JPH0450011Y2 - - Google Patents

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Publication number
JPH0450011Y2
JPH0450011Y2 JP8547186U JP8547186U JPH0450011Y2 JP H0450011 Y2 JPH0450011 Y2 JP H0450011Y2 JP 8547186 U JP8547186 U JP 8547186U JP 8547186 U JP8547186 U JP 8547186U JP H0450011 Y2 JPH0450011 Y2 JP H0450011Y2
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JP
Japan
Prior art keywords
coil
coil wire
surf
nuclear magnetic
magnetic field
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
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JP8547186U
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Japanese (ja)
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JPS62197812U (en
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Priority to JP8547186U priority Critical patent/JPH0450011Y2/ja
Publication of JPS62197812U publication Critical patent/JPS62197812U/ja
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Description

【考案の詳細な説明】 産業上の利用分野 本考案はたとえば人体などの診断に利用される
核磁気共鳴信号の送受信のためのいわゆるRF(高
周波)コイルに関し、更に詳細には当接面近傍の
みの核磁気共鳴信号を送受信するためのサーフエ
スコイルに関するものである。
[Detailed description of the invention] Industrial application field The present invention relates to a so-called RF (high frequency) coil for transmitting and receiving nuclear magnetic resonance signals used for diagnosing the human body, and more specifically, it relates to a so-called RF (high frequency) coil for transmitting and receiving nuclear magnetic resonance signals used for diagnosing the human body. The present invention relates to a surf coil for transmitting and receiving nuclear magnetic resonance signals.

従来の技術 たとえば核磁気共鳴信号を利用して人体などを
診断する際には、所要の磁場を設定し、コイルに
よつて高周波を印加して原子核を共鳴させ、被検
体からの核磁気共鳴信号を受信する。
Conventional technology For example, when diagnosing the human body using nuclear magnetic resonance signals, a required magnetic field is set, a high frequency is applied by a coil to cause the atomic nuclei to resonate, and the nuclear magnetic resonance signals from the subject are detected. receive.

一般に、磁場強度は0.2テスラから2テスラが
用いられ、従つて原子核の共鳴周波数は、およそ
5MHzから600MHzである。人体の所要部分の診断
に使用されるサーフエスコイルは、インダクタ
と、導線の自己容量の影響を除去するためのキヤ
パシタとよりなる。インダクタの多くは核磁気共
鳴用磁石の大きさに制限され、最大外形寸法は1
cm〜30cm程度であり、1ターン以上の円環状、2
〜3ターン以上の渦巻状に構成され、被検体たる
人体の頭部、眼、腕、頸部等に空間的にフイツト
するように形成されることが多かつた。インダク
タより生起する磁界は、円環状インダクタの場
合、円環の垂直方向ではその半径の距離まで充分
な強度を以て及ぶことが知られている。従つて、
従来のサーフエスコイルは、そのインダクタの幾
何学的等価半径と呼ぶべき距離、即ち、そのイン
ダクタを人体表面等に配置したとき、その人体表
面からインダクタの幾何学的等価半径の深さま
で、生起される磁界が及ぶものである。また、核
磁気共鳴信号の受信の際においても、インダクタ
の幾何学的等価半径の距離の点からの核磁気共鳴
信号を受信し得るものであつた。
Generally, the magnetic field strength used is 0.2 Tesla to 2 Tesla, so the resonance frequency of the atomic nucleus is approximately
5MHz to 600MHz. A surf coil used for diagnosing a required part of the human body consists of an inductor and a capacitor for eliminating the influence of the self-capacitance of the conductor. Most inductors are limited by the size of nuclear magnetic resonance magnets, and the maximum external dimensions are 1
cm to 30cm, circular shape with one or more turns, two
It is often formed in a spiral shape with ~3 turns or more, and spatially fits around the head, eyes, arms, neck, etc. of a human subject. It is known that in the case of an annular inductor, the magnetic field generated by an inductor has sufficient strength and extends up to a distance of the radius of the annular ring in the perpendicular direction. Therefore,
Conventional surf coils are generated at a distance that can be called the geometric equivalent radius of the inductor, that is, when the inductor is placed on the human body surface, the inductor is generated from the human body surface to the depth of the inductor's geometric equivalent radius. This is the area where the magnetic field reaches. Also, when receiving nuclear magnetic resonance signals, it was possible to receive the nuclear magnetic resonance signals from a point at a distance of the geometrically equivalent radius of the inductor.

