JPS6334906A - Device for generating and detecting high frequency magnetic field - Google Patents

Device for generating and detecting high frequency magnetic field

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Publication number
JPS6334906A
JPS6334906A JP61179527A JP17952786A JPS6334906A JP S6334906 A JPS6334906 A JP S6334906A JP 61179527 A JP61179527 A JP 61179527A JP 17952786 A JP17952786 A JP 17952786A JP S6334906 A JPS6334906 A JP S6334906A
Authority
JP
Japan
Prior art keywords
conductor
magnetic field
ring
frequency magnetic
vertical
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
JP61179527A
Other languages
Japanese (ja)
Inventor
Susumu Nishihara
西原 進
Kiyoshi Yoda
潔 依田
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP61179527A priority Critical patent/JPS6334906A/en
Priority to US07/013,901 priority patent/US4755756A/en
Publication of JPS6334906A publication Critical patent/JPS6334906A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To improve the power supplying efficiency of a high frequency magnetic field generation detector by opposing the ends of split vertical conductors at a predetermined gap, using the ends as power supplying points, and supplying power in balance to the points through an unbalance/balance converter provided separately. CONSTITUTION:Balanced powers are supplied from power supplying points 7a, 7b through a matching circuit 8 to an equivalent resonator which is composed of a coil 1 made of vertical and lateral conductors 1a, 1b, a capacitor 2, and a guard ring 3 disposed through a dielectric element inside the conductor 1b. The resonance frequency can be mainly regulated by moving upward or downward the ring to vary an electrostatic capacity between the lateral conductors disposed adjacently, and the matching state can be regulated by altering the variable capacitors 8a-8c of the matching circuit 8. Loads are balanced with respect to an earth, the supplying current is completely converted to balanced currents necessary for intrinsic loads which contain coils to be supplied, and resonated and matched regularly. Thus, the power supplying efficiency can be extremely improved.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は高周波磁場発生・検出装置、特に核磁気共鳴
装置に用いる高周波磁場発生・検出装置に関するもので
ある。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a high frequency magnetic field generation/detection device, particularly to a high frequency magnetic field generation/detection device used in a nuclear magnetic resonance apparatus.

〔従来の技術〕 第4図は例えば、ジャーナル オプ マグネティック 
レゾナンス( Journal of Magneti
cResonance ) 3 6巻.447頁〜45
〕頁(ユ979)に示されている従来の高周波磁場発生
・検出装置を示す図であり、図において(1)は銅板で
構成されるコイル部でバーチカルバンド(vertic
al band) (la)、ウィング(wing) 
(lb)窓部(1c)より構成される。(2)は隣接す
るウィング間に挿入されたコンデンサ、(3)はウィン
グの内側に絶縁層を介して設置された電界シールド用の
保護環でガードリング( Guard Ring )と
呼ばれ、トップガードリング(Top Guard R
ing )−(3a)、ボトム ガードリンク(Bot
tom Guard Ring) (3b)、より構成
される。(4)は給電点、(5)はインピーダンス整合
用コンデンサ、(6)は送受信器と接続される端子であ
る。
[Prior art] Figure 4 shows, for example, a journal op magnetic
Resonance ( Journal of Magneti
cResonance) 3 6th volume. pages 447-45
This is a diagram showing a conventional high-frequency magnetic field generation/detection device shown on page (Yu 979).
al band) (la), wing (wing)
(lb) Consists of a window portion (1c). (2) is a capacitor inserted between adjacent wings, and (3) is a protective ring for electric field shield installed inside the wing via an insulating layer, called a guard ring, and the top guard ring. (Top Guard R
ing )-(3a), Bottom Guard Link (Bot
tom Guard Ring) (3b). (4) is a feeding point, (5) is an impedance matching capacitor, and (6) is a terminal connected to a transmitter/receiver.

次に動作について説明する。Next, the operation will be explained.

