JPH02209130A - High frequency output adjustment method - Google Patents

High frequency output adjustment method

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Publication number
JPH02209130A
JPH02209130A JP1029330A JP2933089A JPH02209130A JP H02209130 A JPH02209130 A JP H02209130A JP 1029330 A JP1029330 A JP 1029330A JP 2933089 A JP2933089 A JP 2933089A JP H02209130 A JPH02209130 A JP H02209130A
Authority
JP
Japan
Prior art keywords
pulse
high frequency
magnetic field
frequency output
magnetic resonance
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.)
Granted
Application number
JP1029330A
Other languages
Japanese (ja)
Other versions
JPH0572812B2 (en
Inventor
Masahiko Hatanaka
畑中 雅彦
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.)
Toshiba Corp
Original Assignee
Toshiba 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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP1029330A priority Critical patent/JPH02209130A/en
Publication of JPH02209130A publication Critical patent/JPH02209130A/en
Publication of JPH0572812B2 publication Critical patent/JPH0572812B2/ja
Granted legal-status Critical Current

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Abstract

PURPOSE:To exactly set the condition of a high frequency output such as a 90 deg. pulse or 180 pulse and to obtain an exact signal by setting slice thickness tick so as to include the whole uniform area of a maximum high frequency coil when the inclination angle of a spin system magnetic moment is adjusted to a prescribed value. CONSTITUTION:In a nuclear magnetic resonance imaging device 1, an inclined magnetic field generation coil 2 to generate an inclined magnetic field for obtaining the position information of a part, where a magnetic resonance signal is induced, and a high frequency coil 3 as a transmission/reception system to radiate a rotary high frequency magnetic field and to detect the induced magnetic resonance signal are provided. When an MR signal is obtained to set the high frequency output of the 90 deg. pulse and 180 deg. pulse, slice width S is set thick by adjusting a Z-axis inclined magnetic field, which is a magnetic field for slice, in advance so that the sensitivity of the maximum high frequency coil becomes the uniform area. Accordingly, even when a slice position is dislocated by breating motion, etc., for a part to be checked like the chest, the high frequency output of the 90 deg. pulse and 180 deg. pulse to induce a magnetic resonance phenomenon can be exactly adjusted and an exact tomographic picture can be obtained.

Description

【発明の詳細な説明】 [発明の目的] (産業上の利用分野) 本発明は、核磁気共鳴(NMR:Nuclear Ma
gnetic  Re5onance)現象を応用した
磁気共鳴イメージング方法に係わり、特に、励起回転磁
場発生に供される送信パルス電力を被検体の属性に応じ
て変化させることにより、スピン系磁気モーメントの倒
れ角度を所定の値に調整する高周波出力調整方法に関す
る。
[Detailed Description of the Invention] [Object of the Invention] (Industrial Application Field) The present invention is directed to nuclear magnetic resonance (NMR).
It is related to a magnetic resonance imaging method that applies the phenomenon of magnetic resonance (magnetic resonance), in particular, by changing the transmission pulse power used to generate an excitation rotating magnetic field according to the attributes of the subject, the inclination angle of the spin-based magnetic moment can be adjusted to a predetermined value. This invention relates to a high frequency output adjustment method for adjusting the output value.

(従来の技術) 核磁気共鳴現象は、磁場中におかれた原子核が特定波長
の電磁波エネルギーを共鳴吸収して、次いてこのエネル
ギーを電磁波として放出する現象である。この現象を利
用して生体の診断を行う装置は、上述の原子核、特に、
プロトンから放出される電磁波(以下MR倍信号いう。
(Prior Art) Nuclear magnetic resonance is a phenomenon in which atomic nuclei placed in a magnetic field resonate and absorb electromagnetic wave energy of a specific wavelength, and then emit this energy as electromagnetic waves. Devices that utilize this phenomenon to diagnose living organisms use the above-mentioned atomic nuclei, especially
Electromagnetic waves emitted from protons (hereinafter referred to as MR multiplied signals).

)を検知して、検知されたMR倍信号処理して、原子核
(プロトン)密度、縦緩和時間T 1横緩和時間T2、
流れ、化学シフト等の情報が反映された被検体の断層像
等の診断情報が得られる。
) is detected, the detected MR signal is processed, and the atomic nucleus (proton) density, longitudinal relaxation time T1, transverse relaxation time T2,
Diagnostic information such as a tomographic image of the subject reflecting information such as flow and chemical shift can be obtained.

