JPH024328A - Nuclear magnetic resonance imaging device - Google Patents

Nuclear magnetic resonance imaging device

Info

Publication number
JPH024328A
JPH024328A JP63152341A JP15234188A JPH024328A JP H024328 A JPH024328 A JP H024328A JP 63152341 A JP63152341 A JP 63152341A JP 15234188 A JP15234188 A JP 15234188A JP H024328 A JPH024328 A JP H024328A
Authority
JP
Japan
Prior art keywords
frequency coil
coil
subject
high frequency
connector
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
JP63152341A
Other languages
Japanese (ja)
Inventor
Hidenori Kishino
岸野 秀則
Yukihiro Yasugi
八杉 幸浩
Hiroyuki Takeuchi
博幸 竹内
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 JP63152341A priority Critical patent/JPH024328A/en
Publication of JPH024328A publication Critical patent/JPH024328A/en
Pending legal-status Critical Current

Links

Landscapes

  • Magnetic Resonance Imaging Apparatus (AREA)

Abstract

PURPOSE:To obtain an optimum receiving condition regardless of the build of a checked body and the size of a checked part and to maintain high picture quality by forming a high frequency coil, which detects an electro-magnetic wave to be discharged from the checked body, with a material having flexibility. CONSTITUTION:A coil line material 30 of a high frequency coil 20 is composed of a soft coil line material such as a flat cable or FPC, for example. To the high frequency coil 20, connectors 31 and 32, which are composed of a non- magnetic substance and the material of small high frequency loss, a tuning circuit 33 to tune the high frequency coil 20 to a remove frequency, which is determined by magneto-static intensity, and a lead wire 34 for connection to a pre-amplifier are fit. At the time of image pick-up, for the high frequency coil 20, the coil line material 30 is wound along the checked part of the checked body and the connector 32 (female) is selected so that the length of the coil line material 30 can be most closed to the surrounding length of the checked part in the checked body. Then, after the connector (male) 31 is connected and the lead wire 34 is connected to the pre-amplifier, measurement is executed.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、核磁気共鳴現象を利用して被検体の断層画像
を得る核磁気共鳴イメージング装置に関し、特に被検体
の体格の個人差を補償するのに好適な高周波コイルを備
えた核磁気共鳴イメージング装置に関するものである。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a nuclear magnetic resonance imaging apparatus that obtains tomographic images of a subject using nuclear magnetic resonance phenomena, and in particular, to a nuclear magnetic resonance imaging apparatus that uses nuclear magnetic resonance phenomena to obtain a tomographic image of a subject. The present invention relates to a nuclear magnetic resonance imaging apparatus equipped with a high-frequency coil suitable for the imaging.

〔従来の技術〕[Conventional technology]

従来の装置は、平均的な人体寸法に合わせた固定形状の
高周波コイルを用いていた。そのため、体格の特に大き
い人では高周波コイルが装着できない場合があったり、
逆に体格の小さい人では、装着はできるが画像のS/N
比が劣化するという問題があった。
Previous devices used radio frequency coils with a fixed shape that matched the average human body size. For this reason, high-frequency coils may not be able to be attached to particularly large people.
On the other hand, if you are a small person, you may be able to wear it, but the S/N of the image may be low.
There was a problem that the ratio deteriorated.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

上記従来技術は被検体の体格の個人差の点について配慮
がされておらず、体格の大きな人や妊婦などの場合、高
周波コイルを装着できない問題があった。一方、体格の
小さい人に対しては高周波コイルが装着できても最適形
状より大きすぎるため、得られる画像のS/N比が劣化
する1、J題があった。
The above-mentioned conventional technology does not take into consideration the individual differences in the physique of the subject, and there is a problem in that the high-frequency coil cannot be attached to a large person or a pregnant woman. On the other hand, even if a high-frequency coil can be attached to a person with a small physique, it is too large than the optimal shape, resulting in problems 1 and J in which the S/N ratio of the obtained image deteriorates.