考案が解決しようとする問題点 例えば人体の皮膚、顔面表情筋肉等のインダク
タ当接表面に垂直方向の比較的浅い距離に存在す
る組織の核磁気共鳴現象を観測したい必要性がし
ばしばある。ところが、皮膚の核磁気共鳴現象だ
けを観測しようとしても、従来のサーフエスコイ
ルを用いれば、インダクタの生起する磁界が比較
的遠方に及んで皮膚より深い筋肉組織の核磁気共
鳴現象が併せ観測されてしまい、望ましからぬバ
ツクグラウンド信号として筋肉組織からの信号が
併せ観測されることが多かつた。つまり或程度の
広い範囲を観測したい場合に、当接面に垂直方向
の比較的深い所の有害信号が影響することにな
り、逆にその悪影響を避けるために、コイルを小
さくすると、浅い所の信号のみ観測できるが、所
要の広範囲の領域をカバーできないという問題点
があつた。
Problems to be Solved by the Invention There is often a need to observe nuclear magnetic resonance phenomena in tissues that exist at a relatively shallow distance in the direction perpendicular to the inductor contact surface, such as human skin or facial expression muscles. However, even if one attempts to observe only nuclear magnetic resonance phenomena in the skin, if a conventional SURFS coil is used, the magnetic field generated by the inductor will extend over a relatively long distance, making it difficult to observe nuclear magnetic resonance phenomena in muscle tissue deeper than the skin. As a result, signals from muscle tissue were often observed together as undesirable background signals. In other words, when you want to observe a fairly wide range, harmful signals from a relatively deep place perpendicular to the contact surface will affect the contact surface, and conversely, if you make the coil smaller to avoid that negative effect, it will affect the signal from a shallower place. Although only the signal can be observed, there is a problem in that it cannot cover the wide area required.

本考案は以上のような点に鑑みてなされたもの
で、その目的とするところは、コイルに垂直な方
向の比較的浅い所に磁気感応せしめ、しかも同一
面内の所要領域に亘つて磁気感応せしめ得るサー
フエスコイルを提供することにある。
The present invention was developed in view of the above points, and its purpose is to generate magnetic sensitivity in a relatively shallow area perpendicular to the coil, and to spread magnetic sensitivity over a required area within the same plane. Our goal is to provide a surf coil that can be used as a surfboard.

