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JP2811891B2 - Adjustment method of static magnetic field uniformity - Google Patents
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JP2811891B2 - Adjustment method of static magnetic field uniformity - Google Patents

Adjustment method of static magnetic field uniformity

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Publication number
JP2811891B2
JP2811891B2 JP2085862A JP8586290A JP2811891B2 JP 2811891 B2 JP2811891 B2 JP 2811891B2 JP 2085862 A JP2085862 A JP 2085862A JP 8586290 A JP8586290 A JP 8586290A JP 2811891 B2 JP2811891 B2 JP 2811891B2
Authority
JP
Japan
Prior art keywords
magnetic field
static magnetic
nmr
sample
uniformity
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
JP2085862A
Other languages
Japanese (ja)
Other versions
JPH03286736A (en
Inventor
直人 飯島
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.)
Shimadzu Corp
Original Assignee
Shimadzu 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 Shimadzu Corp filed Critical Shimadzu Corp
Priority to JP2085862A priority Critical patent/JP2811891B2/en
Publication of JPH03286736A publication Critical patent/JPH03286736A/en
Application granted granted Critical
Publication of JP2811891B2 publication Critical patent/JP2811891B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION 【産業上の利用分野】[Industrial applications]

この発明は、NMRイメージング装置やNMRスペクトロメ
ータなどのMR装置における静磁場均一性を調整する方法
に関する。
The present invention relates to a method for adjusting static magnetic field uniformity in an MR device such as an NMR imaging device or an NMR spectrometer.

【従来の技術】[Prior art]

NMRイメージング装置やNMRスペクトロメータなどのMR
装置では、均一な静磁場が必要である。 従来、この静磁場の均一性を上げるための技術とし
て、静磁場内の空間各点の磁場分布を測定し、計算によ
りシムコイルに流す電流値を求める方法が公知である。 また、NMRスペクトロメータにおいては、第3図に示
すようにRFパルス(90゜パルス)31を照射することによ
って発生するNMR信号(FID信号)32を観測し、その信号
量が最大となるようにシムコイルに流す電流値を制御す
る方法が知られている。この場合、RFパルス31の繰り返
し時間TRは緩和時間よりも長く設定され、通常1秒程度
に選ばれる。
MR such as NMR imaging equipment and NMR spectrometer
The device requires a uniform static magnetic field. Conventionally, as a technique for improving the uniformity of the static magnetic field, there is known a method of measuring a magnetic field distribution at each point in space in the static magnetic field and calculating a current value flowing through the shim coil by calculation. In the NMR spectrometer, as shown in FIG. 3, an NMR signal (FID signal) 32 generated by irradiating an RF pulse (90 ° pulse) 31 is observed, and the signal amount is maximized. There is known a method of controlling a current value flowing through a shim coil. In this case, the repetition time TR of the RF pulse 31 is set longer than the relaxation time, and is usually selected to be about 1 second.

【発明が解決しようとする課題】[Problems to be solved by the invention]

しかしながら、空間各点の磁場分布を計測することは
測定時間が非常に長くかかることであり、また計算も大
変であるという問題がある。 また、FID信号を観測する方法は簡便であるが、通
常、90゜パルスの後の待ち時間を緩和時間よりも長くす
るため、パルス繰り返し時間TRを短くできないという問
題を有する。 この発明は、簡便で、且つパルス繰り返し時間を短く
することにより調整のための時間を短縮できる、静磁場
均一性の調整法を提供することを目的とする。
However, measuring the magnetic field distribution at each point in space requires a very long measurement time, and has a problem that the calculation is also difficult. Further, although the method of observing the FID signal is simple, it usually has a problem that the pulse repetition time TR cannot be shortened because the waiting time after the 90 ° pulse is longer than the relaxation time. SUMMARY OF THE INVENTION An object of the present invention is to provide a method for adjusting the uniformity of a static magnetic field, which is simple and can reduce the time for adjustment by shortening the pulse repetition time.

【課題を解決するための手段】[Means for Solving the Problems]

上記の目的を達成するため、この発明による静磁場均
一性の調整法においては、試料の緩和時間よりも短い繰
り返し時間でRFパルスを繰り返し照射して磁化を定常歳
差運動状態とし、この状態を保ちながら静磁場均一性補
正用シムコイルに流す電流値を操作して、観測されるNM
R信号が最大値となるような電流値を選ぶことが特徴と
なっている。
In order to achieve the above object, in the method for adjusting the uniformity of the static magnetic field according to the present invention, the magnetization is brought into a steady precession state by repeatedly irradiating an RF pulse with a repetition time shorter than the relaxation time of the sample. By controlling the value of the current flowing through the shim coil for correcting static magnetic field uniformity while maintaining it, the observed NM
It is characterized by selecting a current value such that the R signal has a maximum value.

