JPH0318450B2 - - Google Patents

Info

Publication number
JPH0318450B2
JPH0318450B2 JP60018444A JP1844485A JPH0318450B2 JP H0318450 B2 JPH0318450 B2 JP H0318450B2 JP 60018444 A JP60018444 A JP 60018444A JP 1844485 A JP1844485 A JP 1844485A JP H0318450 B2 JPH0318450 B2 JP H0318450B2
Authority
JP
Japan
Prior art keywords
coil
conductive
arcuate
linear
conductive piece
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.)
Expired - Lifetime
Application number
JP60018444A
Other languages
Japanese (ja)
Other versions
JPS61176841A (en
Inventor
Hiroshi Ikeda
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.)
Jeol Ltd
Original Assignee
Nihon Denshi KK
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 Nihon Denshi KK filed Critical Nihon Denshi KK
Priority to JP60018444A priority Critical patent/JPS61176841A/en
Publication of JPS61176841A publication Critical patent/JPS61176841A/en
Publication of JPH0318450B2 publication Critical patent/JPH0318450B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/20Arrangements or instruments for measuring magnetic variables involving magnetic resonance
    • G01R33/28Details of apparatus provided for in groups G01R33/44 - G01R33/64
    • G01R33/32Excitation or detection systems, e.g. using radio frequency signals
    • G01R33/34Constructional details, e.g. resonators, specially adapted to MR
    • G01R33/34046Volume type coils, e.g. bird-cage coils; Quadrature bird-cage coils; Circularly polarised coils
    • G01R33/34069Saddle coils

Landscapes

  • Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Magnetic Resonance Imaging Apparatus (AREA)

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(NMR)装置のプローブ
に用いられる試料コイルに関し、特に高い周波数
まで感度良くNMR信号を検出できるコイルの構
造に関するものである。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a sample coil used in a probe of a nuclear magnetic resonance (NMR) device, and particularly relates to a coil structure that can detect NMR signals with high sensitivity up to high frequencies. be.

[従来技術] NMR装置では、試料を収容したプローブを一
様な静磁場内に配置し、プローブ内に試料に近接
して配置された試料コイルから励起用高周波磁界
を照射すると共に、試料の共鳴子からの共鳴信号
をこの試料コイルによつて受信し、受信回路を介
してコンピユータへ送り、フーリエ変換により
NMRスペクトルを得ている。その際、コイルと
試料の共鳴子との結合の良否がNMR装置の感度
を大きく左右するため、コイルの形状や構造には
大きな注意が払われている。超伝導磁石を用いる
NMR装置の場合、例えば第4図に示すような円
筒状の鞍形コイルが通常用いられて来た。第4図
の鞍形コイルは、試料を収容した試料管が配置さ
れる半径Rの円筒状領域の周囲に、2つの渦巻状
巻線コイル部分1,2が円筒軸Zの回りに対称に
配置されている。この渦巻状巻線コイル部分は、
円筒軸Zに平行な直線状部分1A,2Aと、円筒
軸Zに直角な平面内にある円弧状部分1B,2B
とから成つている。第5図は上記直線状部分Aを
円筒軸Zに直交する面で切断した断面図を示し、
半径Rの円周上に直線状部分1A,2AがY平面
を挟んで対称に配置され、このコイルによつてX
方向に高周波磁界が発生する。
[Prior art] In an NMR device, a probe containing a sample is placed in a uniform static magnetic field, and a high-frequency magnetic field for excitation is irradiated from a sample coil placed in the probe close to the sample. The resonance signal from the sample coil is received by the sample coil, sent to the computer via the receiving circuit, and processed by Fourier transformation.
Obtaining NMR spectra. At this time, great attention is paid to the shape and structure of the coil, as the quality of the coupling between the coil and the resonator of the sample greatly affects the sensitivity of the NMR device. Using superconducting magnets
In the case of an NMR apparatus, a cylindrical saddle-shaped coil as shown in FIG. 4, for example, has been commonly used. In the saddle-shaped coil shown in Fig. 4, two spirally wound coil parts 1 and 2 are arranged symmetrically around the cylindrical axis Z around a cylindrical region of radius R in which a sample tube containing a sample is arranged. has been done. This spiral winding coil part is
Linear parts 1A, 2A parallel to the cylinder axis Z, and arcuate parts 1B, 2B in a plane perpendicular to the cylinder axis Z.
It consists of. FIG. 5 shows a cross-sectional view of the linear portion A taken along a plane perpendicular to the cylindrical axis Z,
Linear parts 1A and 2A are arranged symmetrically on the circumference of a radius R with the Y plane in between, and by this coil
A high frequency magnetic field is generated in the direction.

