JPH04282132A - Nuclear magnetic resonance device - Google Patents

Nuclear magnetic resonance device

Info

Publication number
JPH04282132A
JPH04282132A JP3072436A JP7243691A JPH04282132A JP H04282132 A JPH04282132 A JP H04282132A JP 3072436 A JP3072436 A JP 3072436A JP 7243691 A JP7243691 A JP 7243691A JP H04282132 A JPH04282132 A JP H04282132A
Authority
JP
Japan
Prior art keywords
surface coil
magnetic field
magnetic resonance
sensitivity
nuclear magnetic
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.)
Granted
Application number
JP3072436A
Other languages
Japanese (ja)
Other versions
JP3136631B2 (en
Inventor
Yoshikuni Matsunaga
良国 松永
Tetsuhiko Takahashi
哲彦 高橋
Etsuji Yamamoto
山本 悦治
Ryuichi Suzuki
隆一 鈴木
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 Ltd
Hitachi Healthcare Manufacturing Ltd
Original Assignee
Hitachi Ltd
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 Ltd, Hitachi Medical Corp filed Critical Hitachi Ltd
Priority to JP03072436A priority Critical patent/JP3136631B2/en
Priority to US07/793,456 priority patent/US5280246A/en
Publication of JPH04282132A publication Critical patent/JPH04282132A/en
Application granted granted Critical
Publication of JP3136631B2 publication Critical patent/JP3136631B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Abstract

PURPOSE:To extend the visual field without occurring uneven sensitivity at the time of placing the surface coil of unclear magnetic resonance device of vertical magnetic field system like an array. CONSTITUTION:In the nuclear magnetic resonance device of vertical magnetic field system, each surface coil for constituting a surface coil used therefor is placed like an array by overlapping mutually in its sensitivity uniform direction so as to become the minimum mutual coupling to other unit surface coil being adjacent thereto.

Description

【発明の詳細な説明】[Detailed description of the invention]

【0001】0001

【産業上の利用分野】本発明は被検体中の水素や燐等か
らの核磁気共鳴(以下、「NMR」という)信号を測定
し、核の密度分布や緩和時間分布等を映像化するNMR
装置に関し、特にそれに用いられる表面コイルを改良し
たNMR装置に関する。
[Industrial Application Field] The present invention is an NMR system that measures nuclear magnetic resonance (hereinafter referred to as "NMR") signals from hydrogen, phosphorus, etc. in a sample and visualizes the density distribution, relaxation time distribution, etc. of nuclei.
The present invention relates to an NMR apparatus, and particularly to an NMR apparatus with an improved surface coil used therein.

【0002】0002

【従来の技術】従来、NMR装置においては、被検体(
例えば、人)の関心部位を取り巻く各種の頭部用コイル
や腹部用コイル,心臓等の動きの影響を受けにくい表面
コイル等を用い被検体の検査,撮像が行われてきた。と
ころで、上記表面コイルは、上記頭部用コイルや腹部用
コイルに比べて高感度であるが、視野が制限されてしま
うため、脊椎等の如く広範囲を検査する際には、上記表
面コイルを検査対象に沿って移動させ、数回撮像しなけ
ればならず、検査時間が長くかかるという問題が発生し
ていた。これに対しては、例えば、特開平2−1343
2号公報に開示されている如く、NMR装置に用いられ
る複数個の表面コイルを、各表面コイルが隣接する表面
コイルと相互結合しないよう適度にオーバラップさせて
配列し、上記各表面コイルで受信されたNMR信号を合
成することにより実質的に視野を広くする方法が提案さ
れている。
[Prior Art] Conventionally, in an NMR apparatus, an analyte (
For example, various types of head coils, abdominal coils, and surface coils that are less affected by the movement of the heart and the like have been used to examine and image a subject surrounding the body part of interest. By the way, the above-mentioned surface coil has higher sensitivity than the above-mentioned head coil and abdominal coil, but the field of view is limited, so when examining a wide area such as the spine, the above-mentioned surface coil is not used. This poses a problem in that it takes a long time to inspect because it has to be moved along the object and imaged several times. For this, for example, JP-A-2-1343
As disclosed in Publication No. 2, a plurality of surface coils used in an NMR apparatus are arranged with appropriate overlap so that each surface coil does not couple with an adjacent surface coil, and each surface coil receives signals. A method has been proposed in which the field of view is substantially widened by synthesizing the NMR signals obtained.

