JPH088917B2 - High frequency probe for NMR - Google Patents
High frequency probe for NMRInfo
- Publication number
- JPH088917B2 JPH088917B2 JP62103190A JP10319087A JPH088917B2 JP H088917 B2 JPH088917 B2 JP H088917B2 JP 62103190 A JP62103190 A JP 62103190A JP 10319087 A JP10319087 A JP 10319087A JP H088917 B2 JPH088917 B2 JP H088917B2
- Authority
- JP
- Japan
- Prior art keywords
- nmr
- frequency probe
- conductor
- high frequency
- capacitor
- 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
Links
Landscapes
- Magnetic Resonance Imaging Apparatus (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、NMR(核磁気共鳴)用高周波プローブ、
特に同時に用いられる低周波パルス磁場との磁気的干渉
がないNMR用高周波プローブに関するものである。DETAILED DESCRIPTION OF THE INVENTION [Industrial field of application] The present invention relates to a high-frequency probe for NMR (nuclear magnetic resonance),
In particular, the present invention relates to a high-frequency probe for NMR that does not cause magnetic interference with a low-frequency pulsed magnetic field used at the same time.
第3図は、例えば「ジヤーナル・オブ・マグネテイツ
ク・レゾナンス(Journal of Magnetic Resonanc
e)」、第36巻、第447頁〜第451頁(1979年)に示され
ている従来のNMR用高周波プローブを示す斜視図であ
る。図において、(1)はH字型をした1対の導体板例
えば銅板が中空筒状体を構成するように配置されたコイ
ルであり、バーチカル・バンド(vertical band)と呼
ばれる非突出部(1a)およびウイング(wing)と呼ばれ
る突出部(1b)を有している。(2)は隣接する突出部
(1b)間に挿入されかつ突出部(1b)にはんだづけされ
た固定コンデンサである。(3)は突出部(1b)の内側
に絶縁層(図示しない)を介して配置された電界シール
ド用の1対の導体環であり、一方の導体環(3a)がトツ
ブ・ガード・リングと呼ばれかつ他方の導体環(3b)が
ボトム・ガード・リングと呼ばれる。FIG. 3 shows, for example, “Journal of Magnetic Resonanc”.
e) ”, Vol. 36, pp. 447 to 451 (1979), which is a perspective view showing a conventional high-frequency probe for NMR. In the figure, (1) is a coil in which a pair of H-shaped conductor plates, for example, copper plates are arranged so as to form a hollow cylindrical body, and a non-protruding portion (1a) called a vertical band (vertical band). ) And a wing (1b). (2) is a fixed capacitor that is inserted between the adjacent protrusions (1b) and soldered to the protrusions (1b). (3) is a pair of conductor rings for electric field shielding that are arranged inside the protrusion (1b) via an insulating layer (not shown), and one conductor ring (3a) is a tob guard ring. And the other conductor ring (3b) is called the bottom guard ring.
従来のNMR用高周波プローブは上述したように構成さ
れ、コイル(1)、固定コンデンサ(2)、および導体
環(3)が等価的にLC直列共振回路として働く立体回路
を形成する。なお、導体環(3)は上述したように電界
シールドのため、即ちNMR用高周波プローブ内に測定対
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
失を低減するために用いられる。実際、このNMR用高周
波プローブを用いてNMR映像を得る場合には、公知の傾
斜磁場パルスを試料に同時に印加する。The conventional high frequency probe for NMR is configured as described above, and the coil (1), the fixed capacitor (2), and the conductor ring (3) form a three-dimensional circuit equivalently acting as an LC series resonance circuit. The conductor ring (3) is used for the electric field shield as described above, that is, for reducing the dielectric loss in the measurement target due to the generated electric field when the measurement target is installed in the high frequency probe for NMR. In fact, when an NMR image is obtained using this high-frequency probe for NMR, a known gradient magnetic field pulse is simultaneously applied to the sample.
従来のNMR用高周波プローブでは、傾斜磁場パルスの
印加に伴ない、非突出部(1a)にうず電流が流れるの
で、傾斜磁場パルスに波形歪や位相歪が生じるという問
題点があつた。In the conventional high-frequency probe for NMR, an eddy current flows through the non-protruding portion (1a) with the application of the gradient magnetic field pulse, which causes a problem that waveform distortion or phase distortion occurs in the gradient magnetic field pulse.
