetic field direction (direction of arrow A) is detected. The A / D converter 22 converts a detection signal from the magnet sensor 21 and sends it to the sequencer 7.

【0014】磁気共鳴周波数は、上記静磁場発生磁石2
の強度により与えられるので磁場環境Fが変わると、静
磁場発生磁石2の計測空間の磁場強度も変化してしま
い、共鳴周波数も変化する。したがって、計測中に磁場
環境Fが変化すると撮影位置がずれたり、撮影位置が定
まらず画像ボケとなる。
The magnetic resonance frequency depends on the static magnetic field generating magnet 2.
When the magnetic field environment F changes, the magnetic field strength in the measurement space of the static magnetic field generating magnet 2 also changes, and the resonance frequency also changes. Therefore, if the magnetic field environment F changes during measurement, the imaging position shifts or the imaging position is not determined, resulting in image blur.

【0015】そこで、本発明は、図2に示すように、磁
場センサ21で磁場環境Fの変化を検出し、A/D変換
器を介してシーケンサ7に入力する。シーケンサ7は、
CPU8又は自身が所有するMPUにより磁場環境Fの
変化から共鳴周波数の変化を算出し、磁気共鳴を起こさ
せるための電磁波の周波数を算出する。この求められた
共鳴周波数に対応する信号がシーケンサ7より出力さ
れ、高周波発振器11の出力する信号をシーケンサ7の
出力信号に基いて変調器12で変調し、高周波増幅器1
3で増幅して送信系高周波コイル14aに印加すること
により、被検体1へ電磁波(RFパルス)を照射する。
Accordingly, in the present invention, as shown in FIG. 2, a change in the magnetic field environment F is detected by the magnetic field sensor 21 and input to the sequencer 7 via the A / D converter. Sequencer 7
The CPU 8 or its own MPU calculates a change in resonance frequency from a change in the magnetic field environment F, and calculates a frequency of an electromagnetic wave for causing magnetic resonance. A signal corresponding to the obtained resonance frequency is output from the sequencer 7, and a signal output from the high-frequency oscillator 11 is modulated by the modulator 12 based on the output signal of the sequencer 7.
The subject 1 is irradiated with an electromagnetic wave (RF pulse) by amplifying it at 3 and applying it to the transmission system high-frequency coil 14a.

【0016】一方、受信系高周波コイル14bは被検体
1からのNMR信号を検出するようになっている。そし
て、検出信号(NMR信号)はプリアンプ23,増幅器
24で増幅された後、直交位相検波器16に入力される
ようになっている。
On the other hand, the receiving system high-frequency coil 14b detects an NMR signal from the subject 1. The detection signal (NMR signal) is amplified by the preamplifier 23 and the amplifier 24 and then input to the quadrature detector 16.

【0017】画像情報として用いられるNMR信号は、
直交位相検波器16内のミキサ25によって周波数変換
されるが、このミキサ25にシーケンサ7で求められた
共鳴周波数の信号を入力する。これにより、送信信号
(RFパルス)の周波数と検波の周波数とが磁場環境F
が変化しても同一のものとなるので、環境位置ずれや、
画像ボケが生ずることはなくなる。
The NMR signal used as image information is
The frequency is converted by the mixer 25 in the quadrature phase detector 16, and the signal of the resonance frequency determined by the sequencer 7 is input to the mixer 25. As a result, the frequency of the transmission signal (RF pulse) and the frequency of detection become the magnetic field environment F
Will be the same even if the position changes,
Image blur does not occur.

【0018】なお、送信系,受信系に入力する共鳴周波
数の補正は、NMR信号収集の各パルスシーケンス実行
毎に行うのが最も良い方法であるが、数回のパルスシー
ケンス実行毎に1回程度行うことでも画像の改善効果は
得られる。
The resonance frequency input to the transmission system and the reception system is best corrected every time a pulse sequence of NMR signal collection is executed. However, it is about once every several pulse sequences. By doing so, the effect of improving the image can be obtained.

【0019】また、本実施例では、磁場センサ21の検
出方向を静磁場の発生方向と同じにしているが、静磁場
方向と直交する方向を検出しても同様の結果が得られ
る。
Further, in this embodiment, the detection direction of the magnetic field sensor 21 is the same as the direction in which the static magnetic field is generated. However, the same result can be obtained by detecting a direction perpendicular to the static magnetic field direction.

【0020】シーケンサ7内に応答速度を可変する回路
を設ける(立上りを速く,又は遅くする)とより画質の
ボケを抑えることができる。
If a circuit for varying the response speed is provided in the sequencer 7 (the rising speed is made faster or slower), the blur of the image quality can be further suppressed.