問題点を解決するための手段 本考案は、高周波信号を送信し、または核磁気
共鳴信号を受信するための核磁気共鳴装置用サー
フエスコイルであつて、観測領域より遠方では磁
界がキヤンセルするように複数のコイル線素が同
一面内にほぼ等間隔で対向して配設されているこ
とを特徴とするサーフエスコイルである。本考案
のサーフエスコイル線素は、診断すべき被検体な
どの当接すべき測定領域に対応した所要領域に亘
つて配設されており、同一平面内にある場合が多
いが、診断すべき被検体部分が彎曲している場合
には、曲面状または可撓性に設定されることもあ
る。領域内の各点の周囲にはコイル線素が対向配
設されているが、対向は実質的に2つのコイル線
素が対峙する場合、2組の平行するコイル線素に
よりなる場合、多角形に囲繞するコイル線素より
なる場合など特別の制限はない。対向するコイル
線素には逆向きの電流が発生せしめられる。すな
わち領域内の各点では周囲の対向するコイル線素
にはベクトル的に各点を同一モーメント向きに電
流が発生することになる。磁気感応にはサーフエ
スコイルより被検体などに磁場を作用させる場合
と、被検体の核磁気信号などをサーフエスコイル
が受信する場合が含まれる。前者の場合には高周
波発振装置などよりサーフエスコイルに電流が供
給され、後者の場合には、被検体の核磁気信号な
どによつてサーフエスコイルに電流が発生し、サ
ーフエスコイルに連絡されている受信装置に送ら
れる。
Means for Solving the Problems The present invention is a surf coil for a nuclear magnetic resonance apparatus for transmitting high frequency signals or receiving nuclear magnetic resonance signals, and is designed to cancel the magnetic field far from the observation area. A SURF S coil is characterized in that a plurality of coil wire elements are arranged facing each other at approximately equal intervals in the same plane. The SURF S coil wire element of the present invention is arranged over the required area corresponding to the measurement area to be contacted such as the subject to be diagnosed, and although it is often located in the same plane, If the subject part is curved, it may be set to be curved or flexible. Coil wire elements are arranged facing each other around each point in the area, and when the opposite is actually two coil wire elements facing each other, or two sets of parallel coil wire elements, the opposite is a polygon. There are no special restrictions, such as when it consists of a coil element surrounded by a coil element. Currents in opposite directions are generated in the opposing coil wire elements. That is, at each point within the region, a current is generated in the surrounding opposing coil wire elements in the same moment direction vectorwise at each point. Magnetic sensitivity includes cases in which a magnetic field is applied to a subject by a SURF S coil, and cases in which a SURF S coil receives nuclear magnetic signals from the subject. In the former case, a current is supplied to the SURF S coil from a high-frequency oscillator, and in the latter case, a current is generated in the SURF S coil by a nuclear magnetic signal from the subject, etc., and is communicated to the SURF S coil. is sent to the receiving device.

作 用 導体に電流が流れると、その周囲に磁界が生起
される。相互に逆向きの導体の往路と復路とが互
いに近接して配置されると、導体の往路または復
路のいずれかの極く近傍では、その近い側の導体
に流れる向きの電流によつて生起される磁界が発
生する。往路および復路の双方から遠方の点にお
ける磁界は、往路と復路の各々の導体に流れる電
流によつて生起される各々の磁界のベクトル和と
して、キヤンセルされるので、結局、本考案のサ
ーフエスコイルのインダクタが生起する磁界は、
サーフエスコイルに垂直方向の遠方に及ばない。
サーフエスコイルのコイル線素表面から、生起さ
れる磁界の及ぶ距離は、インダクタを構成する導
体の各々に流れる電流についてビオ・サバールの
法則によつて計算される。
Effect When current flows through a conductor, a magnetic field is generated around it. When the forward and return paths of a conductor with mutually opposite directions are placed close to each other, in the immediate vicinity of either the forward or return path of the conductor, a current generated in the direction flowing in the conductor on the near side is generated. A magnetic field is generated. Since the magnetic field at a point far from both the outward and return paths is canceled as a vector sum of the respective magnetic fields generated by the currents flowing through the conductors of the outbound and return paths, the SURF S coil of the present invention The magnetic field generated by the inductor is
It does not extend far vertically to the surf coil.
The distance that the generated magnetic field extends from the surface of the coil wire of the SURF S coil is calculated using the Biot-Savart law for the current flowing through each of the conductors constituting the inductor.

実施例 第1図において、コイル線素1は35mm×55mmの
長方形の同一平面にジグザグ状に平行して配設さ
れている。コイル線素1は長方形の領域全域にお
いて対向配置され、近傍するコイル線素1の間隔
は5mmに設定されている。形体的には、電気絶縁
性、高周波損失特性、耐熱性、可撓性などの良好
な合成樹脂などの材料よりなるシートに銅などの
金属線が固着されているもの、あるいはプリント
配線などの手法によつて基盤にコイル線素が形成
されたものなど格別の制限はない。コイル線素1
の端部は端子2、導線3を経由して所要の高周波
送受信装置(図示されない)などに連絡せしめら
れる。
Embodiment In FIG. 1, coil wire elements 1 are arranged parallel to each other in a zigzag pattern on the same plane of a rectangle measuring 35 mm x 55 mm. The coil wire elements 1 are arranged facing each other over the entire rectangular area, and the interval between adjacent coil wire elements 1 is set to 5 mm. In terms of form, metal wires such as copper are fixed to a sheet made of a material such as synthetic resin with good electrical insulation, high frequency loss characteristics, heat resistance, and flexibility, or methods such as printed wiring. There are no particular restrictions, such as those in which a coil wire element is formed on the base. Coil wire element 1
The end thereof is connected to a required high frequency transmitting/receiving device (not shown) via a terminal 2 and a conductive wire 3.