[発明が解決しようとする問題点] 上述の如き従来のコイルに共通した考え方は、
等しい形状をした2つの渦巻状巻線コイル部分
1,2を円筒状領域を挟んで両側から対向配置す
るということであり、従つてコイルのターン数は
2,4,8,……と偶数ターンになる。
[Problems to be solved by the invention] The common idea of the conventional coils as described above is that
This means that two spirally wound coil parts 1 and 2 with the same shape are arranged facing each other from both sides with a cylindrical area in between, and therefore the number of turns of the coil is an even number of turns such as 2, 4, 8, etc. become.

ところで、近時超伝導磁石によつて強度の大き
な静磁場が得られるようになり、それに伴つて観
測周波数も400MHz程度から500MHz、600MHzへ
と高められようとしている。このように観測周波
数を高めるには、試料コイルとしてはインダクタ
ンスが小さくて同調周波数が高められ、しかもQ
の高いものが要求される。
By the way, in recent years it has become possible to obtain strong static magnetic fields using superconducting magnets, and along with this, the observation frequency is also being raised from about 400MHz to 500MHz or 600MHz. In order to increase the observation frequency in this way, the sample coil must have a small inductance, a high tuning frequency, and a Q
High quality is required.

そのような場合従来は、最もターン数が少なく
インダクタンスを最小にできる第5図の2ターン
のコイルが使われている。しかしながら、このよ
うなコイルを使用してもインダクタンスを十分小
さくすることはできず、従来は好ましくないこと
を承知の上でこのコイルを使用せざるを得なかつ
た。
In such cases, conventionally, a two-turn coil as shown in FIG. 5 has been used because it has the least number of turns and can minimize inductance. However, even if such a coil is used, the inductance cannot be made sufficiently small, and conventionally, this coil has been used even though it is known that it is undesirable.

本発明は、この点に鑑みてなされたものであ
り、上述した従来の考え方からは決して配置され
ることのないY平面上に巻線を配置することによ
り1ターンのコイルを提供し、インダクタンスの
小さなコイルを提供すると共に、感度的にも極め
て優秀なコイルを提供することを目的としてい
る。
The present invention has been made in view of this point, and provides a one-turn coil by arranging the winding wire on the Y plane, which would never be arranged based on the conventional concept described above, and thereby reducing the inductance. The purpose is to provide a small coil and a coil with extremely high sensitivity.

[問題点を解決するための手段] この目的を達成するため、本発明にかかる
NMRプローブ用コイルは、円筒状の試料領域の
周囲に巻回され、該円筒の軸に直交する方向の高
周波磁界を発生させるコイルであつて、上記円筒
軸に平行な方向に伸び前記円筒軸を挟んで略対称
に配置される1対の直線状の導電性部片と、該1
対の直線状導電性部片に先端同士を接続しコイル
を形成するための第1の円弧状導電性部片と、前
記試料領域の中心に関して前記第1の円弧状導電
性部片と略対称性を持つ様に配置される第2の円
弧状導電性部片であつて、複数の円弧導電性部片
からなり且つ該複数の円弧状導電性部片が前記1
対の直線状導電性部片を接続しないように前記直
線状導電性部片の他端に接続される第2の円弧状
導電性部片と、電流を一方の直線状導電性部片か
ら第1の円弧状導電性部片を介して他方の直線状
導電性部片へと流すために前記一対の直線状導電
性部片又は第2の円弧状導電性部片に接続される
一対のリードとを備えたことを特徴としている。
[Means for solving the problem] In order to achieve this objective, the present invention
The NMR probe coil is a coil that is wound around a cylindrical sample area and generates a high-frequency magnetic field in a direction perpendicular to the axis of the cylinder, and extends in a direction parallel to the cylinder axis. a pair of linear conductive pieces arranged approximately symmetrically with each other;
a first arcuate conductive piece for connecting the ends of a pair of linear conductive pieces to form a coil; and a first arcuate conductive piece that is substantially symmetrical with respect to the center of the sample area. a second arc-shaped electrically conductive piece arranged to have a conductive property, the second arc-shaped electrically conductive piece is composed of a plurality of arc-shaped electrically conductive pieces, and the plurality of arc-shaped electrically conductive pieces are
a second arc-shaped conductive piece connected to the other end of the straight conductive piece so as not to connect the pair of straight conductive pieces; a pair of leads connected to said pair of linear conductive pieces or a second arcuate conductive piece for flowing through one arcuate conductive piece to the other linear conductive piece; It is characterized by having the following.

