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JPH0431069B2 - - Google Patents
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JPH0431069B2 - - Google Patents

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Publication number
JPH0431069B2
JPH0431069B2 JP60026719A JP2671985A JPH0431069B2 JP H0431069 B2 JPH0431069 B2 JP H0431069B2 JP 60026719 A JP60026719 A JP 60026719A JP 2671985 A JP2671985 A JP 2671985A JP H0431069 B2 JPH0431069 B2 JP H0431069B2
Authority
JP
Japan
Prior art keywords
coil
pair
arcuate
linear
conductive pieces
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
JP60026719A
Other languages
Japanese (ja)
Other versions
JPS61186841A (en
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 filed Critical
Priority to JP60026719A priority Critical patent/JPS61186841A/en
Priority to US06/828,196 priority patent/US4737715A/en
Publication of JPS61186841A publication Critical patent/JPS61186841A/en
Publication of JPH0431069B2 publication Critical patent/JPH0431069B2/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
    • G01R33/34007Manufacture of RF coils, e.g. using printed circuit board technology; additional hardware for providing mechanical support to the RF coil assembly or to part thereof, e.g. a support for moving the coil assembly relative to the remainder of the MR system
    • 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
    • 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
    • G01R33/34092RF coils specially adapted for NMR spectrometers

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装置(NMR装置)のプロ
ーブに用いられるコイル装置に関し、特に感度を
高めることのできるコイルの構造に関するもので
ある。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a coil device used in a probe of a nuclear magnetic resonance apparatus (NMR apparatus), and particularly to a coil structure that can increase sensitivity.

〔従来技術〕[Prior art]

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、プローブ内の試料に近接
して配置されたコイルから励起用高周波磁界を照
射すると共に、試料からの共鳴信号をこのコイル
によつて受信し、受信回路を介してコンピユータ
へ送り、フーリエ変換処理により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や払
われている。超伝導磁石を用いるNMR装置の場
合、例えば第6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6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7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。
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 coil placed close to the sample within the probe. The NMR spectrum is received by a receiver, sent to a computer via a receiving circuit, and subjected to Fourier transform processing to obtain an NMR spectrum. At this time, the sensitivity of the NMR device is greatly influenced by the quality of the coupling between the coil and the resonator of the sample, so great attention is paid to the shape and structure of the coil. In the case of NMR devices using superconducting magnets, for example, a cylindrical saddle-shaped coil as shown in FIG. 6 has been commonly used. In the saddle-shaped coil shown in Fig. 6, 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 spirally wound coil portion consists of straight portions 1A, 2A parallel to the cylindrical axis Z, and arcuate portions 1B, 2B lying in a plane perpendicular to the cylindrical axis Z. FIG. 7 shows a cross-sectional view of the linear portion A taken along a plane perpendicular to the cylindrical axis Z. The linear portions 1A and 2A are arranged symmetrically on the circumference of the radius R with the Y plane in between. A high frequency magnetic field is generated in the X direction by the coil.

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
2,4,6,8,…と偶数ターンになる。
The idea common to conventional coils as mentioned above is
Two spiral-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 such as 2, 4, 6, 8, etc. It will be a turn.

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500MHz600MHzへと
高められて来ている。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
小さく同調周波数を高められ、しかもQが高く
SN比及び感度を高められるものが要求される。
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 has also been increased from about 400 MHz to 500 MHz and 600 MHz. In order to increase the observation frequency in this way, the sample coil should have a small inductance that can increase the tuning frequency, and a high Q.
A device that can increase the signal-to-noise ratio and sensitivity is required.

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6図の2ターンのコイルがその
ような場合に使われている。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
に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。
Conventionally, the two-turn coil shown in FIG. 6, which has the smallest number of turns and can minimize inductance, has been used in such cases. However, even if such a coil is used, the inductance cannot be made sufficiently small, and in the past, this coil has had to be used even though it is undesirable.