【0021】[0021]

【発明の効果】本発明は、以上のように構成されたの
で、静磁場発生手段の近傍に設けられた磁場センサによ
り磁場発生手段の周囲の磁場環境変動を検出し、共鳴周
波数の変動量に応じて上記シーケンサにより、照射電磁
波及び,受信系の検波器の周波数を同一になるように制
御するので、周囲の磁場環境変動による影響を低減して
画質劣化を防止することができる。
As described above, the present invention is configured as described above, so that the magnetic field sensor provided near the static magnetic field generating means detects the fluctuation of the magnetic field environment around the magnetic field generating means, and the variation of the resonance frequency is detected. Accordingly, the sequencer controls the irradiation electromagnetic wave and the frequency of the detector in the receiving system to be the same, so that the influence of the fluctuation of the surrounding magnetic field environment can be reduced, and the image quality can be prevented from deteriorating.

【0022】また、従来技術のように、補正磁場コイ
ル,補正磁場が不要となるため、設置性,コストが大幅
に改善できる。
Further, unlike the related art, the correction magnetic field coil and the correction magnetic field are not required, so that the installation property and the cost can be greatly improved.

【図面の簡単な説明】[Brief description of the drawings]

【図1】本発明による磁気共鳴イメージング装置の全体
を示す概略構成図。
FIG. 1 is a schematic configuration diagram showing an entire magnetic resonance imaging apparatus according to the present invention.

【図2】実施例における周波数制御の構成図。FIG. 2 is a configuration diagram of frequency control in the embodiment.

【符号の説明】[Explanation of symbols]

1 被検体 2 静磁場発生磁石 4 送信系 5 受信系 6 信号処理系 7 シーケンサ 8 CPU 9 傾斜磁場コイル 14a 送信側の高周波コイル 14b 受信側の高周波コイル 21 磁場センサ 22 ADC 25 ミキサ REFERENCE SIGNS LIST 1 subject 2 static magnetic field generating magnet 4 transmission system 5 reception system 6 signal processing system 7 sequencer 8 CPU 9 gradient magnetic field coil 14a high-frequency coil on transmission side 14b high-frequency coil on reception side 21 magnetic field sensor 22 ADC 25 mixer

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 被検体に静磁場及び傾斜磁場を与える磁
場発生手段と,上記被検体の生体組織を構成する原子の
原子核に核磁気共鳴を起こさせるために電磁波を照射す
る送信系と,上記の核磁気共鳴により放出される電磁波
を検出する受信系と,この受信系で検出した電磁波の信
号を用いて画像再構成演算を行う信号処理系と,上記磁
場発生手段の周囲の磁場環境変動を検出する磁場センサ
と,前記磁場環境変動があったときにこの磁場センサか
らの検出信号をもとに、上記送信系から出力される照射
電磁波の周波数と,上記受信系の検波周波数とを同一と
なるように制御する手段を備えたことを特徴とする磁気
共鳴イメージング装置。
1. A magnetic field generating means for applying a static magnetic field and a gradient magnetic field to a subject, a transmission system for irradiating an electromagnetic wave to cause nuclear magnetic resonance in nuclei of atoms constituting a living tissue of the subject, A receiving system for detecting electromagnetic waves emitted by nuclear magnetic resonance, a signal processing system for performing image reconstruction operations using signals of the electromagnetic waves detected by the receiving system, and a magnetic field environment fluctuation around the magnetic field generating means. Based on the magnetic field sensor to be detected and the detection signal from the magnetic field sensor when the magnetic field environment changes, the frequency of the radiated electromagnetic wave output from the transmission system and the detection frequency of the reception system are the same. A magnetic resonance imaging apparatus, comprising: means for controlling the magnetic resonance imaging apparatus.
JP10112872A 1998-04-09 1998-04-09 Magnetic resonance imaging apparatus Pending JPH11290294A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10112872A JPH11290294A (en) 1998-04-09 1998-04-09 Magnetic resonance imaging apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10112872A JPH11290294A (en) 1998-04-09 1998-04-09 Magnetic resonance imaging apparatus

Publications (1)

Publication Number Publication Date
JPH11290294A true JPH11290294A (en) 1999-10-26

Family

ID=14597649

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10112872A Pending JPH11290294A (en) 1998-04-09 1998-04-09 Magnetic resonance imaging apparatus

Country Status (1)

Country Link
JP (1) JPH11290294A (en)

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