を特徴としている。It is characterized by

[実施例] 以下、図面を用いて本発明の一実施例を詳述す
る。
[Example] Hereinafter, an example of the present invention will be described in detail using the drawings.

第1図は本発明を実施したコイルの一例を示
し、aは導体板から押し抜かれた時の形状、bは
それを円筒状に形成した時の状態を夫々示す。第
1図a,bにおいて、コイルは円筒軸Zに平行な
直線状導体L1,L2と、この直線状導体L1,
L2を直列に接続してコイルを形成するための円
弧状導体L3,L4と、補償用の第2の円弧状導
体L5〜L8と、コイルを外部の回路と接続する
ためのリードL9,L10とから構成される。
FIG. 1 shows an example of a coil embodying the present invention, in which a shows the shape when it is punched out from a conductor plate, and b shows the state when it is formed into a cylindrical shape. In FIGS. 1a and 1b, the coil consists of linear conductors L1, L2 parallel to the cylindrical axis Z, and linear conductors L1, L2 parallel to the cylindrical axis Z.
Arc-shaped conductors L3 and L4 for connecting L2 in series to form a coil, second arc-shaped conductors L5 to L8 for compensation, and leads L9 and L10 for connecting the coil to an external circuit. It consists of

上記円弧状導体L4は導体板から押し抜かれた
状態では2つに分割されており、第1図bのよう
に円筒状に成形する際に若干重なり合うように
し、その重なり部分を例えば半田付けにより接続
し一本化している。
When the arc-shaped conductor L4 is punched out from the conductor plate, it is divided into two parts, and when formed into a cylindrical shape as shown in Fig. 1b, they are slightly overlapped, and the overlapping parts are connected by, for example, soldering. It has been unified.

又、第2の円弧状導体L5〜L8は、互いに接
続されていないことから分るようにコイルとして
の役割は持つておらず、試料が配置される円筒領
域の中心原点Oを挟んで第1の円弧状導体と対称
な位置に略同一形状の導体を配置することによ
り、静磁場の均一度の乱れを補償する目的で設け
られている。従つて、その幅は第1及び第2の円
弧状導体ともWで等しくされている。
Further, the second arc-shaped conductors L5 to L8 do not have the role of a coil, as can be seen from the fact that they are not connected to each other, and the second arc-shaped conductors L5 to L8 do not have the role of a coil, and are located at the first arc-shaped conductor L5 to L8, with the center origin O of the cylindrical region where the sample is placed. This is provided for the purpose of compensating for disturbances in the uniformity of the static magnetic field by arranging a conductor of substantially the same shape at a position symmetrical to the arc-shaped conductor. Therefore, the widths of the first and second arc-shaped conductors are set to be equal to each other.

第2図は、第1図のコイルを円筒領域の中心O
において円筒軸Zに直交するXY平面で切断した
断面図を示す。この図から分るように、直線状導
体L1,L2は高周波磁界の軸(X軸)に直角な
軸(Y軸)上に配置され、1ターンのコイルが実
現されている。従つて本発明によれば、従来の2
ターンのコイルよりもインダクタンスの小さな1
ターンのコイルが実現される。
Figure 2 shows the coil in Figure 1 at the center of the cylindrical area O.
A sectional view taken along an XY plane perpendicular to the cylinder axis Z is shown in FIG. As can be seen from this figure, the linear conductors L1 and L2 are arranged on an axis (Y-axis) perpendicular to the axis of the high-frequency magnetic field (X-axis), and a one-turn coil is realized. Therefore, according to the present invention, the conventional two
1 with smaller inductance than a turn coil
A coil of turns is realized.

しかも、この位置(Y平面上)に配置される直
線状導体が、試料に配置される円筒領域の中心原
点OにおいてX軸方向に発生させる高周波磁界強
度は、直線状導体が他のどんな位置に置かれた場
合よりも強いため、コイルとしてのQが高い。従
つて本発明によれば、Qが高く効率の良いコイル
によつて試料に強い高周波磁界を照射することが
でき、しかもその強い高周波磁界照射によつて派
生した強い共鳴信号を効率良く検出することが可
能となり、その相乗効果によりNMR装置の感度
は著しく高められる。
Moreover, the high-frequency magnetic field strength that a straight conductor placed at this position (on the Y plane) generates in the X-axis direction at the center origin O of the cylindrical area placed on the sample is different from that at any other position of the straight conductor. Since it is stronger than when it is placed, it has a high Q as a coil. Therefore, according to the present invention, it is possible to irradiate a sample with a strong high-frequency magnetic field using a highly efficient coil with a high Q, and to efficiently detect a strong resonance signal derived from the strong high-frequency magnetic field irradiation. This synergistic effect significantly increases the sensitivity of the NMR device.