ところで、この様な核磁気共鳴現象を利用してプロトン
からのMR倍信号検知するためには、901′パルスお
よび180°と称される高周波パルスにより発生される
励起回転磁場により、被検体の被測定部位を選択的に励
起して、被測定部位におけるプロトンのスピン磁気モー
メントの倒れ角度を所定の値にする必要がある。ここで
、90″パルスとは、磁気共鳴吸収を起こさせて原子核
のスピンの磁気モーメントを被検体が置かれた静磁場の
方向と平行な方向から垂直に立ち上がるまで90゜回転
させる働きを有するものである。また、180°パルス
とは、磁気共鳴吸収を起こさせて原子核のスピンの磁気
モーメントを被検体が置かれた静磁場の方向と平行な方
向から180@回転させる働きを有するものである。
By the way, in order to detect MR multiplied signals from protons using such a nuclear magnetic resonance phenomenon, an excitation rotating magnetic field generated by a 901' pulse and a high frequency pulse called 180° is used to It is necessary to selectively excite the measurement site so that the angle of inclination of the proton spin magnetic moment at the measurement site is set to a predetermined value. Here, the 90'' pulse has the function of causing magnetic resonance absorption and rotating the magnetic moment of the spin of an atomic nucleus by 90 degrees from a direction parallel to the direction of the static magnetic field in which the subject is placed until it rises perpendicularly. Furthermore, the 180° pulse has the function of causing magnetic resonance absorption and rotating the magnetic moment of the spin of the atomic nucleus by 180@ from a direction parallel to the direction of the static magnetic field in which the subject is placed. .

これらの90’パルスおよび180°パルスは、被測定
部位からのMR倍信号検知に先立ち、パルスの大きさ等
の条件を予め設定する必要がある。しかしながら、この
高周波パルスの条件設定に際しては、被検体の形状等の
属性により電気的な特性であるストレーキャパシティー
Qが変化してしまうために、夫々のスライス位置で90
″パルスまたハ180″ハルスの条件がずれてしまい、
スピンの磁気モーメントの倒れ角度が設定値と異なって
しまう。その結果、得られる信号は被検体の属性により
ばらついてしまう。特に、被測定部位が胸膜部の場合、
呼吸性運動により、胸膜部が体の前後に揺動すると共に
、横隔膜により身長方向に上下動することにより、スラ
イス位置が被測定部位に対して相対的にずれてしまい、
90″パルスまたは180’パルスの条件がずれてしま
い、さらに、データ収集中にスピンの位相変化が生じ、
得られるMR倍信号強度が変化してしまうという問題が
ある。
For these 90' pulses and 180° pulses, it is necessary to set conditions such as the pulse size in advance before detecting the MR multiplied signal from the measurement site. However, when setting the conditions for this high-frequency pulse, the stray capacity Q, which is an electrical characteristic, changes depending on attributes such as the shape of the subject.
``Pulse 180'' Hals conditions are off,
The angle of inclination of the spin magnetic moment differs from the set value. As a result, the obtained signals vary depending on the attributes of the subject. In particular, when the measurement site is the pleura,
Due to respiratory movements, the pleura swings back and forth in the body, and the diaphragm moves up and down in the direction of the body height, causing the slice position to shift relative to the area to be measured.
The conditions for the 90″ pulse or the 180′ pulse are deviated, and furthermore, spin phase changes occur during data collection.
There is a problem in that the obtained MR multiplied signal strength changes.

(発明が解決しようとする課題) 上述したように、核磁気共鳴現象を利用して胸膜部の断
層像を得る場合、被測定部位からのMR倍信号検知する
に先立ち行われる、90°パルスまたは180@パルス
の高周波出力の条件設定は、相対的なスライス位置がず
れてしまうために、90″パルスまたは180”パルス
の条件がずれてしまい、スピンの磁気モーメントの倒れ
角度が設定値と異なってしまい、正確な信号が得られな
いという、問題点がある。
(Problems to be Solved by the Invention) As described above, when obtaining a tomographic image of the pleural region using nuclear magnetic resonance, the 90° pulse or The condition settings for the high-frequency output of the 180@pulse will shift the relative slice position, so the conditions for the 90" or 180" pulse will shift, and the angle of inclination of the magnetic moment of the spin will differ from the set value. There is a problem in that it is difficult to obtain accurate signals.