高周波送信装置などより第1図のサーフエスコ
イルに高周波が印加されると、或る瞬間にはコイ
ル線素1に矢印の方向に電流が流れる。長方形の
領域全域の各点(厳密にはコイル線素1上の点以
外の)は周囲にコイル線素1が対向し、その対向
しているコイル線素1に逆向きの電流が流れる。
高周波電流の流れ方向が逆になつた瞬間には、コ
イル線素1に流れる電流の向きが第1図の矢印と
逆向きになるが、領域内の各点の周囲の対向して
いるコイル線素1には逆向きの電流が流れる。
When a high frequency wave is applied to the SURF S coil shown in FIG. 1 from a high frequency transmitter or the like, a current flows through the coil wire element 1 in the direction of the arrow at a certain moment. Each point in the entire rectangular area (strictly speaking, other than the points on the coil wire element 1) is surrounded by a coil wire element 1 that faces each other, and current flows in the opposite direction through the opposing coil wire elements 1.
At the moment when the flow direction of the high-frequency current is reversed, the direction of the current flowing through the coil wire element 1 becomes opposite to the arrow in Fig. 1, but the opposite coil wires around each point in the area A current in the opposite direction flows through element 1.

実際の核磁気共鳴診断装置のサーフエスコイル
では、通常、導線の自己容量の影響を除去するた
めに端子2間にキヤパシタCが取りつけられてい
るが、このことは、第2図のように、本考案にも
適用される。
In the actual SURF S coil of nuclear magnetic resonance diagnostic equipment, a capacitor C is usually installed between the terminals 2 to eliminate the influence of the self-capacitance of the conductor, as shown in Figure 2. This also applies to the present invention.

以上は、サーフエスコイルに電流を印加して磁
界を発生させる場合について説明したが、核磁気
信号など磁界によつてサーフエスコイルに電流が
起り外部の受信装置などに伝達される場合にも同
様に適用される。
The above explanation deals with the case where a magnetic field is generated by applying a current to the SURF S coil, but the same applies when a current is generated in the SURF S coil due to a magnetic field such as a nuclear magnetic signal and is transmitted to an external receiving device, etc. applied to.

別の実施例である第4図において、コイル線素
1は直径35mmの円状平面に5mmの間隔を以て同心
円状に配設されている。各円のコイル線素は円の
一部で切欠かれて隣接する円のコイル線素に連絡
せしめられている。最外円のコイル線素に端子2
が設けられ、導線3を経由して所要の高周波送受
信装置などに連絡せしめられる。領域内の各点の
周囲の対向しているコイル線素1には逆向きの電
流が流れる。
In FIG. 4, which is another embodiment, coil wire elements 1 are arranged concentrically on a circular plane having a diameter of 35 mm with an interval of 5 mm. The coil wire elements of each circle are cut out at a part of the circle and connected to the coil wire elements of the adjacent circle. Terminal 2 on the outermost coil wire element
is provided, and is connected to a required high frequency transmitting/receiving device etc. via a conductor 3. Currents in opposite directions flow in the coil wire elements 1 facing each other around each point in the area.

第4図は領域が円状になつているが、同じ相対
配置の考え方で長円状に形成することも、あるい
は正方形、長方形状に形成することも容易に可能
である。
Although the area is circular in FIG. 4, it is easily possible to form it in an elliptical shape, or in a square or rectangular shape using the same concept of relative arrangement.