【0003】0003

【発明が解決しようとする課題】しかしながら、上記従
来技術は、静磁場が垂直磁場方式のNMR装置で用いら
れる表面コイル特有の感度分布については配慮されてお
らず、上述の表面コイルを配列させる方向によっては感
度むらが生ずるという問題があった。本発明は上記事情
に鑑みてなされたもので、その目的とするところは、従
来の技術における上述の如き問題を解消し、上述の表面
コイルが一方向に有する感度均一方向と、該表面コイル
を配列して成る「表面コイルアレイ」の配列方向とを一
致させ、感度むらを生じさせずに視野を拡張可能とする
NMR装置を提供することにある。
[Problems to be Solved by the Invention] However, the above-mentioned conventional technology does not take into account the sensitivity distribution peculiar to the surface coil used in an NMR apparatus in which the static magnetic field is a vertical magnetic field, and the direction in which the above-mentioned surface coils are arranged is not considered. In some cases, there is a problem in that sensitivity unevenness occurs. The present invention has been made in view of the above circumstances, and its purpose is to solve the above-mentioned problems in the conventional technology, and to improve the uniform sensitivity direction that the surface coil has in one direction, and to It is an object of the present invention to provide an NMR device that can extend the field of view without causing sensitivity unevenness by aligning the arrangement direction of a "surface coil array" formed by the arrangement.

【0004】0004

【課題を解決するための手段】本発明の上記目的は、所
定の空間に第1の方向に沿った磁場を形成し、前記空間
内に置かれた被検体の核スピンを高周波磁場により励起
し、前記核スピンによる高周波信号を検出する、垂直磁
場方式のNMR装置において、該NMR装置用の表面コ
イルを構成する各単位表面コイルが、それに隣接する他
の単位表面コイルと最小の相互結合となる如く、その感
度均一方向に相互にオーバラップして配列されたことを
特徴とするNMR装置によって達成される。
[Means for Solving the Problems] The above object of the present invention is to form a magnetic field along a first direction in a predetermined space, and to excite the nuclear spins of a subject placed in the space with a high-frequency magnetic field. , in a vertical magnetic field type NMR device that detects high-frequency signals due to nuclear spins, each unit surface coil constituting the surface coil for the NMR device has minimal mutual coupling with other unit surface coils adjacent to it. This is achieved by an NMR device characterized by being arranged so as to overlap each other in the direction of uniform sensitivity.

【0005】[0005]

【作用】本発明に係るNMR装置においては、垂直磁場
方式のNMR装置で用いられる表面コイルが一方向に有
する感度均一方向と上記表面コイルを配列する際の配列
方向を一致させる如く構成したことにより、感度が均一
なままで視野を拡張できる。すなわち、表面コイルアレ
イ化時に感度均一性を損なわないので、感度むらが生じ
ない。
[Operation] In the NMR apparatus according to the present invention, the uniform sensitivity direction of the surface coil used in a vertical magnetic field type NMR apparatus in one direction is made to match the direction in which the surface coils are arranged. , the field of view can be expanded while sensitivity remains uniform. That is, since the sensitivity uniformity is not impaired when forming the surface coil array, sensitivity unevenness does not occur.