コイル部(1) 、コンデンサ(2)、ガードリング(
3)は等制約KLO直列共振回路を構成する。インピー
ダンス整合用コンデンサ(5)、端子(6)を経て所定
のインピーダンスを有する送信器及び受信器(図示せず
)と接続され送信器から電流がコイル部(1)に供給さ
れ所定の高周波磁場を作る一方、コイル部(1)内に設
けられた測定対象からの信号を受信器に導くように働ら
く。
Coil part (1), capacitor (2), guard ring (
3) constitutes an equi-constrained KLO series resonant circuit. It is connected to a transmitter and receiver (not shown) having a predetermined impedance via an impedance matching capacitor (5) and a terminal (6), and current is supplied from the transmitter to the coil section (1) to generate a predetermined high-frequency magnetic field. The coil part (1) serves to guide the signal from the object to be measured provided in the coil part (1) to the receiver.

ガードリング(3)は、電界シールドの働きをしこの高
周波磁場発生拳検出装置内に測定対象を設置した場合に
、発生電界による測定対象内の誘電損失を低減する。
The guard ring (3) functions as an electric field shield and reduces dielectric loss within the measurement object due to the generated electric field when the measurement object is installed in this high frequency magnetic field generating fist detection device.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

従来の高周波磁場発生●検出装置は以上のように構成さ
れているので、回路インピーダンスの平衡不平衡変換が
考慮されておらず、端子(6)に接続する同軸ケーブル
に同相電流が流れて、不安定、低効率になるなどの欠点
があった。
Conventional high-frequency magnetic field generation/detection devices are configured as described above, so balance-unbalance conversion of circuit impedance is not taken into account, and a common-mode current flows through the coaxial cable connected to terminal (6), causing unbalance. There were drawbacks such as stability and low efficiency.

この発明は上記のような問題点を解消するためになされ
たもので、回路インピーダンスの平衡不平衡性を考慮し
、安定で効率の良い、高周波磁場発生・検出装置を得る
ことを目的とする。
The present invention has been made to solve the above-mentioned problems, and aims to provide a stable and efficient high-frequency magnetic field generation/detection device by taking into consideration the unbalanced circuit impedance.

また、全身用の高周波コイルが円筒型の場合、送信磁場
発生の効率が低く、また受信信号のS/IJ(Sig.
nal to Noise Ratio )か比較的小
さいなどの問題があった。
Furthermore, when the whole-body high-frequency coil is cylindrical, the efficiency of generating the transmitting magnetic field is low, and the S/IJ (Sig.
There were problems such as a relatively small noise ratio (nal to noise ratio).

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

この発明に係る高周波磁場発生・検出装置はコイル部の
バーチカルバンド(タテ導体部)の中央部で部分し、部
分されたタテ導体部の端部を所定のギャップをもって対
向させた構成とすると共に、この部分されたタテ導体部
の各端部部分を給電点とし、別に設けられた不平衡・平
衡変換回路を経てこの給電点に平衡給電するようにした
ものである。また、全身用の高周波コイルの形を楕円型
にする。
The high frequency magnetic field generation/detection device according to the present invention has a structure in which a vertical band (vertical conductor part) of a coil part is divided at the center, and the ends of the vertical conductor part are opposed with a predetermined gap, Each end portion of the divided vertical conductor portion is used as a power feeding point, and balanced power is fed to this feeding point via a separately provided unbalanced/balanced conversion circuit. In addition, the shape of the high-frequency coil for the whole body is made into an oval shape.

〔作用〕[Effect]

この発明における高周波磁場発生●検出装置は、上記の
構成にすることによりコイル部(1)にコイル部を含む
真の負荷にのみ有効に働らく平衡電流(アースに対し、
逆相になっている電流)のみが流れ、アースに対し同相
の同相電流は抑制されるので、給電効率が著しく向上す
る。
The high frequency magnetic field generation/detection device according to the present invention has the above configuration, so that the coil part (1) has a balanced current (relative to ground) that effectively acts only on the true load including the coil part.
Only currents that are in the opposite phase flow, and common-mode currents that are in the same phase as the ground are suppressed, significantly improving power supply efficiency.

また、全身用の高周波コイルを楕円型にすることにより
、送信磁場発生の効率や受信信号のS/Nが向上する。
Further, by making the whole body high-frequency coil elliptical, the efficiency of generating the transmitting magnetic field and the S/N of the received signal are improved.

〔実施例〕〔Example〕

以下この発明の実施例を図について説明する。 Embodiments of the present invention will be described below with reference to the drawings.