この発明は、このような問題点を解決するためになさ
れたもので、傾斜磁場パルスに波形歪や位相歪を生じな
いNMR用高周波プローブを得ることを目的とする。The present invention has been made to solve such a problem, and an object thereof is to obtain a high-frequency probe for NMR that does not cause waveform distortion or phase distortion in a gradient magnetic field pulse.
この発明に係るNMR用高周波プローブは、従来装置に
おける非突出部を複数本の導電セグメントで構成し、少
なくとも一部の導電セグメントにコンデンサを挿入した
ものである。In the high frequency probe for NMR according to the present invention, the non-protruding portion in the conventional device is composed of a plurality of conductive segments, and a capacitor is inserted in at least a part of the conductive segments.
この発明においては、導電セグメントに挿入されたコ
ンデンサがうず電流をしや断する。In the present invention, the capacitor inserted in the conductive segment turns on or off the eddy current.
第1図はこの発明の一実施例を示す斜視図であり、
(2)および(3)は従来装置におけるものと全く同一
である。(11)は中空筒状体例えば円筒または楕円筒を
構成するように配置されたコイルであり、このコイル
(11)は2対の導体板例えば銅板(11a)および(11b)
と、上下の導体板同士(11aと11b)を接続してH字型を
なす複数体の導電セグメント(11c)とから成る。各導
電セグメント(11c)は例えば細い導体板、導線または
導体パイプである。なお、上側の導体板同士(11a)は
彎曲させられた後に固定コンデンサ(2)によつて結合
され、同様に下側の導体板同士(11b)も彎曲させられ
た後に固定コンデンサ(2)によつて結合され、もつて
上述した中空筒状体を構成する。更に、導電セグメント
(11c)にはコンデンサ(12)が個別に挿入されてお
り、しかもこれらコンデンサ(12)の静電容量Cを例え
ば0.1μF〜0.01μF程度にしておく。その結果、この
コンデンサ(12)のインピーダンスは、1KHzでは1600Ω
〜16000Ωであり、また60MHzでは0.03Ω〜0.3Ωとな
る。FIG. 1 is a perspective view showing an embodiment of the present invention,
(2) and (3) are exactly the same as in the conventional device. (11) is a coil arranged so as to form a hollow cylindrical body such as a cylinder or an elliptic cylinder, and the coil (11) includes two pairs of conductor plates such as copper plates (11a) and (11b).
And the upper and lower conductor plates (11a and 11b) are connected to each other to form a plurality of H-shaped conductive segments (11c). Each conductive segment (11c) is, for example, a thin conductor plate, conductor wire or conductor pipe. The upper conductor plates (11a) are bent and then joined by a fixed capacitor (2). Similarly, the lower conductor plates (11b) are also bent and then fixed capacitor (2). They are joined together to form the hollow cylindrical body described above. Furthermore, capacitors (12) are individually inserted in the conductive segments (11c), and the capacitance C of these capacitors (12) is set to, for example, about 0.1 μF to 0.01 μF. As a result, the impedance of this capacitor (12) is 1600Ω at 1KHz.
It is ~ 16000Ω and 0.03Ω ~ 0.3Ω at 60MHz.
さらに傾斜磁場パルスの周波数は約1KHz,NMR信号の周
波数は例えば60MHz程度である。従つて、コンデンサ(1
2)の存在は、例えば60MHzの高周波プローブの動作に
は、インピーダンスが小さいので影響を与えない。Further, the frequency of the gradient magnetic field pulse is about 1 KHz, and the frequency of the NMR signal is, for example, about 60 MHz. Therefore, the capacitor (1
The presence of 2) does not affect the operation of the high-frequency probe of 60 MHz, for example, because the impedance is small.
しかし、傾斜磁場に由来するうず電流の周波数に対し
ては1KΩ以上の抵抗となるのでうず電流をしや断でき
る。However, the resistance of the eddy current due to the gradient magnetic field is 1 KΩ or more, so the eddy current can be turned off or turned off.
第2図に、コンデンサ(12)がないときのうず電流の
経路を矢印で示した。In FIG. 2, the path of the eddy current when there is no capacitor (12) is shown by an arrow.
なお、上記実施例では、全ての導電セグメント(11
c)にコンデンサ(12)を挿入したが、コンデンサ(1
2)が挿入されていない導電セグメント(11c)があつて
もよい。In the above embodiment, all the conductive segments (11
The capacitor (12) was inserted in c), but the capacitor (1
There may be a conductive segment (11c) in which 2) is not inserted.
また、上記実施例では中空筒状体を円筒にしたが、こ
れを楕円筒にしてもよい。Further, in the above embodiment, the hollow cylindrical body is a cylinder, but it may be an elliptic cylinder.