本発明の目的は、90°パルスまたは180″パルスの
高周波出力の条件設定が正確に行え、正確な信号が得ら
れる高周波出力調整方法を提供することにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide a high-frequency output adjustment method that allows accurate setting of high-frequency output conditions for 90° pulses or 180'' pulses and obtains accurate signals.

[発明の構成コ (課題を解決するための手段) 本発明は、静磁場中に配置された被検者から誘起された
磁気共鳴信号を検出して被検出部位の形態情報または機
能情報を得るに先立ち、励起回転磁場発生に供される送
信パルス電力を被検体の属性に応じて変化させることに
より、スピン系磁気モーメントの倒れ角度を所定の値に
調整する高周波出力調整方法において、スピン系磁気モ
ーメントの倒れ角度を所定の値に調整する時のスライス
厚を最大高周波コイルの均一領域全体を含む様に厚く設
定することを特徴とする高周波出力調整方法である。
[Configuration of the Invention (Means for Solving the Problems) The present invention detects magnetic resonance signals induced from a subject placed in a static magnetic field to obtain morphological information or functional information of a detected region. In a high-frequency output adjustment method that adjusts the inclination angle of the spin-based magnetic moment to a predetermined value by changing the transmitted pulse power used to generate an excitation rotating magnetic field according to the attributes of the subject, This high frequency output adjustment method is characterized in that the slice thickness when adjusting the inclination angle of the moment to a predetermined value is set thick so as to include the entire uniform region of the maximum high frequency coil.

(作 用) 本発明の高周波出力調整方法では、スピン系磁気モーメ
ントの倒れ角度を所定の値に調整する時のスライス厚を
最大高周波コイルの均一領域全体を含む様に厚く設定す
ることにより、高周波出力を設定するためにMR倍信号
得る際に、高周波コイルの感度が均一な領域全体を選択
的に励起して、この領域のみからMR倍信号得るために
、被検査部位が胸膜部の様に、呼吸性運動等によりスラ
イス位置がずれても、磁気共鳴現象を励起する90゜パ
ルスおよび180’パルスの高周波出力調整が正確に行
え、正確な断層像が得られる。
(Function) In the high-frequency output adjustment method of the present invention, the slice thickness when adjusting the inclination angle of the spin-based magnetic moment to a predetermined value is set thick so as to include the entire uniform region of the maximum high-frequency coil. When obtaining the MR multiplied signal to set the output, the high frequency coil is selectively excited in the entire region where the sensitivity is uniform, and in order to obtain the MR multiplied signal only from this region, the area to be examined is made like the pleura. Even if the slice position is shifted due to respiratory motion or the like, the high frequency output of the 90° pulse and 180' pulse that excites the magnetic resonance phenomenon can be adjusted accurately, and an accurate tomographic image can be obtained.

(実施例) 以下、本発明の実施例を図面を参照して説明する。第1
図は、本発明の実施例に用いられる核磁気共鳴イメージ
ング装置の構成を示す模式図である。第1図に示す様に
、この装置(1)は、磁気共鳴信号が誘起された部位の
位置情報を得るための傾斜磁場を発生するための傾斜磁
場発生コイル(2)および回転高周波磁場を放射すると
共に誘起された磁気共鳴信号を検出するための送受信系
である高周波コイル(3)を有する。この傾斜磁場発生
コイル(2)は、被検体(P)の身長方向の軸をZ軸と
し、このZ軸と夫々直交する軸をX軸およびY軸とする
と、これらの軸について傾斜磁場を発生するX軸傾斜磁
場発生コイル(2a)、Y軸傾斜磁場発生コイル(2b
)、Z軸傾斜磁場発生コイル(2C)から構成される。
(Example) Hereinafter, an example of the present invention will be described with reference to the drawings. 1st
The figure is a schematic diagram showing the configuration of a nuclear magnetic resonance imaging apparatus used in an example of the present invention. As shown in Figure 1, this device (1) includes a gradient magnetic field generating coil (2) for generating a gradient magnetic field for obtaining positional information of a site where a magnetic resonance signal is induced, and a rotating high-frequency magnetic field for emitting a magnetic field. It also has a high frequency coil (3) which is a transmission/reception system for detecting the induced magnetic resonance signals. This gradient magnetic field generating coil (2) generates a gradient magnetic field about the Z-axis, which is the axis in the height direction of the subject (P), and the X-axis and Y-axis, which are perpendicular to the Z-axis, respectively. X-axis gradient magnetic field generation coil (2a), Y-axis gradient magnetic field generation coil (2b)
), and a Z-axis gradient magnetic field generating coil (2C).