本発明の目的は上記体格の個人差を補償し、被検体ごと
に最適形状になるように調整が可能な高周波コイルを備
えた核磁気共鳴イメージング装置を提供することにある
An object of the present invention is to provide a nuclear magnetic resonance imaging apparatus equipped with a high-frequency coil that can compensate for the individual differences in physique and adjust the shape to be optimal for each subject.

〔課題を解決するための手段〕 上記目的は被検体の体軸方向又はこれと直交する方向に
静磁場を発生する手段を有するとともに。
[Means for Solving the Problems] The above object includes means for generating a static magnetic field in the body axis direction of the subject or in a direction orthogonal thereto.

該被検体に近接して配置され該被検体に電磁波を照射し
かつ該被検体から放出される電磁波を検出する高周波コ
イルを有する核磁気共鳴イメージング装置において、該
高周波コイルを可撓性を有する素材で形成したことを特
徴とする核磁気共鳴イメージング装置で達成することが
できる。
In a nuclear magnetic resonance imaging apparatus having a high-frequency coil that is disposed close to the subject and irradiates the subject with electromagnetic waves and detects electromagnetic waves emitted from the subject, the high-frequency coil is made of a flexible material. This can be achieved with a nuclear magnetic resonance imaging device characterized by being formed with.

また、高周波コイルの素材としては、フラットケーブル
やFPC(フレキシブル・プリント基板)のようなもの
を選び、コイル線材部の長さを変えることにより、被検
体の体格に合った最適形状調節が可能となる。
In addition, by selecting a material such as a flat cable or FPC (flexible printed circuit board) for the high-frequency coil, and changing the length of the coil wire, it is possible to adjust the shape to suit the physique of the subject. Become.

〔作用〕[Effect]

フラットケーブルのような可撓性のある素材で構成した
高周波コイルは、被検体の検査部位に沿って巻きつける
ことが可能であり、例えばケーブルの数箇所に取りつけ
てコネクタを選択することで被検体の体格に応じて最適
寸法の高周波コイルを設定することが可能となる。それ
により、被検体の体格、検査部位の大きさに依らず最適
受信状態が得られ、高画質を維持できる。
A high-frequency coil made of a flexible material such as a flat cable can be wrapped around the test area of the test subject.For example, by attaching it to several locations on the cable and selecting connectors, the high-frequency coil can It becomes possible to set a high-frequency coil with optimal dimensions according to the person's physique. As a result, an optimal reception condition can be obtained regardless of the physique of the subject and the size of the examination site, and high image quality can be maintained.

〔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。
Embodiments of the present invention will be described in detail below with reference to the accompanying drawings.

第5図は核磁気共鳴イメージング装置の全体構成を示す
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(NM)現象を利用して被検体の断層画像
を得るもので、静磁場発生磁石10と、中央処理装置(
CPU)11と、シーケンサ12と、送信系13と、磁
場勾配発生系14と、受信系15と信号処理系16とか
ら成る。
FIG. 5 is a block diagram showing the overall configuration of the nuclear magnetic resonance imaging apparatus. This nuclear magnetic resonance imaging device obtains a tomographic image of a subject by using the nuclear magnetic resonance (NM) phenomenon, and includes a static magnetic field generating magnet 10, a central processing unit (
It consists of a CPU) 11, a sequencer 12, a transmission system 13, a magnetic field gradient generation system 14, a reception system 15, and a signal processing system 16.

上記静磁場発生磁石10は、被検体1の周りにその体軸
方向または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が配置されている。上記シーケン
サ12は、CPU11の制御で動作し、被検体1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
磁場勾配発生系14並びに受信系15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
成り、上記高周波発振器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1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1に照射されるようになっている。上記磁場勾配発
生系14は、x、y、zの三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とから成り、上記シーケンサ12からの命令に従
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。
The static magnetic field generating magnet 10 generates a strong and uniform static magnetic field around the subject 1 in the body axis direction or in a direction perpendicular to the body axis, and is used to generate a strong and uniform static magnetic field around the subject 1 in a certain expanse of space around the subject 1. A magnetic field generating means of a permanent magnet type, a normal conduction type, or a superconducting type is arranged in the magnetic field. The sequencer 12 operates under the control of the CPU 11 and sends various commands necessary for data collection of tomographic images of the subject 1 to the transmission system 13, magnetic field gradient generation system 14, and reception system 15. 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. However, by amplifying this amplitude-modulated high-frequency pulse with a high-frequency amplifier 19 and then supplying it to a high-frequency coil 20a placed close to the subject 1, the subject 1 is irradiated with electromagnetic waves. There is. The magnetic field gradient generation system 14 is composed of gradient magnetic field coils 21 wound in the three axes of x, y, and z, and a gradient magnetic field power supply 22 that drives each coil. X by driving the gradient magnetic field power supply 22 of the coil.