第1図はこの発明の実施例の斜視図、第2図はその説明
のための一部断面構成図である。
FIG. 1 is a perspective view of an embodiment of the present invention, and FIG. 2 is a partially sectional configuration diagram for explaining the same.

第1図及び第2図において同一符号のものは同−又は相
当部分を示す。(1)はコイル部であってタテ導体部(
la) (従来例のバーチカルパントに相当)、と、ヨ
コ導体部(従来例のウィングに相当)より構成される。
In FIG. 1 and FIG. 2, the same reference numerals indicate the same or corresponding parts. (1) is the coil part and the vertical conductor part (
la) (corresponding to the vertical pant of the conventional example), and a horizontal conductor part (corresponding to the wing of the conventional example).

(2)はコンデンサであって隣接するヨコ導体部の端部
を容量結合するものである。(3)はガードリングでト
ップガードリング(3a)と、ボトムガードリング(3
b)とよシ構成される、(6)は端子で給電電流の供給
と検出電流の取出を行う。(7a)。
(2) is a capacitor that capacitively couples the ends of adjacent horizontal conductor portions. (3) are guard rings; top guard ring (3a) and bottom guard ring (3a).
(6) is a terminal that supplies the power supply current and takes out the detection current. (7a).

(7b)は給電点、(8)は整合回路で3ケの可変コン
デンサ(8a) 、 (8b) 、 (8c )で構成
される。(9)は1/2波長ケーブルで、端子(6)か
ら供給される不平衡電流を1800遅相して逆相変換し
整合回路(8)を経て2つの給電点(7a)、(7b)
に同振幅逆相の電流を給電できるようにする不平衡・平
衡変換の働らきをするものである。QOは相対向するタ
テ導体部のギャップである0 なお、タテ導体部(1a)のなす角度θの一例は、80
〈θ〈900である。
(7b) is a feeding point, and (8) is a matching circuit consisting of three variable capacitors (8a), (8b), and (8c). (9) is a 1/2 wavelength cable, which delays the unbalanced current supplied from the terminal (6) by 1800 degrees, converts it into a negative phase, passes through the matching circuit (8), and connects it to the two feeding points (7a) and (7b).
It functions as an unbalanced/balanced converter that allows currents of the same amplitude and opposite phase to be supplied to the QO is the gap between the vertical conductor parts facing each other 0. An example of the angle θ formed by the vertical conductor part (1a) is 80
〈θ〈900.

また、(]C)はタテ導体部(1a)とヨコ導体部(1
b)で包まれる空間部分であってコイル部の窓部という
(]C) is the vertical conductor part (1a) and the horizontal conductor part (1a).
b) This is the space surrounded by the coil part and is called the window part of the coil part.

またaυはリングで、トップガードリング(3a)とボ
トムガードリンク(3b)を絶縁した状態でつなぎ、上
下にうごかすことによりガードリングと対面するヨコ導
体部との間の静電容量を調整できるようにし、隣接配置
されているヨコ導体部との間の結合容量を変化させ得る
ようにしている。
In addition, aυ is a ring that connects the top guard ring (3a) and the bottom guard link (3b) in an insulated state, and by moving it up and down, the capacitance between the guard ring and the horizontal conductor facing the guard ring can be adjusted. This makes it possible to change the coupling capacitance between adjacent horizontal conductor parts.

高周波コイルは楕円の筒型であり、第1図においてはバ
ーチカル着バンドは楕円の短径方向に配置されている例
であり、第3図は長径方向に配置されている例である。
The high frequency coil has an elliptical cylindrical shape, and FIG. 1 shows an example in which the vertical attachment band is arranged in the short axis direction of the ellipse, and FIG. 3 shows an example in which it is arranged in the long axis direction.

次に動作の説明を行う。Next, the operation will be explained.

タテ導体部(1a)とヨコ導体部(1b)よりなる、コ
イル部(1)、コンデンサ(2)及びヨコ導体部(1b
)の内側に誘電体を通して配置されるガードリンク(3
)で構成される等価共振回路に対し、給電点(7a)。
The coil part (1), the capacitor (2), and the horizontal conductor part (1b) consist of a vertical conductor part (1a) and a horizontal conductor part (1b).
) is placed inside the guard link (3) through the dielectric material.
), the feed point (7a).