【0006】[0006]

【実施例】以下、本発明の実施例を図面に基づいて詳細
に説明する。図6は、本発明の一実施例を示すNMR装
置の構成図である。図中、1Aは後述する表面コイルア
レイ、2は被検体、6は本装置全体の制御を行う制御装
置、7は高周波パルス発生器、8は送信用増幅器、9は
後述する高周波プローブ、10は受信用増幅器、11は
位相敏感検波器、12は信号処理装置を示している。ま
た、13〜15は傾斜コイル、16〜18は傾斜コイル
ドライバ、19は静磁場コイル、20は被検体支持用の
ベッド、21はベッド支持台を示している。コイル19
は、その内部の空間に一定強度,一定方向(z軸方向)
の静磁場を発生する高周波コイルである。一方、3組の
傾斜コイル13,14,15は、それぞれ、傾斜コイル
ドライバ16,17,18により駆動され、上記静磁場
の強度に、それぞれ、z方向およびこれに直交するx方
向,y方向に沿った傾斜をつける。これらの各コイルの
内部には、筒状のボビンに形成された高周波プローブ9
が設置されている。また、支持台21の上には移動可能
なベッド20が装着され、被検体2とその背面に配置さ
れた表面コイルアレイ1Aは、上記ベッド20上に載置
されて前述の高周波プローブ9中に挿入される。高周波
パルス発生器7の出力は、送信用増幅器8で増幅されて
上記高周波プローブ9に与えられ、ここで高周波磁場が
発生する。本装置の動作の概要は下記の通りである。制
御装置6は、プログラムされたシーケンスに従って、各
傾斜コイルの駆動および高周波磁場の発生のタイミング
を制御し、被検体の核スピンを励起する。被検体2のN
MRによる高周波信号は、上記表面コイルアレイ1Aで
受信され、受信用増幅器10,位相敏感検波器11を介
して信号処理装置12に導かれる。信号処理装置12は
、サンプリングした受信データに処理を施し、図示され
ていない表示装置にNMR画像を写し出す。
Embodiments Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings. FIG. 6 is a configuration diagram of an NMR apparatus showing an embodiment of the present invention. In the figure, 1A is a surface coil array that will be described later, 2 is a subject, 6 is a control device that controls the entire device, 7 is a high-frequency pulse generator, 8 is a transmission amplifier, 9 is a high-frequency probe that will be described later, and 10 is a A receiving amplifier, 11 a phase sensitive detector, and 12 a signal processing device are shown. Further, 13 to 15 are gradient coils, 16 to 18 are gradient coil drivers, 19 is a static magnetic field coil, 20 is a bed for supporting a subject, and 21 is a bed support stand. coil 19
has a constant strength and constant direction (z-axis direction) in its internal space.
This is a high-frequency coil that generates a static magnetic field. On the other hand, the three sets of gradient coils 13, 14, and 15 are driven by gradient coil drivers 16, 17, and 18, respectively, and respond to the strength of the static magnetic field in the z direction and the x and y directions perpendicular thereto. Create a slope that follows. Inside each of these coils is a high frequency probe 9 formed on a cylindrical bobbin.
is installed. Further, a movable bed 20 is mounted on the support base 21, and the subject 2 and the surface coil array 1A arranged on its back are placed on the bed 20 and inserted into the high frequency probe 9 described above. inserted. The output of the high frequency pulse generator 7 is amplified by a transmitting amplifier 8 and given to the high frequency probe 9, where a high frequency magnetic field is generated. The outline of the operation of this device is as follows. The control device 6 controls the timing of driving each gradient coil and generating a high-frequency magnetic field according to a programmed sequence, and excites the nuclear spins of the subject. N of subject 2
The high frequency signal generated by MR is received by the surface coil array 1A, and guided to the signal processing device 12 via the receiving amplifier 10 and the phase sensitive detector 11. The signal processing device 12 processes the sampled received data and displays an NMR image on a display device (not shown).