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l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、受信側のソレノイド形の高
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とから成り、上記送信側の高周波コイ
ル20a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
グされた二系列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、CPUI 1と、磁気ディスク26及び磁気テ
ープ27等の記録装置と、CRT等のデイスプレィ28
とから成り、上記CPUIIでフーリエ変換、補正係数
計算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
を画像化してデイスプレィ28に表示するようになって
いる。なお、第5図において、送信側及び受信側の高周
波コイル20a、20bと傾斜磁場コイル21は、被検
体1の周りの空間に配置された静磁場発生磁石10の磁
場空間内に配置されている。
Gradient magnetic fields Gx, Gy, and Gz in three y- and z-axis directions are applied to the subject 1. Depending on how this gradient magnetic field is applied, a slice plane for the subject l can be set. The receiving system 15 includes a solenoid-type high-frequency coil 20b on the receiving side, an amplifier 23, a quadrature phase detector 24, and an A/D converter 25. The electromagnetic wave (NMR signal) of response 1 is detected by a high frequency coil 20b placed close to the subject 1, and is inputted to an A/D converter 25 via an amplifier 23 and a quadrature phase detector 24 to be converted into a digital quantity. The signal is converted into two series of collected data which are further sampled by the quadrature phase detector 24 at the timing according to the command from the sequencer 12, and the signals are sent to the signal processing system 16. This signal processing system 16 includes a CPU 1, a recording device such as a magnetic disk 26 and a magnetic tape 27, and a display 28 such as a CRT.
The CPU II performs processing such as Fourier transformation, correction coefficient calculation, and image reconstruction, and the signal intensity distribution of an arbitrary cross section or the distribution obtained by performing appropriate calculations on a plurality of signals is converted into an image and displayed on the display 28. It is designed to be displayed. In addition, in FIG. 5, the high-frequency coils 20a, 20b and the gradient magnetic field coil 21 on the transmitting side and the receiving side are arranged in the magnetic field space of the static magnetic field generating magnet 10 arranged in the space around the subject 1. .

本発明の第一の実施例の要部である高周波コイル部分を
第1図及び第2図に示す。第1図に示すような高周波コ
イル2oのコイル線材30は柔軟なコイル線材、例えば
フラットケーブルとかFPC(フレキシブル・プリント
基板のような材料で構成する。また高周波コイル20に
は非磁性材で、高周波損失の少ない材料、例えばエポキ
シ樹脂やテフロン等の材料からなるコネクタ31.32
と静磁場強度により決定されるラーモア周波数に高周波
コイル20を同調するための同調回路33及びプリアン
プに接続するためのリード線34とを取付ける。コネク
タ(雌)32は、コイル線材3oの長さを複数箇選択で
きるように、コイル線材3oの適当な位置に複数箇数り
付けておく。高周波コイル20は搬像の際、被検体の検
査部位に沿ってコイル線材30を巻き、コイル線材30
の長さが被検体の検査部位の周囲長に最も近くなるよう
にコネクタ(雌)32を選択し、コネクタ(雄)31を
接続し、リード線34をプリアンプに接続した後に、計
測を行う。
A high-frequency coil portion, which is the main part of the first embodiment of the present invention, is shown in FIGS. 1 and 2. The coil wire 30 of the high-frequency coil 2o as shown in FIG. 1 is made of a flexible coil wire, such as a flat cable or FPC (flexible printed circuit board). Connectors 31, 32 made of materials with low loss, such as epoxy resin or Teflon.
A tuning circuit 33 for tuning the high frequency coil 20 to the Larmor frequency determined by the strength of the static magnetic field and a lead wire 34 for connecting to the preamplifier are attached. A plurality of connectors (female) 32 are attached at appropriate positions on the coil wire 3o so that a plurality of lengths of the coil wire 3o can be selected. During image transfer, the high-frequency coil 20 winds a coil wire 30 along the inspection site of the subject.
The connector (female) 32 is selected so that its length is closest to the circumference of the test site of the subject, the connector (male) 31 is connected, the lead wire 34 is connected to the preamplifier, and then measurement is performed.

