JPH03218734A - Tuning method for receiving coil in nuclear magnetic resonance imaging device - Google Patents

Tuning method for receiving coil in nuclear magnetic resonance imaging device

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Publication number
JPH03218734A
JPH03218734A JP2012613A JP1261390A JPH03218734A JP H03218734 A JPH03218734 A JP H03218734A JP 2012613 A JP2012613 A JP 2012613A JP 1261390 A JP1261390 A JP 1261390A JP H03218734 A JPH03218734 A JP H03218734A
Authority
JP
Japan
Prior art keywords
tuning
voltage
receiving coil
subject
capacity
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
JP2012613A
Other languages
Japanese (ja)
Inventor
Yasumasa Saito
齊藤 安正
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 JP2012613A priority Critical patent/JPH03218734A/en
Publication of JPH03218734A publication Critical patent/JPH03218734A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To suppress the fluctuation of a resonance point even if an L value is varied, and to always measure the signal with high quality by executing the control so that a tuning voltage applied in order to take tuning is varied in accordance with a respiratory motion, with respect to a fluctuation of the resonance point which follows a fluctuation of the L value caused by a shape variation of a flexible type receiving coil. CONSTITUTION:A tuning voltage generating part is contained in a sequencer 12, and its tuning voltage generating part 1 generates a prescribed voltage as usual. A respiration sensor 3 generates a waveform corresponding to a motion executed by respiration of a body 6 to be examined. An obtained respiratory waveform 5 is amplified by an amplifier 4 and added to a voltage from the tuning voltage generating part 1 by an adder 2, and applied to a receiving coil 20b. As for a relation of an applied voltage of a variable capacity element of a tuning part in the receiving coil 20b and the capacity, the higher the voltage is, the smaller the capacity becomes. As a result, when an L value becomes large by inspiration and the voltage rises, the capacity decreases, and on the contrary, in the case of exhalation, the L value becomes small, the capacity increases, and a variation of a tuning point can be suppressed, comparing with the time when the tuning voltage is constant.

Description

【発明の詳細な説明】 (産業上の利用分野〕 本発明は、核磁気共鳴イメージング装置(以下、MHI
装置と略す)に係り、特に可撓性を有する高周波受信コ
イルの同調を常に最良の状態にする機能を備えたMRI
装置に関する。
Detailed Description of the Invention (Industrial Field of Application) The present invention relates to a nuclear magnetic resonance imaging apparatus (hereinafter referred to as MHI
(abbreviated as "device"), in particular, an MRI device with a function to always keep the tuning of the flexible high-frequency receiving coil in the best condition.
Regarding equipment.

〔従来の技術〕[Conventional technology]