【0007】図1は、前述の表面コイルアレイ1Aの具
体的実施例を示す図である。表面コイルアレイ1Aは、
縦横それぞれL,L’の長さを有する単位表面コイル1
a,1b(2個とは限らない)を一次元に配列したもの
であり、上述の単位表面コイル1aと1bは、相互結合
が最小となるような距離Dだけオーバラップさせてある
(例えば、L=170mm, L’=270mmの場合
、Dは約12mmとなる)。オーバラップ距離は、上記
単位表面コイルの縦横の長さの比L’/Lにより変化す
るものであることは言うまでもない。ところで、上述の
単位表面コイル1a,1bのそれぞれは、図2に示す如
く、単位表面コイルと水平な第1の方向(X方向)に磁
場を形成する。なお、このX方向には、途中で磁場強度
が落ちこむ不均一な磁場分布が存在するが、第2の方向
(Y方向)には、均一な磁場分布を有する。なお、図2
中の等高線は、感度の均一度分布を示している。そこで
、本実施例では、図1に示す如く、上記単位表面コイル
1a,1bを、該単位表面コイル1a,1bが有する感
度均一方向(第2の方向)に、相互結合が最小となるよ
うな距離Dだけオーバラップさせて配列し、表面コイル
アレイ1Aを形成する。すなわち、上記単位表面コイル
1a,1bの感度均一方向と表面コイルアレイ1Aの配
列方向を一致させる。これにより、上記表面コイルアレ
イ1Aは、上述の第2の方向(Y方向)での感度均一性
を損なわないので、感度むらを生ずることなく視野を拡
張することが可能となる。図4に、上記表面コイルアレ
イ1Aの使用状態を示す。感度均一方向と配列方向とを
一致させ、相互結合が最小になるように一次元上に配置
された表面コイルアレイ1Aは、被検体2の撮像したい
部位に絶縁され、固定される。例えば、脊椎を撮像した
い場合、頸椎から腰椎にかけて複数個(図では、2個)
の単位表面コイルが体軸方向に一次元に配置される。こ
れにより、大型化された均一磁場領域が体軸方向に形成
され、脊椎撮像を容易に行うことが可能になる。
FIG. 1 is a diagram showing a specific embodiment of the above-mentioned surface coil array 1A. The surface coil array 1A is
Unit surface coil 1 having lengths L and L' length and width respectively
a, 1b (not limited to two) are arranged in one dimension, and the above-mentioned unit surface coils 1a and 1b are overlapped by a distance D that minimizes mutual coupling (for example, If L=170mm and L'=270mm, D will be approximately 12mm). It goes without saying that the overlap distance varies depending on the length and width ratio L'/L of the unit surface coil. By the way, each of the unit surface coils 1a and 1b described above forms a magnetic field in a first direction (X direction) horizontal to the unit surface coils, as shown in FIG. Note that in the X direction, there is an uneven magnetic field distribution in which the magnetic field strength drops halfway, but in the second direction (Y direction), there is a uniform magnetic field distribution. In addition, Figure 2
The contour lines inside indicate the uniformity distribution of sensitivity. Therefore, in this embodiment, as shown in FIG. 1, the unit surface coils 1a, 1b are arranged in a direction (second direction) of uniform sensitivity that the unit surface coils 1a, 1b have so that the mutual coupling is minimized. They are arranged so as to overlap by a distance D to form a surface coil array 1A. That is, the uniform sensitivity direction of the unit surface coils 1a and 1b is made to match the arrangement direction of the surface coil array 1A. Thereby, the surface coil array 1A does not impair the sensitivity uniformity in the second direction (Y direction), so that it is possible to expand the field of view without causing sensitivity unevenness. FIG. 4 shows how the surface coil array 1A is used. The surface coil array 1A, which is arranged one-dimensionally so that the direction of uniform sensitivity and the arrangement direction coincide with each other and mutual coupling is minimized, is insulated and fixed to a region of the subject 2 to be imaged. For example, if you want to image the spine, there are multiple images (two in the figure) from the cervical vertebrae to the lumbar vertebrae.
unit surface coils are arranged one-dimensionally in the body axis direction. As a result, an enlarged uniform magnetic field region is formed in the body axis direction, making it possible to easily perform spine imaging.