別の実施例である第5図において、矩形波状の
コイル線素1A,1Bは各屈曲点が近接して全体
として基盤目状に配設されている。コイル線素1
A,1Bは、一つおきに逆方向に電流が流れるよ
うに、両端が内部導線4A,4Bに接続されてい
る。内部導線4A,4Bは端子2A,2B、導線
3A,3Bを経由して所要の高周波送受信装置な
どに連絡せしめられる。領域内の各点の周囲の対
向しているコイル線素1A,1Bには逆向きの電
流が流れる。なおこの場合、第5図の上下端は均
一磁界にならないので、サーフエスコイルの大き
さを所要の診断領域より多少大きく設計すれば良
い。
In FIG. 5, which is another embodiment, rectangular wave-like coil wire elements 1A and 1B are arranged in a grid pattern as a whole with respective bending points close to each other. Coil wire element 1
Both ends of A and 1B are connected to internal conductors 4A and 4B so that current flows in opposite directions in every other wire. The internal conducting wires 4A, 4B are connected to a required high frequency transmitting/receiving device etc. via terminals 2A, 2B and conducting wires 3A, 3B. Currents in opposite directions flow through the opposing coil wire elements 1A and 1B around each point in the area. In this case, since the upper and lower ends of FIG. 5 do not have a uniform magnetic field, the size of the SURF S coil may be designed to be somewhat larger than the required diagnostic area.

更に別の実施例の要部を示す第6図において、
等間隔で平行に配設されるコイル線素1Aに対
し、60度の傾きで交叉するコイル線素1Bが等間
隔で平行に配設され、120度の傾きで交叉するコ
イル線素1Cが等間隔で平行に配設される。コイ
ル線素1A,1B,1Cの各交叉点では電気的に
絶縁されている。電流は図示しない内部導線よ
り、コイル線素1Aでは右方へ、コイル線素1B
では左斜め下方へ、コイル線素1Cでは左斜め上
方へ、夫々、流される。内部導線、端子、導線な
どは前記の実施例と同様に配設される。
In FIG. 6 showing the main part of yet another embodiment,
Coil wire elements 1A are arranged in parallel at equal intervals, coil wire elements 1B are arranged in parallel at equal intervals and intersect at an angle of 60 degrees, and coil wire elements 1C are arranged in parallel at equal intervals at an angle of 120 degrees. Arranged in parallel at intervals. The coil wire elements 1A, 1B, and 1C are electrically insulated at each intersection point. The current flows from an internal conductor (not shown) to the right in coil wire element 1A, and to the right in coil wire element 1B.
In the case of the coil wire element 1C, it flows diagonally downward to the left, and in the case of the coil wire element 1C, it flows diagonally upward to the left. Internal conductors, terminals, conductors, etc. are arranged in the same manner as in the previous embodiment.

高周波電流はコイル線素の表面を流れる性質が
あるが、その場合には例えば第7図のような板状
のコイル線素が利用される。第7図において、厚
さ0.3mm、巾5mmの銅板が5mmの間隔を以て平行
にジグザグ状に形成されている。両端には所要の
導線などが接続される。このコイル線素は10〜
100MZzの高周波要に使用可能である。
The high frequency current has a property of flowing on the surface of a coil wire element, and in this case, for example, a plate-shaped coil wire element as shown in FIG. 7 is used. In FIG. 7, copper plates having a thickness of 0.3 mm and a width of 5 mm are formed in parallel in a zigzag shape with an interval of 5 mm. Required conductor wires and the like are connected to both ends. This coil wire element is 10~
Can be used for high frequency requirements of 100MZz.

効 果 以上説明したように、本考案は電流を印加され
たコイル線素に垂直な方向に磁界を及ぼすサーフ
エスコイルとして、また核磁気信号などの磁界に
よつてコイル線素に電流を発生して、その電流に
よつて磁界の状況を伝達するためのサーフエスコ
イルとして利用される際に、磁気感応する範囲が
サーフエスコイルの垂直方向の近傍内に特定し、
しかもサーフエスコイルとしての大きさ(所要領
域)が前記の近傍の値と無関係に設定することが
できるので、人体などの被検体の状況を診断する
核磁気共鳴情報処理装置に極めて有用である。
Effects As explained above, the present invention can be used as a surf coil that generates a magnetic field in a direction perpendicular to a coil element to which a current is applied, or as a surface coil that generates a current in a coil element by a magnetic field such as a nuclear magnetic signal. When used as a SURF S coil to transmit the state of the magnetic field by the current, the magnetically sensitive range is specified within the vicinity of the SURF S coil in the vertical direction,
Moreover, since the size (required area) of the surface coil can be set independently of the above-mentioned neighboring values, it is extremely useful for a nuclear magnetic resonance information processing apparatus for diagnosing the condition of a subject such as a human body.