各傾斜磁場発生コイル(2a)、(2b)、(2C)は
、図示を省略したX軸傾斜磁場、Y軸傾斜磁場およびZ
軸傾斜磁場用の各電源に、夫々接続されて磁場発生用の
電流が供給される。また、高周波コイル(3)は、後述
する様に、被検体(P)の胸膜部の位置に対応した位置
に被検体(P)を挾んで上下に配置されると共に、高周
波パルスを供給する送信器および被測定部位に誘起され
るMR倍信号受信するために受信器に接続されている。
Each gradient magnetic field generating coil (2a), (2b), (2C) generates an X-axis gradient magnetic field, a Y-axis gradient magnetic field, and a Z-axis gradient magnetic field (not shown).
Each power supply for the axial gradient magnetic field is connected to supply a current for generating a magnetic field. Furthermore, as will be described later, the high-frequency coils (3) are placed above and below the subject (P) at positions corresponding to the position of the pleura of the subject (P), and are transmitters that supply high-frequency pulses. The device is connected to a receiver to receive the MR multiplied signal induced in the device and the site to be measured.

さらに、この装置(1)は、各傾斜磁場および90°パ
ルス並びに180°パルスの高周波パルスのパルスシー
ケンスを実施するシーケンサ、並びに各電源、送信器、
受信器およびシーケンサてを制御すると共に検出信号の
信号処理を行うコンピュータシステムをも備える。この
コンピュータシステムで処理された信号はデイスプレィ
等で表示される。この装置(1)は、被検体(P)に対
してZ軸方向に静磁場を発生する静磁場コイル(図示せ
ず)およびこの静磁場コイルに電流を供給する電源(図
示せず)をも備える。
Furthermore, this device (1) includes a sequencer for implementing each gradient magnetic field and a pulse sequence of high-frequency pulses of 90° pulses and 180° pulses, and each power source, transmitter,
It also includes a computer system that controls the receiver and sequencer and performs signal processing of the detected signals. The signals processed by this computer system are displayed on a display or the like. This device (1) also includes a static magnetic field coil (not shown) that generates a static magnetic field in the Z-axis direction toward the subject (P), and a power source (not shown) that supplies current to this static magnetic field coil. Be prepared.

次に、上述の構成を有するイメージング装置を用いて本
実施例の高周波出力調整方法について、説明する。まず
、第2図に示す様に、90″パルスおよび180@パル
スの高周波出力を設定するためのMR倍信号得る際に、
予め、スライス用磁場である2軸傾斜磁場を調整するこ
とにより、第1図に斜線を付して示した領域であるスラ
イス幅Sを最大高周波コイルの感度が均一な領域となる
様にこれまでの調整方法に比べて厚く設定する。この様
な条件の下で、第3図(a)に示すスライス用傾斜磁場
を印加すると共に、第3図(b)に示す様に9011パ
ルスおよび180°パルスを高周波コイルに印加して、
誘起されるMR倍信号検知して、MR倍信号最大となる
様に各パルスの大きさを調整して、スピン系磁気モーメ
ントの倒れ角度が所定の値となる様に、各パルスの条件
を設定する。
Next, the high frequency output adjustment method of this embodiment will be explained using the imaging apparatus having the above-described configuration. First, as shown in Figure 2, when obtaining the MR multiplied signal for setting the high frequency output of 90'' pulse and 180 @ pulse,
By adjusting the two-axis gradient magnetic field, which is the magnetic field for slicing, in advance, the slice width S, which is the shaded area in Figure 1, is adjusted so that the maximum high-frequency coil sensitivity is uniform. Set it thicker than the adjustment method. Under these conditions, the slicing gradient magnetic field shown in FIG. 3(a) was applied, and 9011 pulses and 180° pulses were applied to the high-frequency coil as shown in FIG. 3(b).
Detect the induced MR multiplied signal, adjust the size of each pulse to maximize the MR multiplied signal, and set the conditions for each pulse so that the angle of inclination of the spin-based magnetic moment becomes a predetermined value. do.

この条件の設定に際して、各パルスの条件を自動的に設
定できる回路システムとして、例えば、第4図にブロッ
ク図を示したものが利用できる。
When setting these conditions, for example, the block diagram shown in FIG. 4 can be used as a circuit system that can automatically set the conditions for each pulse.