【0008】図5に、前述の実施例に示した表面コイル
アレイ1Aの駆動回路のブロック図を示す。感度均一方
向と配列方向とを一致させ、一次元に配列された表面コ
イルアレイ1Aの各単位表面コイル1a,1bの信号取
出し点には、それぞれ、インピーダンス整合回路を有す
るプリアンプ3が接続され、このプリアンプ3の出力端
は、装置使用者によって任意に選択可能な選択回路4を
介して加算器5に導かれ、位相敏感検波器11へ接続さ
れる。なお、必要に応じてプリアンプ3の出力にフェー
ズシフタを追加し、位相ずれを調整することも可能であ
る。実際の検査においては、例えば、脊椎の検査の場合
、広い撮像視野が要求されるので、上記表面コイルアレ
イ1Aを用い、実質的に単位表面コイル2個分と等価な
視野で撮像を行う。この場合、単位表面コイル1a,1
bで受信された被検体からのNMR信号は、それぞれ、
プリアンプ3で増幅され、必要に応じてフェーズシフタ
で位相ずれを調整されて選択回路4を通過し、加算機5
で合成され、位相敏感検波器11へ送られ、矢状および
冠状断層像を得る。また、上述の矢状および冠状断層像
から特定の部位に着目して、その部位に対応した表面コ
イル(例えば、上記表面コイル1b)のみで、限られた
視野の撮像を行う。この場合、被検体2の特定の部位か
らのNMR信号は、単位表面コイル1a,1bでそれぞ
れ受信され、プリアンプ3でそれ備れ増幅され、必要に
応じてフェーズシフタで位相ずれを調整されて選択回路
4へ導かれる。選択回路4へ導かれたNMR信号のうち
、上述の単位表面コイル1bで受信されたもののみが後
段へ送られ、単位表面コイル1aで受信されたものは遮
断される。これらの動作により、被検体2の特定の部位
の矢状および冠状断層像が得られる。つまり、撮像視野
を任意に設定できる。これにより、フェーズエンコード
で決められる視野よりも広い感度分布を有することから
生じる折り返し現象を防ぐことができる。なお、単位表
面コイルは2個だけに限らず、複数の単位表面コイルを
用い、また、種々の単位表面コイルを組み合せることが
可能である。
FIG. 5 shows a block diagram of a drive circuit for the surface coil array 1A shown in the above embodiment. A preamplifier 3 having an impedance matching circuit is connected to the signal extraction point of each unit surface coil 1a, 1b of the surface coil array 1A, which is arranged one-dimensionally so that the direction of uniform sensitivity matches the arrangement direction. The output terminal of the preamplifier 3 is led to an adder 5 via a selection circuit 4 which can be arbitrarily selected by the user of the device, and is connected to a phase sensitive detector 11. Note that it is also possible to add a phase shifter to the output of the preamplifier 3 to adjust the phase shift, if necessary. In actual examinations, for example, in the case of examining the spine, a wide imaging field of view is required, so the surface coil array 1A is used to perform imaging with a field of view substantially equivalent to two unit surface coils. In this case, unit surface coils 1a, 1
The NMR signals from the subject received at b are, respectively,
It is amplified by the preamplifier 3, the phase shift is adjusted by a phase shifter as necessary, and the signal is passed through the selection circuit 4, and then added to the adder 5.
are combined and sent to the phase sensitive detector 11 to obtain sagittal and coronal tomographic images. Further, by focusing on a specific region from the sagittal and coronal tomographic images described above, imaging of a limited field of view is performed using only the surface coil (for example, the surface coil 1b) corresponding to that region. In this case, NMR signals from specific parts of the subject 2 are received by the unit surface coils 1a and 1b, respectively amplified by the preamplifier 3, and selected after adjusting the phase shift by a phase shifter as necessary. Leads to circuit 4. Of the NMR signals guided to the selection circuit 4, only those received by the above-mentioned unit surface coil 1b are sent to the subsequent stage, and those received by the unit surface coil 1a are blocked. Through these operations, sagittal and coronal tomographic images of a specific region of the subject 2 are obtained. In other words, the imaging field of view can be set arbitrarily. Thereby, it is possible to prevent the aliasing phenomenon caused by having a sensitivity distribution wider than the field of view determined by phase encoding. Note that the number of unit surface coils is not limited to two, and it is possible to use a plurality of unit surface coils or to combine various unit surface coils.