そこで本発明者は、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第7図のY軸上に
巻線を配置する第8図に示すような1ターンの新
規なコイルを提案した。第8図aは導体板から押
し抜かれた時の形状を示し、第8図bはそれを円
筒状に形成した時の状態を示す。第8図a,bに
おいて、コイルは円筒軸Zに平行な直線状導体L
1,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L
3,L4と、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。上記第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
も分るように、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、静磁場の同一度の
乱れを補償する目的で設けられている。
Therefore, the present inventor proposed a novel one-turn coil as shown in FIG. 8, in which the winding is arranged on the Y axis in FIG. 7, which would never be arranged based on the conventional concept described above. FIG. 8a shows the shape when punched out from the conductor plate, and FIG. 8b shows the state when it is formed into a cylindrical shape. In Figures 8a and 8b, the coil is a straight conductor L parallel to the cylindrical axis Z.
1, L2, and an arc-shaped conductor L for forming a coil by connecting the linear conductors L1, L2 in series.
3. L4, second arc-shaped conductors L5 to L8, and lead L9 for connecting the coil to an external circuit.
It consists of L10. As can be seen from the fact that they are not connected to each other, the second arc-shaped conductors L5 to L8 do not have a role as a coil, and are located at the center point O of the cylindrical area where the sample is placed. By arranging a conductor having substantially the same shape at a position symmetrical to the first arc-shaped conductor, it is provided for the purpose of compensating for disturbances of the same degree in the static magnetic field.

このような提案コイルによれば、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。しかもこの提案コイル
では、コイルとしての役割を果す直線状導体L
1,L2が高周波磁界の軸(X軸)に直角なYZ
平面に配置されるが、この位置に配置される直線
状導体が、試料の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。
According to such a proposed coil, a one-turn coil having a smaller inductance than a conventional two-turn coil can be realized. Moreover, in this proposed coil, the linear conductor L that plays the role of the coil
1. YZ where L2 is perpendicular to the axis of the high frequency magnetic field (X axis)
Although the straight conductor is placed on a plane, the high-frequency magnetic field strength generated in the X-axis direction at the center origin O of the cylindrical area where the sample is placed by the straight conductor placed at this position is different from that of the straight conductor at any other position. Since it is stronger than when it is placed, it has a high Q as a coil.

従つて、この提案コイルによりインダクタンス
が小さくQの高いコイルが実現されるが、この提
案コイルを実際の装置に使用しても同調回路のQ
は期待されたほど高くならなかつた。その理由
は、実際のNMRプローブでは、提案コイルを静
磁場の中心に配置すると共に、このコイルからリ
ード線を伸ばし、コイルから離れた位置において
同調用コンデンサを接続して共振回路を形成して
いるからであり、このリード線のインダクタンス
や浮遊容量によつて同調回路(共振回路)のQが
期待されたほど良くならなかつたのである。
Therefore, this proposed coil realizes a coil with low inductance and high Q, but even if this proposed coil is used in an actual device, the Q of the tuned circuit will be low.
was not as high as expected. The reason for this is that in an actual NMR probe, the proposed coil is placed at the center of the static magnetic field, a lead wire is extended from this coil, and a tuning capacitor is connected at a position away from the coil to form a resonant circuit. This is because the inductance and stray capacitance of the lead wires prevented the Q of the tuned circuit (resonant circuit) from becoming as good as expected.

そこで本発明の目的は、上記提案コイルの中に
同調用コンデンサを組込むことにより、同調回路
のQを高めることのできるコイル装置を実現する
ことを目的としている。
Therefore, an object of the present invention is to realize a coil device that can increase the Q of a tuning circuit by incorporating a tuning capacitor into the proposed coil.