従来技術では、コイル線材30の長さは一定であり、し
かも固形ボビン上に設置されていたため。
In the prior art, the length of the coil wire 30 was constant and was installed on a solid bobbin.

被検体の検査部位に応じて高周波コイル20の最適寸法
を調整することが不可能であり、被検体の個人差による
画質のばらつきが見られた。しかし。
It is impossible to adjust the optimum dimensions of the high-frequency coil 20 according to the examination site of the subject, and variations in image quality are observed due to individual differences among the subjects. but.

本発明によれば上記調整が可能となった。According to the present invention, the above adjustment has become possible.

第2図に高周波コイル2oのコイル線材3oの長さの調
整例を示す。第2図(a)はコネクタ(雌)32を3箇
取り付けた例で、コイル線材30の長さを最大にした場
合である。コネクタ(雄)31を最も端に近いコネクタ
(雌)32に接続することにより得られる。コネクタ(
雌)32を端から順次内側のものに変えて接続すること
により、コイル線材30は順次短くなる。第2図(b)
はコイル線材30を最短にした場合を示す。この場合、
環状をなすコイルの外側の余分なコネクタ (雌)32
と共に余ったコイル線材はコイルの機能をもたない。上
記の実施原理に基づいてコイル線材30の長さ及びコネ
クタ(雌)32の筒数、取付間隔を変えることにより、
被検体体格の個人差及び検査部位の大きさの違いを補償
した高周波コイル20を構成できる。上記高周波コイル
を使用することにより、高周波コイルの装着の問題や被
検体の個人差による画質のばらつきの問題が解決できる
FIG. 2 shows an example of adjusting the length of the coil wire 3o of the high frequency coil 2o. FIG. 2(a) shows an example in which three connectors (female) 32 are attached, and the length of the coil wire 30 is maximized. This is obtained by connecting the connector (male) 31 to the connector (female) 32 closest to the end. connector(
By changing the female (female) 32 from the end to the inner one and connecting them, the coil wire 30 becomes gradually shorter. Figure 2(b)
shows the case where the coil wire 30 is made the shortest. in this case,
Extra connector (female) 32 on the outside of the ring-shaped coil
The remaining coil wire material does not have the function of a coil. By changing the length of the coil wire 30, the number of tubes of the connector (female) 32, and the installation interval based on the above implementation principle,
It is possible to configure the high-frequency coil 20 that compensates for individual differences in the physique of the subject and differences in the size of the test site. By using the above-described high-frequency coil, it is possible to solve the problem of mounting the high-frequency coil and the problem of variations in image quality due to individual differences in subjects.

第3図に第二の実施例を示す。第2図に示した第一の実
施例ではコイル線材30の長さの調整間隔がコネクタ(
雌)32の配列の間隔によって決まる。コネクタ(雌)
32を配列する際、通常−定の間隔で配列することにな
るため、被検体の体格にちょうど合うコイル線材30の
長さが2箇のコネクタ(雌)32の間に来る場合もあり
得る。
FIG. 3 shows a second embodiment. In the first embodiment shown in FIG. 2, the adjustment interval of the length of the coil wire 30 is
Female) Determined by the spacing of the 32 arrays. Connector (female)
When arranging the coil wires 32, they are usually arranged at regular intervals, so the length of the coil wire 30 that exactly matches the physique of the subject may be located between the two connectors (female) 32.