(7b)から整合回路(8)を経て平衡給電が行える。Balanced power feeding can be performed from (7b) through a matching circuit (8).

共振周波数は主としてリングを上下にうごかし隣接配置
されているヨコ導体部間の静電容量を変化させることに
より調整できる。
The resonance frequency can be adjusted mainly by moving the ring up and down to change the capacitance between adjacent horizontal conductor parts.

また整合状態は整合回路(8)の可変コンデンサ(8a
)、(8b)、(8c)を変化させることにより調整で
きる。
Also, the matching state is determined by the variable capacitor (8a) of the matching circuit (8).
), (8b), and (8c).

この構成では負荷はアースに対しバランスしており、か
つ給電電流はコイル部を含む真の負荷が必要とする平衡
電流(アースに対し逆相の電流)に完全に変換されて供
給される。また、共振と共に整合もきちんととれるよう
になっているので給電効率は極めてよいものとなる。
In this configuration, the load is balanced with respect to the ground, and the feed current is completely converted into a balanced current (a current in reverse phase with respect to the ground) required by the true load including the coil section and supplied. In addition, since resonance and matching are properly achieved, power feeding efficiency is extremely high.

また、かかる構成になっているので、コイル部(1)中
に置かれた測定対象からの信号も効率よく抽出すること
ができる。
Furthermore, with this configuration, signals from the measurement target placed in the coil section (1) can also be efficiently extracted.

また、前記実施例では不平衡・平衡変換を172波長ケ
ーブルを用いて構成する場合について述べたが、バラン
スのよい2次捲線をもつトランスであってもよい。また
、タテ導体部の1方に給電をして、対向部のタテ導体部
の中間にコンデンサを接続して、高い周波数に対応させ
ることもできる。
Further, in the above embodiment, a case has been described in which the unbalanced/balanced conversion is configured using a 172 wavelength cable, but a transformer having a well-balanced secondary winding may also be used. Further, it is also possible to supply power to one of the vertical conductor parts and connect a capacitor between the opposite vertical conductor parts to correspond to a high frequency.

また、全身用の円筒型の高周波磁場発生・検品tgは大
型になり、送信磁場発生の効率または受信信号のS/N
が小さくなる。人間の体の断面はほぼ楕円形であるので
、高周波磁場発生・検出器を円筒の直径が長径となるよ
うな楕円筒にすることができる。これにより、円筒の場
合に比べて高い磁場発生の効率となり受信信号のS/N
も向上する。
In addition, the cylindrical high-frequency magnetic field generation/inspection TG for the whole body has become larger, and the efficiency of transmitting magnetic field generation or the S/N of the received signal has increased.
becomes smaller. Since the cross section of the human body is approximately elliptical, the high-frequency magnetic field generator/detector can be made into an elliptical cylinder whose diameter is the major axis. As a result, the efficiency of magnetic field generation is higher than in the case of a cylinder, and the S/N of the received signal is
It also improves.

例えば64MH2に対しては、円筒の場合に比較してだ
円形では同一の送信電力の場合60〜70%送信磁場が
増加することが実験により判明した。
For example, for 64MH2, it has been found through experiments that the transmitted magnetic field increases by 60 to 70% for the same transmission power in the case of an oval shape compared to the case of a cylinder.

また、楕円の長径方向が水平になるようにRFヨコルを
設置した時に高周波磁場を水平又は鉛直方向に発生させ
るかにより、それぞれバーチカルパントを短径方向、長
径方向に配置する。
Further, when the RF horizontal is installed so that the major axis direction of the ellipse is horizontal, the vertical punts are arranged in the minor axis direction and the major axis direction depending on whether the high frequency magnetic field is generated horizontally or vertically.