〔問題点を解決するための手段〕[Means for solving problems]

この目的を達成するため、本発明にかかる
NMRプローブ用コイル装置は、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装置であつて、
上記円筒軸に平行な方向に伸び該円筒軸を挟んで
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部同士を接
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、該1対の直線状導電性部片の他端部同士
を接続するための第2の円弧状導電性部片とを備
え、該第1の円弧状導電性部片は前記円筒状領域
の外周に沿つて連続的にのびて前記1対の直線状
導電性部片同士を接続し、該第2の円弧状導電性
部片の途中にコンデンサを介挿すると共に、前記
第2の円弧状導電性部片と前記1対の直線状導電
性部片との接続部を介して外部回路と接続するよ
うにしたことを特徴としている。
To achieve this objective, the present invention
A coil device for an NMR probe is a coil device that is wound around a cylindrical sample region and generates a high-frequency magnetic field in a direction perpendicular to the axis of the cylinder, and includes:
A pair of straight conductive pieces extending in a direction parallel to the cylindrical axis and arranged approximately symmetrically across the cylindrical axis, and connecting the tips of the pair of straight conductive pieces to each other. comprising a first arcuate conductive piece for forming a coil, and a second arcuate conductive piece for connecting the other ends of the pair of linear conductive pieces, The first arc-shaped conductive piece extends continuously along the outer periphery of the cylindrical region to connect the pair of linear conductive pieces, and the second arc-shaped conductive piece A capacitor is inserted in the middle of the conductive piece, and the second arc-shaped conductive piece is connected to an external circuit through a connecting part between the pair of linear conductive pieces. There is.

〔作用〕[Effect]

本発明は、上記提案コイルにおいて、第1の円
弧状導体L3,L4の存在を補償するために第2
の円弧状導体L5〜L8が設けられていることに
着目し、この第2の円弧状導体に同調用コンデン
サを介挿したことを特徴としている。このように
すれば、コイル構造体単独で同調回路(共振回
路)が形成されるため、リード像を伸ばして同調
用コンデンサを接続していた従来に比べ同調回路
のQは飛躍的に高められることになる。
In the proposed coil, the present invention provides a second conductor to compensate for the presence of the first arc-shaped conductors L3 and L4.
The second arc-shaped conductor L5 to L8 are provided, and a tuning capacitor is inserted into the second arc-shaped conductor. In this way, since a tuned circuit (resonant circuit) is formed by the coil structure alone, the Q of the tuned circuit can be dramatically increased compared to the conventional method in which the lead image is extended and a tuning capacitor is connected. become.

〔実施例〕〔Example〕

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

第1図は本発明を実施したNMRプローブ用コ
イル装置の一例を示す斜視図である。このコイル
装置が第8図bの提案コイルと異なるのは、円弧
状導体L5とL6の間及びL7とL8との間に
夫々コンデンサが介挿されている点である。本実
施例では、コイルを第2の円弧状導体の位置で円
筒軸Zに直交する面で切断した断面図を示す第2
図から分るように、円弧状導体L5とL6及びL
7とL8の間に重なり合う部分を設け、その重な
り部分に誘電体フイルムFを挟み込んで絶縁する
ことにより、その重なり部分に容量を持たせコン
デンサとしている。
FIG. 1 is a perspective view showing an example of a coil device for an NMR probe embodying the present invention. This coil device differs from the proposed coil shown in FIG. 8b in that capacitors are inserted between the arcuate conductors L5 and L6 and between L7 and L8. In this example, a second cross-sectional view showing a cross-sectional view of the coil cut along a plane perpendicular to the cylindrical axis Z at the position of the second arc-shaped conductor is used.
As can be seen from the figure, arc-shaped conductors L5, L6 and L
By providing an overlapping portion between 7 and L8 and insulating the overlapping portion by sandwiching a dielectric film F, the overlapping portion has a capacitance, thereby forming a capacitor.