【作用】[Action]

試料の緩和時間よりも短い繰り返し時間でRFパルスを
繰り返し照射することにより、磁化の定常歳差運動状態
を出現させることができる。 この定常歳差運動状態では、試料の各点の磁化は、そ
の点における静磁場強度に対応した位相で回転する。そ
のため、各点からのNMR信号は、その点での静磁場強度
を位相情報として含んでいることになる。そして、観測
されるNMR信号は、試料全体の各点からのNMR信号の和と
考えられる。 そこで、この定常歳差運動状態を持続させながら、均
一性補正用シムコイルに流す電流値を変化させて、NMR
信号が最大値となる電流値を選ぶならば、その電流値を
シムコイルに流すとき試料中の静磁場の均一性が最適な
ものとなる。
By repeatedly irradiating the RF pulse with a repetition time shorter than the relaxation time of the sample, a steady precession state of magnetization can appear. In this steady precession state, the magnetization at each point of the sample rotates with a phase corresponding to the static magnetic field strength at that point. Therefore, the NMR signal from each point includes the static magnetic field strength at that point as phase information. Then, the observed NMR signal is considered to be the sum of the NMR signals from each point of the entire sample. Therefore, while maintaining this steady precession state, the current value flowing through the uniformity correction shim coil was changed to
If the current value at which the signal has the maximum value is selected, the uniformity of the static magnetic field in the sample becomes optimal when the current value is passed through the shim coil.

【実 施 例】【Example】

以下、この発明の一実施例について図面を参照しなが
ら詳細に説明する。NMRイメージング装置やNMRスペクト
ロメータなどのMR装置では、第1図に示すように、主マ
グネット1内に、この主マグネット1が発生する静磁場
の均一性を補正するための補正用シムコイル2が配置さ
れ、このシムコイル2にシムコイル電源3より補正用の
電流が供給される。この主マグネット1が形成する静磁
場内にプローブ4が配置され、このプローブ4の中に図
示しない試料が置かれる。 このプローブ4にはNMR送受信機5が接続されてお
り、このプローブ4を通じてRF信号の送受が行われる。
パルスプログラマ6は、CPU7の制御のもとで、所定のパ
ルスシーケンスに基づきNMR送受信機5を制御して、こ
のNMR送受信機5からプローブ4にRF信号を供給させ
る。こうして試料にRF信号の照射が行われる。励起され
た試料の核スピンからNMR信号が放出され、このNMR信号
はプローブ4によって受信され送受信機5に送られる。
この送受信機5を経て得たNMRデータはCPU7に送られ
る。CPU7はこのNMRデータを監視するとともに、パルス
プログラマ6を介してシムコイル電源3をオンラインで
制御する。これにより、シムコイル2に流される電流が
増加、または減少させられることになる。 この発明の一実施例にかかる静磁場均一性の調整法で
は、第2図に示すようにRFパルス21が、繰り返し時間TR
で繰り返し照射される。この繰り返し時間TRは、プロー
ブ4内の試料の緩和時間T1,T2よりも十分に短いものと
する。このように繰り返し時間TRが試料の緩和時間T1,T
2よりも十分に短いと、磁化はSSFPと呼ばれる定常歳差
運動を行う状態となり、第2図に示すようにRFパルス21
の前後両側にNMR信号22が発生するような状態となる。
代表的な値としてT1=T2=500msとすると、TR=100ms程
度とすればこのSSFP状態となる。 このときのNMR信号の大きさは、 ただし、 Mx,Mr;回転系における横磁化 ω0;NMR共鳴周波数 Φ;TRの間の横磁化の回転量(∝H0) Ak;定数 で表される(なお、たとえばM.L.Gyngell,J.Mag.Reson,
81,474(1989)を参照)。 このときの試料の各部分を考えると、各部分はその場
所の静磁場の大きさによって定まるΦを持ち、その結
果、サンプルの各部分はその場所の静磁場の値に対応す
る位相を持つ信号を発生し、その試料全体からの信号の
和がプローブ4によって受信されるNMR信号として観測
されることになる。 そこで、パルス繰り返し時間TRをSSFP状態が持続でき
る程度(上記の例であれば100ms程度)に保ちながらシ
ムコイル2に流す電流値をオンライン制御し、受信NMR
信号が最大値になるように電流値を定める。 すると、このようにNMR信号が最大値となる状態で
は、試料の各部分の位相角Φが試料全体で均一になっ
て、試料全体から同じ位相を持ったNMR信号が発生して
いることになる。その結果、試料の各部分が感応してい
る静磁場の大きさが均一になり、非常に均一性の高い静
磁場を形成できたことになる。
Hereinafter, an embodiment of the present invention will be described in detail with reference to the drawings. In an MR apparatus such as an NMR imaging apparatus or an NMR spectrometer, as shown in FIG. 1, a correction shim coil 2 for correcting the uniformity of a static magnetic field generated by the main magnet 1 is arranged in the main magnet 1. Then, a correction current is supplied from the shim coil power supply 3 to the shim coil 2. A probe 4 is arranged in a static magnetic field formed by the main magnet 1, and a sample (not shown) is placed in the probe 4. An NMR transceiver 5 is connected to the probe 4, and an RF signal is transmitted and received through the probe 4.
The pulse programmer 6 controls the NMR transmitter / receiver 5 based on a predetermined pulse sequence under the control of the CPU 7, and causes the NMR transmitter / receiver 5 to supply an RF signal to the probe 4. Thus, the sample is irradiated with the RF signal. An NMR signal is emitted from the excited nuclear spin of the sample, and the NMR signal is received by the probe 4 and sent to the transceiver 5.
The NMR data obtained via the transceiver 5 is sent to the CPU 7. The CPU 7 monitors the NMR data and controls the shim coil power supply 3 online via the pulse programmer 6. As a result, the current flowing through the shim coil 2 is increased or decreased. In the method of adjusting the uniformity of the static magnetic field according to one embodiment of the present invention, as shown in FIG.
Irradiated repeatedly. The repetition time TR is sufficiently shorter than the relaxation times T1 and T2 of the sample in the probe 4. Thus, the repetition time TR is equal to the relaxation time T1, T
If it is sufficiently shorter than 2, the magnetization will be in a state of performing a steady precession called SSFP, and as shown in FIG.
The state is such that the NMR signal 22 is generated on both sides before and after.
Assuming that T1 = T2 = 500 ms as a representative value, this SSFP state is obtained when TR = about 100 ms. The magnitude of the NMR signal at this time is Where, Mx, Mr; transverse magnetization in a rotating system ω 0 ; NMR resonance frequency Φ; rotation amount of transverse magnetization during TR (∝H 0 ) Ak; constant (for example, see MLGyngell, J. Mag. Reson, IA US
81,474 (1989)). Considering each part of the sample at this time, each part has Φ determined by the magnitude of the static magnetic field at that location, and as a result, each part of the sample has a signal having a phase corresponding to the value of the static magnetic field at that location And the sum of the signals from the entire sample is observed as an NMR signal received by the probe 4. Therefore, while controlling the pulse repetition time TR to an extent that the SSFP state can be maintained (about 100 ms in the above example), the current value flowing through the shim coil 2 is controlled online, and the reception NMR is controlled.
The current value is determined so that the signal has the maximum value. Then, in such a state where the NMR signal has the maximum value, the phase angle Φ of each part of the sample becomes uniform over the entire sample, and an NMR signal having the same phase is generated from the entire sample. . As a result, the magnitude of the static magnetic field to which each part of the sample is sensitive becomes uniform, and a highly uniform static magnetic field can be formed.