MHI装置では原子核に高周波パルスを照射して励起し
、共鳴した原子核より放出される高周波信号(これをN
MR信号という)を検出する.このNMR信号は非常に
微弱であるため質の高い信号を得るために受信コイルを
構成している共振回路は高いQ(クオリティファクタ)
が要求される.受信コイルの共振特性は被検体と受信コ
イルの間に浮遊容量が存在するため、被検体によって変
化する.従って共振特性を維持し、感度の良好な状態に
するには、被検体に合わせて受信コイルのコンデンサの
容量を調整し、共振点に同調させなければならない.こ
の同調方法は特願昭61− 255664号に詳細に記
されている. また、腹部を撮像する受信コイルは、平均的な人体寸法
に合わせた固定形状のものであった.コイルの形状には
被検体の体格に応じて画像のSZN比が最良となる最適
形状が存在するため,体格の小さい人に対しては固定形
状のコイルでは大きすぎ、得られる画像のSN比が劣化
する問題があった。これに対し特願昭63−15234
1号に示されるような可撓性を有する素材で作られた受
信コイルを使うことによりどのような体格の人に対して
も受信コイルが被検体に密着しS/Nの良好な画像が得
られるようになった. 〔発明が解決しようとする課題〕 しかしながら、上述した可撓性を有する受信コイルは、
被検体の呼吸による腹部の動きのために形状が変化する
.コイル形状の変化により受信コイルのインダクタンス
(L値)は変化し、一般に吸気ではL値は大きくなり、
呼気の場合にはL値は小さくなる.同調のための制御電
圧は一定であるため、コイルの形状変化によるL値の変
化で同調点が移動し,質の高い信号を検出することがで
きなくなり、画像の劣化が生じるという問題がある. 本発明は上述したような問題点を解消するためになされ
たものであり、信号計測中,受信コイルの同調が常にと
れた状態を維持し、S/N比の高い良質な画像が得られ
る核磁気共鳴イメージング装置を提供することを目的と
する. 〔課題を解決するための手段〕 上記目的を達成するためには、被検体の呼吸による腹部
の動きによって変化する受信コイルのL値に対応させて
、同調を行なう可変容量素子の容量を変化させて共振点
の変動を抑えることとした.すなわち、L値が増加した
時は、共振の周波数が下がるので容量を小さくし、逆に
L値が減少した時には、容量を大きくする.容量の制御
は可変容量素子に印加する同調電圧で行なわれているの
で、この電圧を共振点の変動が小さくなるように制御す
ればよい. 〔作用〕 本発明によれば、被検体の呼吸による動きに対応して変
化する可撓性受信コイルの共振点に対し該受信コイルに
印加する同調電圧を共振点が変化しないように制御する
ので、信号計測中のいずれの時においても受信コイルは
最良の同調状態となる。これにより、コイル形状が変化
しても最適受信状態が得られ、SN比の高い良質な画像
が得られる。
In the MHI device, atomic nuclei are irradiated with high-frequency pulses to excite them, and the high-frequency signals emitted from the resonant nuclei (this is called N
MR signal) is detected. This NMR signal is very weak, so in order to obtain a high quality signal, the resonant circuit that makes up the receiving coil has a high Q (quality factor).
is required. The resonance characteristics of the receiving coil vary depending on the subject because there is stray capacitance between the subject and the receiving coil. Therefore, in order to maintain resonance characteristics and achieve good sensitivity, it is necessary to adjust the capacitance of the receiver coil capacitor according to the object to be examined and tune it to the resonance point. This tuning method is described in detail in Japanese Patent Application No. 61-255664. In addition, the receiving coil used to image the abdomen had a fixed shape that matched the average human body size. There is an optimal shape of the coil that gives the best SZN ratio of the image depending on the physique of the subject, so a coil with a fixed shape is too large for a person with a small physique, and the SN ratio of the image obtained may be too large. There was a problem with deterioration. In contrast, patent application No. 15234/1983
By using a receiving coil made of a flexible material as shown in No. 1, the receiving coil can be closely attached to the subject and images with good S/N ratio can be obtained for people of any size. Now you can [Problem to be solved by the invention] However, the above-mentioned flexible receiving coil has the following problems:
The shape changes due to the movement of the abdomen due to the subject's breathing. The inductance (L value) of the receiving coil changes due to changes in the coil shape, and in general, the L value becomes larger during intake.
In the case of exhalation, the L value becomes smaller. Since the control voltage for tuning is constant, there is a problem that the tuning point moves due to changes in the L value due to changes in the shape of the coil, making it impossible to detect high-quality signals and causing image deterioration. The present invention has been made in order to solve the above-mentioned problems, and is a core system that can maintain the receiving coil in a state of constant tuning during signal measurement and obtain high-quality images with a high S/N ratio. The purpose is to provide a magnetic resonance imaging device. [Means for solving the problem] In order to achieve the above object, the capacitance of the variable capacitance element that performs tuning is changed in accordance with the L value of the receiving coil, which changes with the movement of the abdomen due to respiration of the subject. We decided to suppress the fluctuation of the resonance point. That is, when the L value increases, the resonance frequency decreases, so the capacitance is reduced, and conversely, when the L value decreases, the capacitance is increased. Since the capacitance is controlled by the tuning voltage applied to the variable capacitance element, this voltage can be controlled so that the fluctuation of the resonance point is small. [Function] According to the present invention, the tuning voltage applied to the flexible receiving coil is controlled so that the resonance point does not change with respect to the resonance point of the flexible receiving coil that changes in response to the breathing movement of the subject. , the receiving coil is in the best tuned state at any time during signal measurement. As a result, even if the coil shape changes, an optimal reception condition can be obtained, and a high-quality image with a high S/N ratio can be obtained.