従つて、第1図のコイルを等価回路で表わすと
第3図の如くなり、直線状導体L1,L2が主に
寄与するインダクタンスとコンデンサC1,C2
の合成容量とで並列共振回路が構成される。この
共振回路は従来のようにコイルとコンデンサとの
間にリード線等が存在せず、言わばコイルの中に
同調用コンデンサが組込まれていることになるた
め、共振回路のQは極めて高い。
Therefore, if the coil in Figure 1 is represented as an equivalent circuit, it will be as shown in Figure 3, where the inductance and capacitors C1 and C2 are mainly contributed by the linear conductors L1 and L2.
A parallel resonant circuit is constructed with the combined capacitance of . In this resonant circuit, there is no lead wire or the like between the coil and the capacitor as in the conventional case, and the tuning capacitor is built into the coil, so the Q of the resonant circuit is extremely high.

第4図は本発明の他の実施例を示し、本実施例
では第1図の構成に加えて市販の小型チツプコン
デンサC5,C6を円弧状導体L5,L6に夫々
取付け、このコンデンサC5,C6同士を第3の
円弧状導体L11で接続し、この円弧状導体L1
1からリードL12を引出している。それに伴
い、第1図のコイルにおけるリードL10は除か
れている。
FIG. 4 shows another embodiment of the present invention. In this embodiment, in addition to the configuration shown in FIG. 1, commercially available small chip capacitors C5 and C6 are attached to the arc-shaped conductors L5 and L6, are connected to each other by a third arc-shaped conductor L11, and this arc-shaped conductor L1
Lead L12 is pulled out from 1. Accordingly, the lead L10 in the coil of FIG. 1 is removed.

本実施例のコイルを等価回路で表わすと第5図
の如くなり、コイルのインダクタンスがコンデン
サC5によつてキヤンセルされるかたちとなつて
実質的に減少するので、第1図のコイルよりも共
振周波数(同調周波数)を上昇させることが可能
である。
If the coil of this embodiment is represented as an equivalent circuit, it will be as shown in Fig. 5. Since the inductance of the coil is canceled by the capacitor C5 and is substantially reduced, the resonance frequency will be higher than that of the coil of Fig. 1. (tuned frequency) can be increased.

尚、上記各実施例において誘電体フイルムFを
円弧状導体で挟んで構成したコンデンサを、第4
図の実施例で一部使用した小型チツプコンデンサ
で置換するようにしても良いことは言うまでもな
い。
In addition, in each of the above embodiments, the capacitor constructed by sandwiching the dielectric film F between arc-shaped conductors is
It goes without saying that the small chip capacitors partially used in the illustrated embodiment may be substituted.

又、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。
In addition to being punched out from a conductor plate as described above, the coil of the present invention can also be formed by attaching a conductor wire to a bobbin, by vapor deposition technology on the surface of a bobbin, or by forming a printed circuit on a substrate with or without flexibility. It can be manufactured by forming it as.

又、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。
Further, 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〕〔Effect of the invention〕

以上詳述した如く、本発明によればインダクタ
ンスが小さくて高い周波数まで使用できると共
に、高い共振回路のQを持つたNMRプローブ用
コイル装置が実現されるため、NMR装置の観測
周波数が更に高められると共に感度を飛躍的に向
上させることが可能となる。
As detailed above, according to the present invention, a coil device for an NMR probe is realized which has small inductance, can be used up to high frequencies, and has a high resonant circuit Q, so that the observation frequency of the NMR device can be further increased. At the same time, it becomes possible to dramatically improve sensitivity.

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

第1図は本発明を実施したNMRプローブ用コ
イル装置の一例を示す斜視図、第2図はコイルを
第2の円弧状導体L5〜L8の位置で円筒軸Zに
直交する面で切断した断面図、第3図は第1図の
コイルの等価回路を示す図、第4図は本発明の他
の実施例を示す斜視図、第5図は第4図のコイル
の等価回路を示す図、第6図及び第7図は従来の
鞍型コイルを説明するための図、第8図は本発明
者が提案した新規なコイルを説明するための図で
ある。 L1,L2…直線状導体、L3〜L8…円弧状
導体、F…誘電体フイルム、C1〜C6…コンデ
ンサ。
FIG. 1 is a perspective view showing an example of a coil device for an NMR probe embodying the present invention, and FIG. 2 is a cross section of the coil taken along a plane perpendicular to the cylindrical axis Z at the positions of the second arc-shaped conductors L5 to L8. 3 is a diagram showing an equivalent circuit of the coil in FIG. 1, FIG. 4 is a perspective view showing another embodiment of the present invention, and FIG. 5 is a diagram showing an equivalent circuit of the coil in FIG. 4. 6 and 7 are diagrams for explaining a conventional saddle-shaped coil, and FIG. 8 is a diagram for explaining a novel coil proposed by the present inventor. L1, L2...Straight conductor, L3-L8...Circular conductor, F...Dielectric film, C1-C6...Capacitor.