【発明の効果】【The invention's effect】

この発明の静磁場均一性の調整法によれば、簡便で且
つ高速に均一性の高い静磁場を得ることができる。
According to the static magnetic field uniformity adjusting method of the present invention, a highly uniform static magnetic field can be obtained simply and at high speed.

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

第1図はこの発明の一実施例で用いる静磁場均一性補正
系のブロック図、第2図は同実施例における波形図、第
3図は従来例における波形図である。 1……主マグネット、2……シムコイル、3……シムコ
イル電源、4……プローブ、5……NMR送受信機、6…
…パルスプログラマ、7……CPU。
FIG. 1 is a block diagram of a static magnetic field uniformity correction system used in one embodiment of the present invention, FIG. 2 is a waveform diagram in the embodiment, and FIG. 3 is a waveform diagram in a conventional example. 1 ... Main magnet, 2 ... Shim coil, 3 ... Shim coil power supply, 4 ... Probe, 5 ... NMR transceiver, 6 ...
... pulse programmer, 7 ... CPU.

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】試料の緩和時間よりも短い繰り返し時間で
RFパルスを繰り返し照射して磁化を定常歳差運動状態と
し、この状態を保ちながら静磁場均一性補正用シムコイ
ルに流す電流値を操作して、観測されるNMR信号が最大
値となるような電流値を選ぶことを特徴とする静磁場均
一性の調整法。
1. A repetition time shorter than a relaxation time of a sample.
The RF pulse is repeatedly irradiated to set the magnetization to a steady precession state, and while maintaining this state, the current flowing through the shim coil for static magnetic field uniformity correction is manipulated so that the observed NMR signal becomes the maximum value. A method for adjusting the uniformity of the static magnetic field, characterized by selecting a value.
JP2085862A 1990-03-31 1990-03-31 Adjustment method of static magnetic field uniformity Expired - Lifetime JP2811891B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2085862A JP2811891B2 (en) 1990-03-31 1990-03-31 Adjustment method of static magnetic field uniformity

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2085862A JP2811891B2 (en) 1990-03-31 1990-03-31 Adjustment method of static magnetic field uniformity

Publications (2)

Publication Number Publication Date
JPH03286736A JPH03286736A (en) 1991-12-17
JP2811891B2 true JP2811891B2 (en) 1998-10-15

Family

ID=13870697

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2085862A Expired - Lifetime JP2811891B2 (en) 1990-03-31 1990-03-31 Adjustment method of static magnetic field uniformity

Country Status (1)

Country Link
JP (1) JP2811891B2 (en)

Also Published As

Publication number Publication date
JPH03286736A (en) 1991-12-17

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