即ち、この回路システムは、送信パルス制御手段(10
)、送信部(11)および受信部(12)から構成され
る。この送信パルス制御手段(lO)は例えば中央処理
装置などを中心に構成されたものであり、高周波コイル
(3)による励起回転磁場の発生に供される送信パルス
電力を、被検体の属性に応じて変化させることにより、
スピン系磁気モーメントの倒れ角度を所定の値に設定す
るものである。例えば、測定部位に誘起されたMR倍信
号高周波コイルを介して受信しながら、送信パルス電力
を所定の範囲で変化させた際に受信したMR倍信号ピー
ク値が最大となる送信パルス電力値を把握し、この値を
基に被検体の断層像の撮影の際の送信パルス電力を自動
的設定するものである。
That is, this circuit system includes transmission pulse control means (10
), a transmitter (11), and a receiver (12). This transmission pulse control means (lO) is configured mainly of, for example, a central processing unit, and controls the transmission pulse power used for generating the excitation rotating magnetic field by the high-frequency coil (3) according to the attributes of the subject. By changing the
This is to set the angle of inclination of the spin-based magnetic moment to a predetermined value. For example, while receiving the MR multiplied signal induced in the measurement site via a high-frequency coil, while changing the transmitted pulse power within a predetermined range, determine the transmission pulse power value that maximizes the received MR multiplied signal peak value. Based on this value, the transmission pulse power when taking a tomographic image of the subject is automatically set.

また、送信部(11)は各パルスを放射する高周波コイ
ル(3)に接続される。この送信部(11)は連続波を
出力する発振手段(13)、この発振手段(13)より
の連続波を変調する変調手段(14)、この変調手段(
14)において連続波を変調するためのパルス波の振幅
、パルス幅を選択設定する選択手段(15)、送信パル
ス制御手段(lO)の制御によって送信パルス電力を可
変するパワーコントローラ(APC)(1B)、このA
 P C(1B)の出力を夫々増幅する第1の増幅手段
(ラジオ周波アンプ) (17)、第2の増幅手段(駆
動アンプ) (18)、第3の増幅手段(最終アンプ)
’ (19)、インピーダンス整合を行うインピーダン
ス整合手段(20)および高周波コイル(3)との同調
をとる同調手段(21)から構成される。
Further, the transmitter (11) is connected to a high frequency coil (3) that emits each pulse. This transmitter (11) includes an oscillating means (13) for outputting a continuous wave, a modulating means (14) for modulating the continuous wave from the oscillating means (13), and a modulating means (14) for modulating the continuous wave from the oscillating means (13).
14), a selection means (15) for selecting and setting the amplitude and pulse width of the pulse wave for modulating the continuous wave, and a power controller (APC) (1B) for varying the transmission pulse power by controlling the transmission pulse control means (lO). ), this A
A first amplification means (radio frequency amplifier) (17), a second amplification means (drive amplifier) (18), and a third amplification means (final amplifier) that amplify the output of the PC (1B), respectively.
(19), an impedance matching means (20) for performing impedance matching, and a tuning means (21) for tuning with the high frequency coil (3).

さらに、受信部(12)はこのパルスにより誘起された
MR倍信号受信する高周波コイル(3)に接続される。
Further, the receiving section (12) is connected to a high frequency coil (3) that receives the MR multiplied signal induced by this pulse.

高周波パルスの放射とMR倍信号受信とを共通の高周波
コイル(3)で兼用している場合は、送信部(11)と
受信部(12)とをアイソレータ等により分離する必要
がある。また、本実施例の高周波出力調整方法において
は、スライス厚を最大高周波コイルの均一領域全体を含
む様に厚く設定しているために、各パルスの条件設定時
のMR倍信号強度は、撮影時の信号強度に比べて大きく
なる。
When a common high-frequency coil (3) is used for both high-frequency pulse emission and MR multiplied signal reception, it is necessary to separate the transmitting section (11) and receiving section (12) using an isolator or the like. In addition, in the high-frequency output adjustment method of this embodiment, since the slice thickness is set thick so as to include the entire uniform area of the maximum high-frequency coil, the MR multiplied signal intensity at the time of setting the conditions for each pulse is signal strength.