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
イル装置であつて、上記円筒軸に平行な方向に伸
び該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
の先端部同士を接続するための第1の円弧状導電
性部片と、該1対の直線状導電性部片の他端部同
士を接続しコイルを形成するための第2の円弧状
導電性部片とを備え、該第1の円弧状導電性部片
は前記円筒状領域の外周に沿つて連続的にのびて
前記1対の直線状導電性部片同士を接続し、該第
2の円弧状導電性部片の途中にコンデンサを介挿
すると共に、前記第2の円弧状導電性部片と前記
1対の直線状導電性部片との接続部を介して外部
回路と接続するようにしたことを特徴とする
NMRプローブ用コイル装置。 2 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項記載のコイル。 3 前記第1及び第2の円弧状導電性部片は試料
領域を挾んで対称に夫々1対設けられ、該1対の
第2の円弧状導電性部片の夫々にコンデンサが介
挿される特許請求の範囲第1項乃至第2項のいず
れかに記載のNMRプローブ用コイル装置。
[Scope of Claims] 1. A coil device that is wound around a cylindrical sample region and generates a high-frequency magnetic field in a direction perpendicular to the axis of the cylinder, which extends in a direction parallel to the axis of the cylinder. A pair of linear conductive pieces arranged substantially symmetrically across an axis, and a first arcuate conductive piece for connecting the tips of the pair of linear conductive pieces. and a second arcuate conductive piece for connecting the other ends of the pair of linear conductive pieces to form a coil, the first arcuate conductive piece being The linear conductive pieces extend continuously along the outer periphery of the cylindrical region to connect the pair of linear conductive pieces, and a capacitor is inserted in the middle of the second arcuate conductive piece, and the The second arcuate conductive piece is connected to an external circuit through a connecting portion between the pair of linear conductive pieces.
Coil device for NMR probe. 2. The coil according to claim 1, wherein the conductive piece is formed of a plate-shaped conductor. 3. A patent in which the first and second arcuate conductive pieces are provided in pairs symmetrically across the sample area, and a capacitor is inserted into each of the pair of second arcuate conductive pieces. An NMR probe coil device according to any one of claims 1 to 2.
JP60026719A 1985-02-14 1985-02-14 Coil device for nmr Granted JPS61186841A (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP60026719A JPS61186841A (en) 1985-02-14 1985-02-14 Coil device for nmr
US06/828,196 US4737715A (en) 1985-02-14 1986-02-10 Coil system for nuclear magnetic resonance spectrometer probe

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60026719A JPS61186841A (en) 1985-02-14 1985-02-14 Coil device for nmr

Publications (2)

Publication Number Publication Date
JPS61186841A JPS61186841A (en) 1986-08-20
JPH0431069B2 true JPH0431069B2 (en) 1992-05-25

Family

ID=12201148

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60026719A Granted JPS61186841A (en) 1985-02-14 1985-02-14 Coil device for nmr

Country Status (1)

Country Link
JP (1) JPS61186841A (en)

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60224076A (en) * 1984-04-23 1985-11-08 Mitsubishi Electric Corp Device for generating and detecting high-frequency magnetic field
FI853150L (en) * 1984-10-09 1986-04-10 Gen Electric RADIO FREQUENCY FOER NMR.

Also Published As

Publication number Publication date
JPS61186841A (en) 1986-08-20

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