このような場合に第3図(a)に示した実施例が適当で
ある。基本的な構成は第2図、と同じで、コイル線材3
0、コネクタ31,32、同調回路33、リード線34
から構成される。しがし第3図では、高周波コイルを一
重のループにするための接続部に面ファスナ36を用い
る点で、第2図のコネクタのみで接続するものと大きく
異なる。
In such a case, the embodiment shown in FIG. 3(a) is appropriate. The basic configuration is the same as in Figure 2, with coil wire 3
0, connectors 31, 32, tuning circuit 33, lead wire 34
It consists of However, in FIG. 3, a hook-and-loop fastener 36 is used as the connecting portion to form a single loop between the high-frequency coils, which is greatly different from the connection using only the connector shown in FIG. 2.

面ファスナ36を用いると接続部の長さを可変範囲内で
任意に変えられるので被検体の体格に最も合う位置でコ
イル線材30のループを形成することができる。面フア
スナ自身には導電性が無く、機械的な固定機能を有する
のみであるので、電気的な接続は面ファスナによる固定
後、接続#!35の先端にあるコネクタ(雄)31をコ
ネクタ(雌)32に接続することで行われる。接続線3
5は面ファスナ36をその接続可変範囲内のどの位置に
固定したときでも、コネクタ31.32の接続が可能に
なる長さにしである。本実施例ではコネクタ31.32
に力が加わることなく高周波コイルを被検体体幹部に固
定することが可能となる。
When the hook-and-loop fastener 36 is used, the length of the connecting portion can be arbitrarily changed within a variable range, so that a loop of the coil wire 30 can be formed at a position that best suits the physique of the subject. Since the hook-and-loop fastener itself has no conductivity and only has a mechanical fixing function, the electrical connection is made after fixing with the hook-and-loop fastener. This is done by connecting the connector (male) 31 at the tip of the connector 35 to the connector (female) 32. Connection line 3
The length 5 is such that the connectors 31 and 32 can be connected whenever the hook and loop fastener 36 is fixed at any position within its variable connection range. In this example, connectors 31 and 32
It becomes possible to fix the high-frequency coil to the trunk of the subject's body without applying force to the body.

第4図に第三の実施例を示す。本実施例の高周波コイル
20は、コイル線材3o、同調回路33、リード線34
、ローラ37.ローラ圧着ピン38から構成されている
。第3図と異なる点は、面ファスナで固定する代りにロ
ーラとローラ圧着ピンで固定することである。コイル線
材30の長さは従来の固形ボビン上に設置したものと同
様一定であるが、分割のない一重コイルである。第4図
(b)の如く被検体の検査部位に高周波コイルを取付け
たときは、被検体の検査部位に密着するようにローラ3
7とローラ圧着ピン38により調整する。被検体に取付
ける際の便宜上、途中にコネクタ31.32を入れて2
分割することもできる。
FIG. 4 shows a third embodiment. The high frequency coil 20 of this embodiment includes a coil wire 3o, a tuned circuit 33, and a lead wire 34.
, roller 37. It is composed of a roller pressure pin 38. The difference from FIG. 3 is that instead of fixing with hook-and-loop fasteners, it is fixed with rollers and roller pressure pins. The length of the coil wire 30 is constant like that installed on a conventional solid bobbin, but it is a single coil without division. When the high-frequency coil is attached to the test site of the test subject as shown in Figure 4(b), the roller 3 should be placed in close contact with the test site of the test subject.
7 and roller crimp pin 38. For convenience when attaching to the test object, insert connectors 31 and 32 in the middle.
It can also be divided.

〔発明の効果〕〔Effect of the invention〕

本発明は以上説明したように、被検体に電磁波を照射し
たり、または被検体から放出される電磁波を検出するソ
レノイド形の高周波コイルをフラットケーブルのような
可撓性のある素材で構成することで高周波コイルを被検
体の検査部位に沿って巻きつけることが可能となる。ま
た高周波コイルを機械的に2分割し、複数個のコネクタ
を設けることで上記被検体の体格個人差に依らず最適寸
法に高周波コイルを調節できる。それにより、被検体の
体格、検査部位の大きさに依らず最適寸法の高周波コイ
ルを構成することができ、個人差による画質のばらつき
を軽減し、高画質を維持できる効果がある。
As explained above, the present invention includes a solenoid-shaped high-frequency coil that irradiates electromagnetic waves to a subject or detects electromagnetic waves emitted from the subject, which is made of a flexible material such as a flat cable. This makes it possible to wrap the high-frequency coil along the test site of the subject. Furthermore, by mechanically dividing the high-frequency coil into two and providing a plurality of connectors, the high-frequency coil can be adjusted to an optimal size regardless of the individual differences in body size of the subject. As a result, it is possible to configure a high-frequency coil with an optimal size regardless of the physique of the subject and the size of the examination site, which has the effect of reducing variations in image quality due to individual differences and maintaining high image quality.