従って、この受信部(12)では、増幅器の利得を下げ
たり、適当な減衰器を設けてMR信号レベルを下げ、適
正なMR倍信号受信することが必要である。例えば、増
幅器の利得を下げるためには、第5図(a)に示す様に
、高周波コイル側の第1段の増幅器(22)の利得を可
変できる様にしておき、出力設定に際してはこの利得を
下げておいたり、また、MR信号レベルを下げるために
は、第5図(b)に示すように、第1段の増幅器(22
)と第2段の増幅器(23)との間に減衰器(24)を
設けることができる。この回路システムの作用について
説明する。被検体の撮影に先立って行われる送信パルス
電力の設定は、オペレータのマニュアル操作によって、
予め、90@パルス条件および180@パルス条件の疎
調整後、送信制御手段(10)からの制御信号に基づき
送信部(11)から高周波コイル(3)に90@パルス
および180°パルスが印加されることにより、高周波
コイル(3〉から被測定部位に励起回転磁場が印加され
る。被測定部位からのMR倍信号高周波コイル(3)を
介して受信部(12)によって受信され、送信パルス制
御手段(10)に入力される。
Therefore, in this receiving section (12), it is necessary to lower the gain of the amplifier or provide an appropriate attenuator to lower the MR signal level to receive an appropriate MR multiplied signal. For example, in order to lower the gain of the amplifier, as shown in Figure 5(a), the gain of the first stage amplifier (22) on the high frequency coil side should be made variable, and when setting the output, this gain should be adjusted. In order to lower the MR signal level or to lower the MR signal level, the first stage amplifier (22
) and the second stage amplifier (23) can be provided with an attenuator (24). The operation of this circuit system will be explained. The transmission pulse power setting, which is performed prior to imaging the subject, is done manually by the operator.
After coarse adjustment of the 90@pulse condition and the 180@pulse condition in advance, a 90@pulse and a 180° pulse are applied from the transmitter (11) to the high frequency coil (3) based on a control signal from the transmission control means (10). By doing so, an excitation rotating magnetic field is applied from the high-frequency coil (3) to the measurement site.The MR multiplied signal from the measurement site is received by the reception unit (12) via the high-frequency coil (3), and the transmission pulse is controlled. It is input into means (10).

送信パルス制御手段(lO)は、入力されたMR倍信号
ピーク値を保持する。この後、A P C(1B)内の
減衰器を可変して送信パルス電力を変えて、上述と同様
に異なる送信パルス電力におけるMR倍信号受信して、
MR倍信号ピーク値を保持する。
The transmission pulse control means (lO) holds the input MR multiplied signal peak value. After this, the attenuator in APC (1B) is varied to change the transmission pulse power, and the MR multiplied signal at different transmission pulse powers is received in the same way as described above.
Holds the MR multiplied signal peak value.

この様に送信パルス電力を変えて収集された複数のMR
倍信号基に、送信パルス制御手段(10)はMR倍信号
ピーク値が最大となる時の送信パルス電力、即ち、A 
P C(1B)内の減衰器の制御状態を認識する。これ
により、被検体の属性に応じた送信パルス電力が設定さ
れる。換言すれば、90°パルスおよび180’パルス
の条件が被検体の属性に応じて適格に設定され、スピン
系磁気モーメントの倒れ角度が90°および180°の
所定値に調整される。
Multiple MRs collected by changing the transmission pulse power in this way
Based on the multiplication signal, the transmission pulse control means (10) controls the transmission pulse power when the MR multiplication signal peak value is maximum, that is, A
Recognize the control state of the attenuator in PC(1B). Thereby, the transmission pulse power is set according to the attributes of the subject. In other words, the conditions for the 90° pulse and the 180' pulse are appropriately set according to the attributes of the subject, and the inclination angles of the spin-based magnetic moments are adjusted to predetermined values of 90° and 180°.

しかも、本実施例の場合、さらに、スライス幅を最大高
周波コイルの感度・均一領域を含む様に厚くするので、
受信されるMR倍信号強度が大きくなり、胸腹部の様に
呼吸性運動により、相対的なスライス位置の変化が、ス
ライス厚より小さくなり、MR倍信号強度の変化が小さ
くなるので、より正確に各パルス条件が設定できる。
Moreover, in the case of this embodiment, the slice width is further increased to include the maximum sensitivity/uniform area of the high frequency coil.
The received MR double signal intensity increases, and due to respiratory movements such as the thoracoabdominal region, the change in relative slice position becomes smaller than the slice thickness, and the change in MR double signal intensity becomes smaller, making it more accurate. Each pulse condition can be set.