【0009】図3は、本発明の他の実施例に係る、表面
コイルアレイ1Aの具体的構成例を示す図である。表面
コイルアレイ1Aは、縦がL1およびL2,横がL’の
長さである単位表面コイル1c,1dを一次元に配列し
たものであり、上記単位表面コイル1cと1dは、相互
結合が最小となるような距離Dだけオーバラップさせて
ある。オーバラップ距離Dは、上記単位表面コイルの縦
横の長さにより変化するものであることは前述の通りで
ある。本実施例が前述の実施例と異なる点は、単位表面
コイル1c,1dの縦の長さをL1およびL2と変えた
ことにより、相互結合を最小とするオーバラップ距離D
を大きくし、上記単位表面コイル1cと1dのオーバラ
ップ領域での感度落ち込みを小さくすることを可能とし
た点にある。本実施例においても、表面コイルアレイ1
Aは、前述の第2の方向(Y方向)での感度均一性を損
なわないので、感度むらを生ずることなく視野を拡張す
ることが可能となる。なお、上述の各実施例に示した、
高周波磁場の発生と高周波信号の受信を別々のコイルで
おこなうクロス方式の他に、高周波磁場の発生と高周波
信号の受信を同一のコイルでおこなうシングル方式があ
り、本発明に係る表面コイルアレイ1Aが用い得ること
は言うまでもないことである。
FIG. 3 is a diagram showing a specific example of the structure of a surface coil array 1A according to another embodiment of the present invention. The surface coil array 1A is a one-dimensional arrangement of unit surface coils 1c and 1d whose lengths are L1 and L2 and whose width is L', and the unit surface coils 1c and 1d have minimum mutual coupling. They are overlapped by a distance D such that As described above, the overlap distance D varies depending on the length and width of the unit surface coil. This embodiment differs from the previous embodiments by changing the vertical lengths of the unit surface coils 1c and 1d to L1 and L2, thereby minimizing the overlap distance D
The advantage is that it is possible to increase the sensitivity and reduce the drop in sensitivity in the overlapping region of the unit surface coils 1c and 1d. Also in this embodiment, the surface coil array 1
Since A does not impair the sensitivity uniformity in the second direction (Y direction), it is possible to expand the field of view without causing sensitivity unevenness. In addition, shown in each of the above-mentioned examples,
In addition to the cross method in which high-frequency magnetic field generation and high-frequency signal reception are performed using separate coils, there is a single method in which high-frequency magnetic field generation and high-frequency signal reception are performed using the same coil. Needless to say, it can be used.

【0010】0010

【発明の効果】以上、詳細に説明した如く、本発明によ
れば、垂直磁場方式のNMR装置において、表面コイル
が一方向に有する感度均一方向と、該表面コイルを配列
して成る「表面コイルアレイ」の配列方向とを一致させ
たことにより、感度むらを生じさせずに視野を拡張可能
とするNMR装置を実現できるという顕著な効果を奏す
るものである。
As described in detail above, according to the present invention, in a vertical magnetic field type NMR apparatus, the surface coil has a uniform sensitivity direction in one direction, and the "surface coil" formed by arranging the surface coil By matching the arrangement direction of the "array", it is possible to realize an NMR apparatus that can expand the field of view without causing sensitivity unevenness, which is a remarkable effect.