〔実施例〕〔Example〕

以下、本発明の実施例を添付図面に基づいて詳細に説明
する. 第7図は本発明に係る核磁気共鳴イメージング装置の全
体構成図を示すブロック図である.この核磁気共鳴イメ
ージング装置は、核磁気共鳴(NMR)現象を利用して
被検体6の断層画像を得るもので静磁場発生磁石10と
、中央処理装置(以下,CPUという)11と、シーケ
ンサ12と送信系13と、勾配磁場発生系14と、受信
系15と、信号処理系16とからなる.上記静磁場発生
磁石10は被検体6の周りにその体軸と直交する方向に
強く均一な静磁場を発生させるもので、上記被検体6の
周りのある広がりをもった空間に永久磁石方式又は常伝
導方式あるいは超伝導方式の磁場発生手段が配置されて
いる.上記シーケンサ12は、CPUIlの制御で動作
し、被検体6の断層画像のデータ収集に必要な種々の命
令を送信系13及び勾配磁場発生系14並びに送信系1
5に送るものである.上記送信系13は、高周波発振器
17と変調器18と高周波増幅器19と送信側の高周波
コイル20aとからなり,上記高周波発撮器17から出
力された高周波パルスをシーケンサ12の命令に従って
変調器18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19で増幅した後に被検体6に近接
して配置された高周波コイル20aに供給することによ
り、電磁波が上記被検体6に照射されるようになってい
る.上記勾配磁場発生系14は、X,Y,Zの3軸方向
に巻かれた傾斜磁場コイル21とそれぞれのコイルを駆
動する傾斜磁場電源22とからなり、上記シーケンサ1
2からの命令↓こ従ってそれぞれのコイルの傾斜磁場電
源22を駆動することにより、x,y,zの3軸方向の
傾斜磁場GX ,Gy ,Gzを被検体6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
6に対するスライス面を設定することができる.上記受
信系15は、受信側の高周波コイル20bと増幅器23
と直交位相検波器24とA/D変換器25とからなり、
上記送信系の高周波コイル20aから照射された電磁波
による被検体6の応答の電磁波(NMR信号)は被検体
6に近接して配置された高周波コイル20bで検出され
、増幅器23及び直交位相検波器24を介してA/D変
換器25に入力してデジタル量に変換され、さらにシー
ケンサ12からの命令によるタイミングで直交位相検波
器24によりサンプリングされた2系統の収集データと
され、その信号が信号処理系16に送られるようになっ
ている.この信号処理系16は、CPUIIと、磁気デ
ィスク26及び磁気テープ27等の記録装置と、CRT
等のディスプレイ28とからなり上記CPUIIでフー
リ工変換、補正係数計算、画像再構成等の処理を行ない
,任意断面の信号強度分布あるいは複数の信号に適当な
演算を行なって得られた分布を画像化してディスプレイ
28に表示するようになっている。
Hereinafter, embodiments of the present invention will be described in detail based on the accompanying drawings. FIG. 7 is a block diagram showing the overall configuration of the nuclear magnetic resonance imaging apparatus according to the present invention. This nuclear magnetic resonance imaging apparatus obtains a tomographic image of a subject 6 by using the nuclear magnetic resonance (NMR) phenomenon, and includes a static magnetic field generating magnet 10, a central processing unit (hereinafter referred to as CPU) 11, and a sequencer 12. It consists of a transmission system 13, a gradient magnetic field generation system 14, a reception system 15, and a signal processing system 16. The static magnetic field generating magnet 10 generates a strong and uniform static magnetic field around the subject 6 in a direction perpendicular to the body axis of the subject 6. A normal-conducting or superconducting magnetic field generating means is installed. The sequencer 12 operates under the control of the CPU I, and sends various commands necessary for data collection of tomographic images of the subject 6 to the transmission system 13, the gradient magnetic field generation system 14, and the transmission system 1.
5. The transmission system 13 includes a high-frequency oscillator 17, a modulator 18, a high-frequency amplifier 19, and a high-frequency coil 20a on the transmitting side. The amplitude modulated high frequency pulse is amplified by a high frequency amplifier 19 and then supplied to a high frequency coil 20a placed close to the subject 6, so that the subject 6 is irradiated with electromagnetic waves. It has become. The gradient magnetic field generation system 14 is composed of gradient magnetic field coils 21 wound in three axial directions of X, Y, and Z, and a gradient magnetic field power supply 22 for driving each coil.
By driving the gradient magnetic field power supply 22 of each coil in accordance with the command from 2 ↓, gradient magnetic fields GX, Gy, Gz in the three axis directions of x, y, and z are applied to the subject 6. .. A slice plane for the subject 6 can be set by applying this gradient magnetic field. The receiving system 15 includes a high frequency coil 20b and an amplifier 23 on the receiving side.
It consists of a quadrature phase detector 24 and an A/D converter 25,
Electromagnetic waves (NMR signals) in response to the subject 6 due to the electromagnetic waves irradiated from the high frequency coil 20a of the transmission system are detected by the high frequency coil 20b placed close to the subject 6, and are detected by the amplifier 23 and the quadrature phase detector 24. The signals are input to the A/D converter 25 via the A/D converter 25 and converted into digital quantities, and further sampled by the quadrature phase detector 24 at the timing according to the command from the sequencer 12, resulting in two systems of collected data, and the signals are subjected to signal processing. It is now sent to system 16. This signal processing system 16 includes a CPU II, a recording device such as a magnetic disk 26 and a magnetic tape 27, and a CRT.
The CPU II performs processing such as Fourier transform, correction coefficient calculation, and image reconstruction, and displays the signal intensity distribution of an arbitrary cross section or the distribution obtained by performing appropriate calculations on multiple signals as an image. The image is displayed on the display 28.