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

第1図は本考案の一実施例の同一平面内の所要
領域に配設されるコイル線素の状況を示す模式
図、第2図は導線の自己容量の影響を除去するた
めにキヤパシタを接続した状況を示す配線図、第
3図は従来のサーフエスコイルの模式図、第4
図、第5図は別の実施例の同一平面内の所要領域
に配設されるコイル線素の状況を示す模式図、第
6図は別の実施例のコイル線素の要部を示す模式
図、第7図は高周波用の実施例のコイル線素を示
す斜視図である。 1……コイル線素、2……端子、3……導線、
4……内部導線、C……キヤパシタ、L……イン
ダクタ。
Fig. 1 is a schematic diagram showing the situation of coil wire elements arranged in the required area in the same plane in one embodiment of the present invention, and Fig. 2 shows the connection of capacitors to eliminate the influence of the self-capacitance of the conducting wire. Figure 3 is a schematic diagram of a conventional SurfS coil, Figure 4 shows a wiring diagram showing the situation
5 is a schematic diagram showing the situation of coil wire elements arranged in a required area in the same plane in another embodiment, and FIG. 6 is a schematic diagram showing the main parts of a coil wire element in another embodiment. FIG. 7 is a perspective view showing a coil wire element of an embodiment for high frequency use. 1... Coil wire element, 2... Terminal, 3... Conductor wire,
4... Internal conductor, C... Capacitor, L... Inductor.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 高周波信号を送信し、または核磁気共鳴信号を
受信するための核磁気共鳴装置用サーフエスコイ
ルであつて、観測領域より遠方では磁界がキヤン
セルするように複数のコイル線素が同一面内にほ
ぼ等間隔で対向して配設されていることを特徴と
するサーフエスコイル。
A surf coil for a nuclear magnetic resonance apparatus for transmitting high frequency signals or receiving nuclear magnetic resonance signals.Multiple coil wire elements are arranged approximately in the same plane so that the magnetic field is canceled in areas far from the observation area. Surf S coils are characterized by being arranged facing each other at equal intervals.
JP8547186U 1986-06-06 1986-06-06 Expired JPH0450011Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8547186U JPH0450011Y2 (en) 1986-06-06 1986-06-06

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8547186U JPH0450011Y2 (en) 1986-06-06 1986-06-06

Publications (2)

Publication Number Publication Date
JPS62197812U JPS62197812U (en) 1987-12-16
JPH0450011Y2 true JPH0450011Y2 (en) 1992-11-25

Family

ID=30940904

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8547186U Expired JPH0450011Y2 (en) 1986-06-06 1986-06-06

Country Status (1)

Country Link
JP (1) JPH0450011Y2 (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE10025582C1 (en) * 2000-05-24 2001-12-06 Siemens Ag Electrical conductor arrangement has conducting meshes in areas whose boundary lines are defined by net structure, electrical control devices electrically bound into meshes to control currents
JP2010233665A (en) * 2009-03-30 2010-10-21 Ge Medical Systems Global Technology Co Llc Coil, coil device, and magnetic resonance imaging apparatus
JP5581393B2 (en) * 2010-10-07 2014-08-27 株式会社日立メディコ Antenna apparatus and magnetic resonance imaging apparatus
JP2014087673A (en) * 2013-12-17 2014-05-15 Ge Medical Systems Global Technology Co Llc Coil device and magnetic resonance imaging device

Also Published As

Publication number Publication date
JPS62197812U (en) 1987-12-16

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