〔発明の効果〕〔Effect of the invention〕

以上のようにこの発明に係る高周波磁場発生・検出装置
は、全身用の高周波磁場発生・検a[の形を楕円にする
ことKより高い磁場発生の効率とし、受信信号のS/N
も向上させた。又コイル部のタテ導体部の中央部で二つ
に分け、この部分されたタテ導体部の端部部分を給電点
として、別に不平衡・平衡変換回路を設けてこの給電点
に平衡給電するようにしたので、コイル部にはコイル部
を含む真の負荷にのみ有効に働らく平衡電流のみが給電
され、不平衡電流が流れないので給電効率及び信号検出
効率が著しく向上する効果を有する。
As described above, the high-frequency magnetic field generation/detection device according to the present invention has a high-frequency magnetic field generation/detection device for the whole body.
has also been improved. In addition, the vertical conductor part of the coil part is divided into two at the center, and the end part of the vertical conductor part is used as a feeding point, and a separate unbalanced/balanced conversion circuit is installed to supply balanced power to this feeding point. Therefore, only the balanced current that effectively acts only on the true load including the coil portion is fed to the coil portion, and no unbalanced current flows, resulting in the effect of significantly improving power feeding efficiency and signal detection efficiency.

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

第1図はこの発明の実施例、第2図はこの実施例の説明
用の図面、第3図はこの発明の他の実施例を示す斜視図
、第4図は従来例を示す図である。 (1)・・・コイル部、  (la)・・・タテ導体部
、  (1’b)・・・ヨコ導体部、(lc)・・・窓
部、(2)・・・コンデンサ、(3)・・・ガードリン
グ、  (3a)・・・トップガードリング、(3b)
・・・ボトムガードリング、(6)・・・端子、(7a
)、(’7b)・・・給電点、(8)−・・整合回路、
(aa)、(sb)、(sc) ・・・可変コンデンサ
、(9)・・弓/2波長ケーブル、αO・・・ギヤラス
αυ・・・リング。 なお、図中同一符号は同−又は相当部分を示す。
Fig. 1 is an embodiment of the present invention, Fig. 2 is an explanatory drawing of this embodiment, Fig. 3 is a perspective view showing another embodiment of the invention, and Fig. 4 is a diagram showing a conventional example. . (1) Coil part, (la) Vertical conductor part, (1'b) Horizontal conductor part, (lc) Window part, (2) Capacitor, (3 )...Guard ring, (3a)...Top guard ring, (3b)
... Bottom guard ring, (6) ... Terminal, (7a
), ('7b)... feeding point, (8) -... matching circuit,
(aa), (sb), (sc)...variable capacitor, (9)...bow/two-wavelength cable, αO...gear lath αυ...ring. Note that the same reference numerals in the figures indicate the same or equivalent parts.

Claims (6)