本発明に係る同調電圧発生部は第7図のシーケンサ12
に含まれ、その詳細を第1図に示す.これは従来の同調
電圧発生部1と加算器2と呼吸センサ3と増幅器4とか
らなる。従来の同調電圧発生部1は、従来通り、一定の
電圧を発生する.呼吸センサ3は被検体6の呼吸による
動きに応じた波形を発生する.第2図はこの波形の概略
図で呼気の時と比較して吸気の時には受信コイルのL値
は大きくなる。得られた呼吸波形5は増幅器4で増幅さ
れ加算器2により上述した従来の同調電圧発生部1から
の電圧と加算され、受信コイル20bに印加される。従
来の同調電圧に呼吸による電圧を加算した本発明の同調
電圧の概略を第3図に示す.受信コイル20b内の同調
部の可変容量素子の印加電圧と容量の関係は第4図に示
すように電圧が高いほど容量は小さくなる.コイル形状
の変化による同調周波数の変化は約6 0 k H z
でL値の変化は0.1μHである.この変化を補償する
容量の変化は実測で80pFであった.可変容量素子の
容量変化幅は約120pFであるからコイル形状変化の
中点で同調が行なわれていればコイルのL値の変化を容
量素子の容量変化で補償が可能である.すなわち吸気で
L値が大きくなり電圧が上がると容量が減少し、逆に呼
気ではL値が小さくなり、容量が増加し、同調点の変化
を同調電圧が一定の時と比較して抑えることができる。
The tuning voltage generating section according to the present invention is the sequencer 12 shown in FIG.
The details are shown in Figure 1. It consists of a conventional tuning voltage generator 1, an adder 2, a respiratory sensor 3, and an amplifier 4. The conventional tuning voltage generator 1 generates a constant voltage as before. The breathing sensor 3 generates a waveform corresponding to the movement of the subject 6 due to breathing. FIG. 2 is a schematic diagram of this waveform, and the L value of the receiving coil is larger during inspiration than during exhalation. The obtained respiratory waveform 5 is amplified by an amplifier 4, added to the voltage from the conventional tuning voltage generator 1 described above by an adder 2, and applied to the receiving coil 20b. Figure 3 shows an outline of the tuning voltage of the present invention, which is obtained by adding the voltage caused by breathing to the conventional tuning voltage. The relationship between the applied voltage and the capacitance of the variable capacitance element of the tuning section in the receiving coil 20b is shown in FIG. 4, as shown in FIG. 4, the higher the voltage, the smaller the capacitance. The change in tuning frequency due to the change in coil shape is approximately 60 kHz.
The change in L value is 0.1μH. The change in capacitance to compensate for this change was actually measured to be 80 pF. Since the capacitance change width of the variable capacitance element is about 120 pF, if tuning is performed at the midpoint of the coil shape change, it is possible to compensate for the change in the L value of the coil by the capacitance change of the capacitor. In other words, when the L value increases during inspiration and the voltage increases, the capacity decreases, and conversely during exhalation the L value decreases and the capacity increases, making it possible to suppress changes in the tuning point compared to when the tuning voltage is constant. can.