尚、上記実施例では直線状導体L1,L2を2
つの円弧状導体L3,L4で並列に接続したが、
接続は一方だけで良いので、2つに分割されてい
る円弧状導体L4を電気的に接続する必要は必ず
しもなく、若干の間隔をおいて離したままにして
おいても良い。ただし、円弧状導体L4を完全に
なくしてしまうことは、導体の存在が非対称にな
るために好ましくない。
In the above embodiment, the linear conductors L1 and L2 are
Connected in parallel with two arc-shaped conductors L3 and L4,
Since only one connection is required, it is not necessarily necessary to electrically connect the two halves of the arc-shaped conductor L4, and they may be left separated with a slight interval between them. However, it is not preferable to completely eliminate the arc-shaped conductor L4 because the presence of the conductor becomes asymmetrical.

第3図はこの点を考慮すると共にリードの取出
し位置を近付けた例を示す。同図aは導体板から
押し抜いた状態であり、同図bは円筒状に成形し
た状態を示す。
FIG. 3 shows an example in which this point is taken into consideration and the lead extraction position is moved closer. Figure a shows the state in which it has been punched out from the conductor plate, and figure b shows the state in which it has been formed into a cylindrical shape.

尚、本発明のコイルは、上述した導体板からの
押し抜きの他、ボビンに導体ワイヤを張付けた
り、ボビンの表面に蒸着技術で形成したり、柔軟
性を持つあるいは持たない基板上にプリント回路
として形成したりして製作することができる。導
体の強度が十分にある場合、ボビン等の他の支持
体で支持する必要はなく、導体だけで自立させる
ことが可能である。
The coil of the present invention can be formed by pasting a conductor wire onto a bobbin, by forming it by vapor deposition technology on the surface of the bobbin, in addition to being punched out from the conductor plate as described above, or by forming a printed circuit on a substrate with or without flexibility. It can be manufactured by forming it as. If the conductor has sufficient strength, it is not necessary to support it with another support such as a bobbin, and the conductor can stand alone.

尚、上記実施例では直線状導体をZ軸に対して
正確に対称に配置したが、直線状導体は略対称に
配置されれば良く、若干のずれは許容される。
In the above embodiment, the linear conductors are arranged exactly symmetrically with respect to the Z axis, but the linear conductors only need to be arranged substantially symmetrically, and a slight deviation is allowed.

[発明の効果] 以上詳述した如く、本発明によれば1ターンで
インダクタンスの小さなNMRプローブ用コイル
が実現されるため、観測周波数の高まりに十分対
応することができる。しかも、本発明のコイルは
高いQを持つため、NMR装置の感度を向上させ
ることが可能となる。
[Effects of the Invention] As described in detail above, according to the present invention, an NMR probe coil with small inductance can be realized with one turn, so that it can sufficiently cope with an increase in observation frequency. Moreover, since the coil of the present invention has a high Q, it is possible to improve the sensitivity of the NMR apparatus.

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

第1図及び第3図は夫々本発明を実施したコイ
ルの一例を示す図、第2図は第1図のコイルにつ
いてZ軸の回りの直線状導体の配置を説明するた
めの図、第4図及び第5図は従来の鞍型コイルを
説明するための図である。 L1,L2:直線状導体、L3〜L10:円弧
状導体。
1 and 3 are diagrams each showing an example of a coil embodying the present invention, FIG. 2 is a diagram for explaining the arrangement of linear conductors around the Z axis in the coil of FIG. 1, and FIG. 5 and 5 are diagrams for explaining a conventional saddle-shaped coil. L1, L2: straight conductors, L3 to L10: arc conductors.

Claims (1)