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

第1図は本発明の一実施例の高周波コイルの全体構成を
示す説明図、第2図は上記高周波コイルの使用状態を示
す説明図、第3図、第4図はその他の実施例の高周波コ
イルを示す説明図、第5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を示すブロック図である。 1・・・被検体、10・・・静磁場発生磁石、11・・
・CPU(中央処理装置)、12・・・シーケンサ、1
3・・・送信系、14・・・磁場勾配発生系、15・・
・受信系、16・・・信号処理系、20・・・高周波コ
イル、3o・・・コイル線材、31・・・コネクタ(雄
)、32・・・コネクタ(雌)、33・・・同調回路、
34・・・リード線。 35・・・接続線、36・・・面ファスナ、37・・・
ローラ、票I図 第 図 茶 図 (ω
FIG. 1 is an explanatory diagram showing the overall configuration of a high-frequency coil according to an embodiment of the present invention, FIG. 2 is an explanatory diagram showing how the above-mentioned high-frequency coil is used, and FIGS. 3 and 4 are high-frequency diagrams of other embodiments. FIG. 5 is a block diagram showing the overall configuration of the nuclear magnetic resonance imaging apparatus according to the present invention. 1... Subject, 10... Static magnetic field generating magnet, 11...
・CPU (Central Processing Unit), 12...Sequencer, 1
3... Transmission system, 14... Magnetic field gradient generation system, 15...
・Reception system, 16... Signal processing system, 20... High frequency coil, 3o... Coil wire, 31... Connector (male), 32... Connector (female), 33... Tuning circuit ,
34... Lead wire. 35... Connection wire, 36... Velcro fastener, 37...
Laura, chart I, chart tea (ω

Claims (1)

【特許請求の範囲】 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
に近接させて配置され該被検体に電磁波を照射しかつ該
被検体から放出される電磁波を検出する高周波コイルを
有する核磁気共鳴イメージング装置において、該高周波
コイルを可撓性を有する素材で形成したことを特徴とす
る核磁気共鳴イメージング装置。 2、高周波コイルを切断し、その一端にコネクタ(雄、
又は雌)を、他端にコイル線材の長さ方向に沿つて間隔
を置いて複数箇のコネクタ(雌、又は雄)を取付け、該
コネクタの接続を変えることにより該高周波コイルのル
ープ長を変えることができるようにしたことを特徴とす
る特許請求の範囲第1項記載の核磁気共鳴イメージング
装置。 3、高周波コイルを切断し、その一端にコネクタ(雌、
又は雄)及び面ファスナの片側を、他端にコネクタ(雄
、又は雌)及び面ファスナの残りの片側を取付け、該面
ファスナの接続長さを変えることにより該高周波コイル
のループ長を変えることができ、該高周波コイルの導通
はコネクタの接続により行うことを特徴とする特許請求
の範囲第1項記載の核磁気共鳴イメージング装置。 4、高周波コイルにローラ等の止め具を取付け、該止め
具の位置を変えることにより該高周波コイルのループ長
を変えることができるようにしたことを特徴とする特許
請求の範囲第1項記載の核磁気共鳴イメージング装置。
[Claims] 1. A magnet that generates a static magnetic field in the direction of the body axis of the subject or in a direction perpendicular thereto, and is placed close to the subject and irradiates the subject with electromagnetic waves. A nuclear magnetic resonance imaging apparatus comprising a high frequency coil for detecting electromagnetic waves emitted from the subject, characterized in that the high frequency coil is made of a flexible material. 2. Cut the high frequency coil and attach a connector (male,
Attach a plurality of connectors (female or male) to the other end of the coil wire at intervals along the length direction of the coil wire, and change the loop length of the high-frequency coil by changing the connections of the connectors. The nuclear magnetic resonance imaging apparatus according to claim 1, wherein the nuclear magnetic resonance imaging apparatus is configured to be able to perform the following functions. 3. Cut the high frequency coil and attach a connector (female,
Or attach a connector (male or female) and the remaining side of the hook-and-loop fastener to one end of the hook-and-loop fastener, and change the loop length of the high-frequency coil by changing the connection length of the hook-and-loop fastener. 2. The nuclear magnetic resonance imaging apparatus according to claim 1, wherein the high-frequency coil is electrically connected by connecting a connector. 4. A stopper such as a roller is attached to the high-frequency coil, and the loop length of the high-frequency coil can be changed by changing the position of the stopper. Nuclear magnetic resonance imaging device.
JP63152341A 1988-06-22 1988-06-22 Nuclear magnetic resonance imaging device Pending JPH024328A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63152341A JPH024328A (en) 1988-06-22 1988-06-22 Nuclear magnetic resonance imaging device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63152341A JPH024328A (en) 1988-06-22 1988-06-22 Nuclear magnetic resonance imaging device