また、増幅器4は受信コイルのL値の変化を補償し、共
振点の変動を最小限に抑えるために呼吸波形の増幅率や
オフセットを調整できるようになっている.上記した呼
吸センサは,たとえば第5図に示すように被検体両側に
対応するガントリ−40側面にいくつかの赤外線送受信
部30.31の対を対向してならべ、被検体の呼吸によ
る動きにより受信部31に到達する信号の変化を観測し
てもよいし、あるいは、第6図に示したように被検体上
方のガントリ−40に設置された1対の赤外線等の送受
信部30.31を使い、送信部30から送4 られた信号が受信部31に到達する時間の変化を観測し
てもよいし、又は、一般的な呼吸同期撮像時に使用され
る呼吸センサなど、被検体の呼吸波形が計測できるもの
であれば何れのものでもよい.なお、第3図に示した本
発明の同調電圧波形において、従来の一定の同調電圧8
が被検体6の呼気の時と同じであるのは、従来の同調電
圧8を決定する時に被検体に呼気の状態で呼吸を止めて
行なった時の例である。
Furthermore, the amplifier 4 is capable of adjusting the amplification factor and offset of the respiratory waveform in order to compensate for changes in the L value of the receiving coil and to minimize fluctuations in the resonance point. The above-mentioned respiration sensor has several pairs of infrared transmitting/receiving units 30 and 31 arranged facing each other on the side of the gantry 40 corresponding to both sides of the subject, and receives signals based on the breathing movement of the subject. It is also possible to observe changes in the signal reaching the section 31, or to use a pair of infrared transmitting/receiving sections 30 and 31 installed on a gantry 40 above the subject as shown in FIG. It is also possible to observe changes in the time at which the signal sent from the transmitting section 30 reaches the receiving section 31, or to monitor the respiratory waveform of the subject using a respiratory sensor used in general respiratory gated imaging. It can be anything that can be measured. Note that in the tuning voltage waveform of the present invention shown in FIG.
The fact that is the same as when the subject 6 is exhaling is an example when the conventional tuning voltage 8 is determined by having the subject hold their breath while exhaling.

〔発明の効果〕〔Effect of the invention〕

以上述べたように本発明は、可撓型受信コイルの形状変
化によるL値の変動に伴う共振点の変動に対し、同調を
とるために印加する同調電圧をこれまでの一定であった
ものから、呼吸動に応じて変化するように制御したので
、L値が変わっても共振点の変動を抑えることができ、
常に質の高い信号計測が行え、画質の向上が計れるとい
う効果がある.
As described above, the present invention changes the tuning voltage applied for tuning from the conventional constant voltage to the fluctuation of the resonance point due to the fluctuation of the L value due to the change in the shape of the flexible receiving coil. , because it was controlled to change according to respiratory movements, it was possible to suppress fluctuations in the resonance point even if the L value changed,
This has the effect of always being able to perform high-quality signal measurements and improving image quality.