【特許請求の範囲】 1 円筒状の試料領域の周囲に巻回され、該円筒
の軸に直交する方向の高周波磁界を発生させるコ
イルであつて、上記円筒軸に平行な方向に伸び前
記円筒軸を挟んで略対称に配置される1対の直線
状の導電性部片と、該1対の直線状導電性部片の
先端同士を接続しコイルを形成するための第1の
円弧状導電性部片と、前記試料領域の中心に関し
て前記第1の円弧状導電性部片と略対称性を持つ
様に配置される第2の円弧状導電性部片であつ
て、複数の円弧状導電性部片からなり且つ該複数
の円弧状導電性部片が前記1対の直線状導電性部
片同士を接続しないように前記直線状導電性部片
の他端に接続される第2の円弧状導電性部片と、
電流を一方の直線状導電性部片から第1の円弧状
導電性部片を介して他方の直線状導電性部片へと
流すために前記一対の直線状導電性部片又は第2
の円弧状導電性部片に接続される一対のリードと
を備えたことを特徴とするNMRプローブ用コイ
ル。 2 前記導電性部片は断面が円形の導線である特
許請求の範囲第1項記載のNMRプローブ用コイ
ル。 3 前記導電性部片は板状導体で形成される特許
請求の範囲第1項記載のNMRプローブ用コイ
ル。 4 前記コイルは中空の円筒ボビンに支持される
特許請求の範囲第1項乃至第3項のいずれかに記
載のNMRプローブ用コイル。 5 前記コイルは前記ボビンに蒸着によつて形成
される特許請求の範囲第4項記載のNMRプロー
ブ用コイル。 6 前記コイルは絶縁性基板によつて支持される
プリンと回路からなる特許請求の範囲第1項記載
のNMRプローブ用コイル。 7 前記絶縁性基板は柔軟性を持ち折曲げ可能で
ある特許請求の範囲第6項記載のNMRプローブ
用コイル。 8 前記コイルは自己を保持する強度を持つ特許
請求の範囲第1項乃至第3項のいずれかに記載の
NMRプローブ用コイル。
[Scope of Claims] 1. A coil that is wound around a cylindrical sample region and that generates a high-frequency magnetic field in a direction perpendicular to the axis of the cylinder, and that extends in a direction parallel to the cylindrical axis. a pair of linear conductive pieces arranged substantially symmetrically across the pair of linear conductive pieces; and a first arc-shaped conductive piece for connecting the tips of the pair of linear conductive pieces to form a coil. a second arcuate conductive piece arranged so as to be substantially symmetrical with the first arcuate conductive piece with respect to the center of the sample region, the second arcuate conductive piece comprising a plurality of arcuate conductive pieces; a second arcuate conductive piece, the second arcuate conductive piece being connected to the other end of the linear conductive piece such that the plurality of arcuate conductive pieces do not connect the pair of linear conductive pieces; a conductive piece;
said pair of linear electrically conductive segments or a second arcuate electrically conductive segment to allow current to flow from one linear electrically conductive segment through the first arcuate electrically conductive segment to the other linear electrically conductive segment.
A coil for an NMR probe, comprising a pair of leads connected to the arc-shaped conductive piece. 2. The NMR probe coil according to claim 1, wherein the conductive piece is a conductive wire with a circular cross section. 3. The NMR probe coil according to claim 1, wherein the conductive piece is formed of a plate-shaped conductor. 4. The NMR probe coil according to any one of claims 1 to 3, wherein the coil is supported by a hollow cylindrical bobbin. 5. The NMR probe coil according to claim 4, wherein the coil is formed on the bobbin by vapor deposition. 6. The coil for an NMR probe according to claim 1, wherein the coil comprises a circuit and a circuit supported by an insulating substrate. 7. The NMR probe coil according to claim 6, wherein the insulating substrate has flexibility and is bendable. 8. The coil according to any one of claims 1 to 3, wherein the coil has strength to maintain itself.
Coil for NMR probe.
JP60018444A 1985-02-01 1985-02-01 Coil for nmr probe Granted JPS61176841A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60018444A JPS61176841A (en) 1985-02-01 1985-02-01 Coil for nmr probe

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60018444A JPS61176841A (en) 1985-02-01 1985-02-01 Coil for nmr probe

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JPS61176841A JPS61176841A (en) 1986-08-08
JPH0318450B2 true JPH0318450B2 (en) 1991-03-12

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JP60018444A Granted JPS61176841A (en) 1985-02-01 1985-02-01 Coil for nmr probe

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Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03283604A (en) * 1990-03-30 1991-12-13 Shimadzu Corp Differentiation type coil
JP5156190B2 (en) * 2005-12-21 2013-03-06 株式会社 Jeol Resonance Combined cylindrical coil for NMR

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4694255A (en) * 1983-11-04 1987-09-15 General Electric Company Radio frequency field coil for NMR
US5274332A (en) * 1983-11-14 1993-12-28 General Electric Company Inductively coupled multi-section radio frequency field coil for NMR
US4692705A (en) * 1983-12-23 1987-09-08 General Electric Company Radio frequency field coil for NMR
US4641097A (en) * 1984-05-10 1987-02-03 General Electrtic Company Elliptical cross-section slotted-tube radio-frequency resonator for nuclear magnetic resonance imaging

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JPS61176841A (en) 1986-08-08

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