【0011】[0011]

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

【図1】本発明の一実施例を示すNMR装置に用いられ
る表面コイルアレイの具体的構成例を示す図である。
FIG. 1 is a diagram showing a specific example of the configuration of a surface coil array used in an NMR apparatus representing an embodiment of the present invention.

【図2】実施例に係る表面コイルの磁場(感度)分布を
示す図である。
FIG. 2 is a diagram showing the magnetic field (sensitivity) distribution of the surface coil according to the example.

【図3】本発明の他の実施例を示す図である。FIG. 3 is a diagram showing another embodiment of the present invention.

【図4】実施例の表面コイルアレイの使用状態を示す図
である。
FIG. 4 is a diagram showing how the surface coil array of the example is used.

【図5】実施例の表面コイルアレイを用いた回路のブロ
ック図である。
FIG. 5 is a block diagram of a circuit using the surface coil array of the example.

【図6】本発明の一実施例を示すNMR装置の構成図で
ある。
FIG. 6 is a configuration diagram of an NMR apparatus showing an embodiment of the present invention.

【符号の説明】[Explanation of symbols]

1a〜1d  単位表面コイル 1A  表面コイルアレイ 2  被検体 3  プリアンプ 4  選択回路 5  加算器 6  制御装置 7  高周波パルス発生器 8  送信用増幅器 9  高周波プローブ 10  受信用増幅器 11  位相敏感検波器 12  信号処理装置 13,14,15  傾斜コイル 16,17,18  傾斜コイルドライバ19  静磁
場コイル 20  ベッド 21  支持台
1a to 1d Unit surface coil 1A Surface coil array 2 Subject 3 Preamplifier 4 Selection circuit 5 Adder 6 Control device 7 High frequency pulse generator 8 Transmission amplifier 9 High frequency probe 10 Reception amplifier 11 Phase sensitive detector 12 Signal processing device 13 , 14, 15 Gradient coils 16, 17, 18 Gradient coil driver 19 Static magnetic field coil 20 Bed 21 Support stand

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】  所定の空間に第1の方向に沿った磁場
を形成し、前記空間内に置かれた被検体の核スピンを高
周波磁場により励起し、前記核スピンによる高周波信号
を検出する、垂直磁場方式の核磁気共鳴装置において、
該核磁気共鳴装置用の表面コイルを構成する各単位表面
コイルが、それに隣接する他の単位表面コイルと最小の
相互結合となる如く、その感度均一方向に相互にオーバ
ラップして配列されたことを特徴とする核磁気共鳴装置
1. Forming a magnetic field along a first direction in a predetermined space, exciting nuclear spins of a subject placed in the space with a high-frequency magnetic field, and detecting a high-frequency signal due to the nuclear spins. In a vertical magnetic field type nuclear magnetic resonance apparatus,
Each unit surface coil constituting the surface coil for the nuclear magnetic resonance apparatus is arranged so as to overlap each other in the direction of uniform sensitivity so as to minimize mutual coupling with other unit surface coils adjacent thereto. A nuclear magnetic resonance device featuring:
【請求項2】  前記表面コイルが静磁場方向と直交す
る平面内に配置されたことを特徴とする請求項1記載の
核磁気共鳴装置。
2. The nuclear magnetic resonance apparatus according to claim 1, wherein the surface coil is arranged in a plane perpendicular to the direction of the static magnetic field.
【請求項3】  前記表面コイルの配列方向,前記感度
均一方向が前記被検体の体軸方向と一致する如く配置さ
れたことを特徴とする請求項1または2記載の核磁気共
鳴装置。
3. The nuclear magnetic resonance apparatus according to claim 1, wherein the arrangement direction of the surface coils and the uniform sensitivity direction are arranged so as to coincide with the body axis direction of the subject.
JP03072436A 1990-11-16 1991-03-12 Nuclear magnetic resonance equipment Expired - Fee Related JP3136631B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP03072436A JP3136631B2 (en) 1991-03-12 1991-03-12 Nuclear magnetic resonance equipment
US07/793,456 US5280246A (en) 1990-11-16 1991-11-18 Nuclear magnetic resonance apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP03072436A JP3136631B2 (en) 1991-03-12 1991-03-12 Nuclear magnetic resonance equipment