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

第1図は本発明の同調電圧発生部の実施例図,第2図は
被検体の呼吸波形の概略図、第3図は本発明の同調電圧
波形の概略図、第4図は同調電圧対容量の関係を示す概
略図、第5図および第6図は呼吸波形計測の方法を示す
実施例図、第7図は本発明のMRI装置の実施例図であ
る.1・・・従来の同調電圧発生部、2・・・加算器、
3・・・呼吸センサ、4・・・増幅器、5・・・呼吸波
形,6・・・被検体、7・・・同調電圧波形、8・・・
従来の同調電圧、30・・・送信部(呼吸波形計測用)
、31・・・受信部第 g l 第 Z (2) 咋同 #3 m 茶4の
Fig. 1 is an example diagram of the tuning voltage generation section of the present invention, Fig. 2 is a schematic diagram of a breathing waveform of a subject, Fig. 3 is a schematic diagram of a tuning voltage waveform of the present invention, and Fig. 4 is a diagram of a tuning voltage pair. FIGS. 5 and 6 are schematic diagrams showing the relationship between volumes, FIGS. 5 and 6 are examples of a method of measuring respiratory waveforms, and FIG. 7 is an example of the MRI apparatus of the present invention. 1... Conventional tuning voltage generator, 2... Adder,
3... Breathing sensor, 4... Amplifier, 5... Breathing waveform, 6... Subject, 7... Tuning voltage waveform, 8...
Conventional tuning voltage, 30... Transmitter (for respiratory waveform measurement)
, 31... Receiving part g l Z (2) Kui Tong #3 m Tea 4

Claims (1)

【特許請求の範囲】[Claims] 1. 被検体の体軸方向又はこれと直交する方向に静磁
場を発生させる静磁場発生磁石を有すると共に該被検体
に電磁波を照射する高周波送信系と該被検体に近接させ
て配置され該被検体から放出される電磁波を検出する高
周波受信コイルと受信した信号を増幅、周波数変換する
高周波受信系と該高周波送信系と該高周波受信系の制御
を行なう高周波制御系を有する核磁気共鳴イメージング
装置において、該高周波制御系の高周波受信コイルの同
調電圧発生部は受信コイルの同調点の変化を少なくする
ような制御電圧を発生することを特徴とする核磁気共鳴
イメージング装置における受信コイルのチユーニング方
法。
1. A high frequency transmission system having a static magnetic field generating magnet that generates a static magnetic field in the direction of the body axis of the subject or in a direction perpendicular thereto, and irradiating electromagnetic waves to the subject; A nuclear magnetic resonance imaging apparatus comprising a high frequency receiving coil for detecting emitted electromagnetic waves, a high frequency receiving system for amplifying and frequency converting the received signal, and a high frequency control system for controlling the high frequency transmitting system and the high frequency receiving system. A method for tuning a receiving coil in a nuclear magnetic resonance imaging apparatus, characterized in that a tuning voltage generating section of a high-frequency receiving coil of a high-frequency control system generates a control voltage that reduces changes in a tuning point of the receiving coil.
JP2012613A 1990-01-24 1990-01-24 Tuning method for receiving coil in nuclear magnetic resonance imaging device Pending JPH03218734A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2012613A JPH03218734A (en) 1990-01-24 1990-01-24 Tuning method for receiving coil in nuclear magnetic resonance imaging device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2012613A JPH03218734A (en) 1990-01-24 1990-01-24 Tuning method for receiving coil in nuclear magnetic resonance imaging device

Publications (1)

Publication Number Publication Date
JPH03218734A true JPH03218734A (en) 1991-09-26

Family

ID=11810225

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2012613A Pending JPH03218734A (en) 1990-01-24 1990-01-24 Tuning method for receiving coil in nuclear magnetic resonance imaging device

Country Status (1)

Country Link
JP (1) JPH03218734A (en)

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