さらに、2対の導体板(11a)および(11b)を使用し
たが、例えば各導体板を2分割以上に分割することによ
り4対以上の導体板を使用することもできる。Further, although two pairs of conductor plates (11a) and (11b) are used, four or more pairs of conductor plates can be used by dividing each conductor plate into two or more.
また、導電セグメントは銅パイプ以外に、銅線幅が狭
い銅板でもよい。In addition to the copper pipe, the conductive segment may be a copper plate having a narrow copper wire width.
以上のように、この発明によれば、従来装置における
非突出部を複数本の導電セグメントで構成し、少なくと
も一部の導電セグメントにコンデンサを挿入したので、
傾斜磁場パルスに波形歪や位相歪を生じさせないNMR用
高周波プローブが得られる効果がある。As described above, according to the present invention, the non-protruding portion in the conventional device is composed of a plurality of conductive segments, and the capacitor is inserted in at least a part of the conductive segments.
There is an effect that a high-frequency probe for NMR that does not cause waveform distortion or phase distortion in the gradient magnetic field pulse can be obtained.
第1図はこの発明の一実施例を示す斜視図、第2図はう
ず電流の経路を示す図、第3図は従来のNMR用高周波プ
ローブを示す斜視図である。 図において、(11)はコイル、(11a)と(11b)は導体
板、(11c)は導電セグメント、(2)は固定コンデン
サ、(3)は導体環、(12)はコンデンサである。 なお、図中、同一符号は同一、又は相当部分を示す。FIG. 1 is a perspective view showing an embodiment of the present invention, FIG. 2 is a view showing an eddy current path, and FIG. 3 is a perspective view showing a conventional high frequency probe for NMR. In the figure, (11) is a coil, (11a) and (11b) are conductor plates, (11c) is a conductive segment, (2) is a fixed capacitor, (3) is a conductor ring, and (12) is a capacitor. In the drawings, the same reference numerals indicate the same or corresponding parts.
Claims (6)
を接続する複数本の導電セグメントによつて中空筒状体
を構成するように配置されたコイルと、同一平面にある
導体板同士を接続する固定コンデンサと、前記同一平面
にある導体板の内側にそれらと同心に設置された導体環
と、少なくとも一部の導電セグメントに挿入されたコン
デンサとを備えたことを特徴とするNMR用高周波プロー
ブ。1. A coil arranged to form a hollow cylindrical body by two or more pairs of conductor plates and a plurality of conductive segments connecting upper and lower conductor plates, and conductor plates on the same plane. For NMR, characterized in that it comprises a fixed capacitor for connecting, a conductor ring concentrically installed inside the conductor plate on the same plane, and a capacitor inserted in at least a part of the conductive segment. High frequency probe.
特許請求の範囲第1項記載のNMR用高周波プローブ。2. The high frequency probe for NMR as set forth in claim 1, wherein the hollow cylindrical body is a cylinder.
る特許請求の範囲第1項記載のNMR用高周波プローブ。3. The high-frequency probe for NMR as set forth in claim 1, wherein the hollow cylindrical body is an elliptic cylinder.
特徴とする特許請求の範囲第1項ないし第3項のいずれ
か記載のNMR用高周波プローブ。4. The high frequency probe for NMR as set forth in claim 1, wherein the conductive segment is a thin conductor plate.
する特許請求の範囲第1項ないし第3項のいずれか記載
のNMR用高周波プローブ。5. The high frequency probe for NMR as set forth in claim 1, wherein the conductive segment is a conductive wire.
特徴とする特許請求の範囲第1項ないし第3項のいずれ
か記載のNMR用高周波プローブ。6. A high-frequency probe for NMR use according to claim 1, wherein the conductive segment is a conductor pipe.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62103190A JPH088917B2 (en) | 1987-04-28 | 1987-04-28 | High frequency probe for NMR |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62103190A JPH088917B2 (en) | 1987-04-28 | 1987-04-28 | High frequency probe for NMR |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63270035A JPS63270035A (en) | 1988-11-08 |
| JPH088917B2 true JPH088917B2 (en) | 1996-01-31 |
Family
ID=14347601
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62103190A Expired - Lifetime JPH088917B2 (en) | 1987-04-28 | 1987-04-28 | High frequency probe for NMR |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH088917B2 (en) |
-
1987
- 1987-04-28 JP JP62103190A patent/JPH088917B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63270035A (en) | 1988-11-08 |
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