Publications (2)

Publication Number Publication Date
JPH04282132A true JPH04282132A (en) 1992-10-07
JP3136631B2 JP3136631B2 (en) 2001-02-19

Family

ID=13489253

Family Applications (1)

Application Number Title Priority Date Filing Date
JP03072436A Expired - Fee Related JP3136631B2 (en) 1990-11-16 1991-03-12 Nuclear magnetic resonance equipment

Country Status (1)

Country Link
JP (1) JP3136631B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009268898A (en) * 2008-04-30 2009-11-19 General Electric Co <Ge> Tile displacement type receiver coil array with improved spatial coverage
JP2011007665A (en) * 2009-06-26 2011-01-13 Chugoku Electric Power Co Inc:The Magnetic measuring device, non-destructive inspection device, and arrangement method of detecting coil of magnetic sensor

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2009268898A (en) * 2008-04-30 2009-11-19 General Electric Co <Ge> Tile displacement type receiver coil array with improved spatial coverage
JP2011007665A (en) * 2009-06-26 2011-01-13 Chugoku Electric Power Co Inc:The Magnetic measuring device, non-destructive inspection device, and arrangement method of detecting coil of magnetic sensor

Also Published As

Publication number Publication date
JP3136631B2 (en) 2001-02-19

Similar Documents

Publication Publication Date Title
JP5047537B2 (en) Magnetic resonance elastography using multiple drives
CN100563555C (en) MR imaging apparatus and nuclear magnetic resonance RF receiving coil apparatus
CN100558296C (en) High frequency winding assembly and MR imaging apparatus
JPH11244260A (en) Mr method and device using microcoil arranged in inspection area
JPH0856928A (en) Mr modulus that determines core magnetization distribution by surface coil setting
US20150301143A1 (en) System and method for reduced field of view magnetic resonance imaging
US7498809B2 (en) Magnetic resonance imaging device with multiple RF coils applying half-pulse waveforms for selective excitation of a local region
JP5575454B2 (en) Magnetic resonance imaging system
JP2004358221A (en) Method and system for high-speed imaging using parallel mri
JPH07370A (en) Magnetic resonance imaging device and magnetic resonance imaging method
EP1260826A2 (en) Magnetic resonance imaging method with sub-sampling
JP2000241519A (en) Rf coil array device for vertical magnetic field mri
JP2006507071A (en) Magnetic resonance method
US6487436B1 (en) Switchable field of view apparatus and method for magnetic resonance imaging
JP2006175223A (en) Method and system for spatial-spectrum excitation by parallel radio frequency transmission
JP3342853B2 (en) Magnetic resonance imaging device
JP2002248089A (en) Apparatus and method for magnetic resonance imaging
US6492810B1 (en) Anti-aliasing magnetic resonance device which reduces aliasing from regions outside of the excitation volume
US6492811B1 (en) Multishot echo planar imaging fluoroscopic technique
JP5675044B2 (en) Magnetic resonance imaging system
JPH04282132A (en) Nuclear magnetic resonance device
JP3111045B2 (en) RF probe for magnetic resonance imaging
JP2007510488A (en) Parallel MR imaging method
JP2006175226A (en) Method and system for mr scan acceleration using selective excitation and parallel transmission
JPH04180733A (en) Surface coil for nuclear magnetic resonance device

Legal Events

Date Code Title Description
FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20091208

Year of fee payment: 9

LAPS Cancellation because of no payment of annual fees