Publications (1)

Publication Number Publication Date
JPH024328A true JPH024328A (en) 1990-01-09

Family

ID=15538423

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63152341A Pending JPH024328A (en) 1988-06-22 1988-06-22 Nuclear magnetic resonance imaging device

Country Status (1)

Country Link
JP (1) JPH024328A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009011836A (en) * 2007-07-02 2009-01-22 Siemens Ag Assembly for laying patient

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6159806A (en) * 1984-08-31 1986-03-27 Hitachi Ltd High-frequency coil for nmr imaging device
JPS6343509B2 (en) * 1981-04-24 1988-08-31 Asahi Glass Co Ltd

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6343509B2 (en) * 1981-04-24 1988-08-31 Asahi Glass Co Ltd
JPS6159806A (en) * 1984-08-31 1986-03-27 Hitachi Ltd High-frequency coil for nmr imaging device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009011836A (en) * 2007-07-02 2009-01-22 Siemens Ag Assembly for laying patient

Similar Documents

Publication Publication Date Title
JP3562902B2 (en) RF probe for magnetic resonance imaging equipment
JP4554056B2 (en) Unique uncoupled sandwich solenoid array coil
US5682098A (en) Open quadrature whole volume imaging NMR surface coil array including three figure-8 shaped surface coils
US5327898A (en) Signal receiving coil device for MRI apparatus
US7061242B2 (en) Magnetic resonance imaging system
JP3411631B2 (en) RF probe and magnetic resonance imaging apparatus
US4887038A (en) Solenoidal surface coils for magnetic resonance imaging
JPH0454451B2 (en)
US4831330A (en) Probe for magnetic resonance imaging system
JP4588830B2 (en) RF coil array device for vertical magnetic field MRI
JPH04332531A (en) Inspecting device using nuclear magnetic resonance
JPH0268036A (en) Nuclear magnetic resonance imaging device
JPH024328A (en) Nuclear magnetic resonance imaging device
JPH048348A (en) Receiving coil for magnetic resonance imaging device
JPH07163543A (en) High-frequency signal receiving coil of magnetic resonance imaging system
JP2860682B2 (en) Method for stabilizing static magnetic field uniformity of magnetic resonance imaging apparatus
JPH0947444A (en) Rf probe for magnetic resonance device
WO2011016398A1 (en) Magnetic resonance measurement device
JPH0630165Y2 (en) Receiver coil for nuclear magnetic resonance imaging
JP2650955B2 (en) Inspection equipment using nuclear magnetic resonance
JP3213819B2 (en) High frequency receiving coil for magnetic resonance imaging equipment
JPS62172940A (en) Magnetic resonance imaging apparatus
JP3007383B2 (en) Magnetic resonance imaging equipment
JPH05161624A (en) High frequency reception coil for magnetic resonance imaging device
JPH0392137A (en) Receiving coil for nuclear magnetic resonance imaging apparatus