【特許請求の範囲】[Claims] (1)たて方向にのびる所定幅のタテ導体部とこの上端
部にこれと直交して左右にのびる所定幅のヨコ導体部を
有するT字型導体板を前記タテ導体部を軸方向として所
定の弧を描くように湾曲させたもの複数個を楕円状に隣
接して配列した第1の導体と、この第1の導体と略相似
の形状を有し、第1の導体とそれぞれの有するタテ導体
部が所定の間隔を履いて対向するよう配置された第2の
導体と、 前記第1の導体のヨコ導体部の内側に所定厚みの誘電体
を経て配置されたリング状の第1のガードリングと、前
記第2の導体のヨコ導体部の内側に所定厚みの誘電体を
経て配置されたリング状の第2のガードリング及びこの
2つのリングを接続し、前記第1のリングと第2のリン
グを平行移動的にうごかせるようにし、前記各リングと
それぞれが対面するタテ導体部との対向面積を変化して
その間の静電容量を変化させ得るようにした絶縁物でで
きたリングと、 前記第1の導体のタテ導体部に設けられた第1の給電点
と前記第2の導体の前記第1の導体のタテ導体部に対向
する位置のタテ導体部に設けられた第2の給電点とを介
して前記各導体に高周波平衡電流を給電する給電回路と
を備えたことを特徴とする高周波磁場発生・検出装置。
(1) A T-shaped conductor plate having a vertical conductor portion with a predetermined width extending in the vertical direction and a horizontal conductor portion with a predetermined width extending left and right at right angles to the upper end of the T-shaped conductor plate is set with the vertical conductor portion in the axial direction. A first conductor in which a plurality of conductors curved to draw an arc are arranged adjacently in an elliptical shape, and a first conductor having a shape substantially similar to the first conductor, and a vertical conductor respectively having a shape similar to the first conductor. a second conductor whose conductor parts are arranged to face each other with a predetermined interval; and a ring-shaped first guard which is arranged inside the horizontal conductor part of the first conductor through a dielectric material of a predetermined thickness. A ring, a ring-shaped second guard ring disposed inside the horizontal conductor portion of the second conductor through a dielectric material of a predetermined thickness, and these two rings are connected, and the first ring and the second guard ring are connected to each other. A ring made of an insulator, which is made to move in a parallel manner, and by changing the facing area of each ring and the vertical conductor portion facing each ring, the capacitance therebetween can be changed. , a first feeding point provided on the vertical conductor portion of the first conductor and a second feed point provided on the vertical conductor portion of the second conductor at a position opposite to the vertical conductor portion of the first conductor. A high-frequency magnetic field generation/detection device comprising: a power supply circuit that supplies a high-frequency balanced current to each of the conductors via a power supply point.
(2)立体回路は、導体板の外側に、所定の軸を中心軸
とする導体筒を有することを特徴とする特許請求の範囲
第1項記載の高周波磁場発生・検出装置。
(2) The high-frequency magnetic field generation/detection device according to claim 1, wherein the three-dimensional circuit has a conductor tube having a predetermined axis as its central axis on the outside of the conductor plate.
(3)平衡給電は、入力電流を1/2波長回路を経て逆
相としこの信号を各給電点へ給電することによつて達成
するようにしたことを特徴とする前記特許請求の範囲第
1項又は第2項に記載の高周波磁場発生・検出装置。
(3) Balanced power supply is achieved by passing the input current through a 1/2 wavelength circuit, reverse phase, and feeding this signal to each power supply point. The high frequency magnetic field generation/detection device according to item 1 or 2.
(4)平衡給電は入力電流をλ/2回路とインピーダン
スマッチング回路を経て各給電点へ給電することによつ
て達成するようにしたことを特徴とする前記特許請求の
範囲第1項ないし第3項のいずれかに記載の高周波磁場
発生・検出装置。
(4) Balanced power supply is achieved by supplying input current to each power supply point via a λ/2 circuit and an impedance matching circuit. The high frequency magnetic field generation/detection device according to any one of paragraphs.
(5)給電を前記給電点の1組又は複数組に対して行い
、給電しない給電点は所定のインピーダンスを接続する
ことを特徴とする前記特許請求の範囲第1項ないし第4
項のいずれかに記載の高周波磁場発生・検出装置。
(5) The power is supplied to one or more sets of the power supply points, and the power supply points to which power is not supplied are connected to a predetermined impedance.
The high frequency magnetic field generation/detection device according to any one of paragraphs.
(6)隣接するT字型導体板のヨコ導体部を所定の静電
容量を介して接続して第1の導体及び第2の導体が構成
されていることを特徴とする前記特許請求の範囲第1項
ないし第5項のいずれかに記載の高周波磁場発生・検出
装置。
(6) The scope of the above claim, characterized in that the first conductor and the second conductor are constructed by connecting horizontal conductor portions of adjacent T-shaped conductor plates via a predetermined capacitance. The high frequency magnetic field generation/detection device according to any one of Items 1 to 5.
JP61179527A 1986-02-18 1986-07-29 Device for generating and detecting high frequency magnetic field Pending JPS6334906A (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP61179527A JPS6334906A (en) 1986-07-29 1986-07-29 Device for generating and detecting high frequency magnetic field
US07/013,901 US4755756A (en) 1986-02-18 1987-02-12 Radio frequency coil for nuclear magnetic resonance imaging

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61179527A JPS6334906A (en) 1986-07-29 1986-07-29 Device for generating and detecting high frequency magnetic field

Publications (1)

Publication Number Publication Date
JPS6334906A true JPS6334906A (en) 1988-02-15

Family

ID=16067317

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61179527A Pending JPS6334906A (en) 1986-02-18 1986-07-29 Device for generating and detecting high frequency magnetic field

Country Status (1)

Country Link
JP (1) JPS6334906A (en)

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