上記実施例において、送信パルス電力を変化させる時、
パワーコントローラー(APC)(1B)を使用したが
、パルス波の振幅、パルス幅を選択設定する選択手段(
15)を用いて、振幅を変化させて送信パルス電力を変
化させる等の種々の変形は行える。
In the above embodiment, when changing the transmission pulse power,
Although a power controller (APC) (1B) was used, there is no selection means (for selecting and setting the amplitude and pulse width of the pulse wave).
15), various modifications such as changing the amplitude and changing the transmission pulse power can be performed.

また、送信パルスを流す高周波コイルの特性(均一領域
の大きさ、回転磁場発生の効率等)および疎調整後の9
0°パルス、180@パルスの送信パルス電力値等、さ
らに受信部(12)での増幅器の利得および減衰器の減
衰量等をコンピユーjシステム等に予め保持させておく
ことも行える。
In addition, the characteristics of the high-frequency coil that sends the transmission pulse (size of uniform region, efficiency of rotating magnetic field generation, etc.) and the 9
The transmission pulse power values of 0° pulse and 180@pulse, etc., as well as the gain of the amplifier and the amount of attenuation of the attenuator in the receiving section (12), etc. can be stored in advance in the computer j system or the like.

また、上記実施例では、90’パルス−180°パルス
系列によって生じるMR倍信号最大値を利用したが、t
aO°パルスのみを使用した場合に得られるMR倍信号
最小値を利用する方法等も行える。
Further, in the above embodiment, the maximum value of the MR multiplied signal generated by the 90' pulse-180° pulse sequence was used, but t
A method using the minimum value of the MR multiplied signal obtained when only the aO° pulse is used can also be used.

[発明の効果] 以上の様に、本発明によれば、90″パルスまたは18
0”パルスの高周波出力の条件設定が正確に行え、正確
な信号が得られる高周波出力調整方法を提供することが
できる。
[Effects of the Invention] As described above, according to the present invention, 90″ pulse or 18″ pulse
It is possible to provide a high frequency output adjustment method that can accurately set the conditions for high frequency output of 0'' pulses and obtain accurate signals.

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

第1図は本発明の実施例に用いられる磁気共鳴イメージ
ング装置の構成を示す模式図、第2図は本発明の詳細な
説明するための特性図、第3図(a)は本実施例におけ
るスライス用傾斜磁場を示すグラフ、第3図(b)は本
実施例におけるパルスシーケンスを示すグラフ、第4図
は本実施例に用いられるシステム回路を示すブロック図
、第5図(a)および第5図(b)は本実施例に用いら
れる回路における受信部の主要部を示す回路図である。 l・・・磁気共鳴イメージング装置、 2・・・傾斜磁場発生コイル、 3・・・高周波コイル lO・・・送信パルス制御手段 11・・・送信手段、 12・・・受信手段
FIG. 1 is a schematic diagram showing the configuration of a magnetic resonance imaging apparatus used in an embodiment of the present invention, FIG. 2 is a characteristic diagram for explaining the present invention in detail, and FIG. FIG. 3(b) is a graph showing the gradient magnetic field for slicing, FIG. 3(b) is a graph showing the pulse sequence in this example, FIG. 4 is a block diagram showing the system circuit used in this example, FIG. 5(a) and FIG. FIG. 5(b) is a circuit diagram showing the main parts of the receiving section in the circuit used in this embodiment. l...Magnetic resonance imaging device, 2...Gradient magnetic field generation coil, 3...High frequency coil lO...Transmission pulse control means 11...Transmission means, 12...Reception means

Claims (1)

【特許請求の範囲】[Claims] 静磁場中に配置された被検者から誘起された磁気共鳴信
号を検出して被検出部位の形態情報または機能情報を得
るに先立ち、励起回転磁場発生に供される送信パルス電
力を被検体の属性に応じて変化させることにより、スピ
ン系磁気モーメントの倒れ角度を所定の値に調整する高
周波出力調整方法において、スピン系磁気モーメントの
倒れ角度を所定の値に調整する時のスライス厚を最大高
周波コイルの均一領域全体を含む厚さに設定することを
特徴とする高周波出力調整方法。
Prior to detecting magnetic resonance signals induced from a subject placed in a static magnetic field to obtain morphological or functional information of the detected region, transmit pulse power used to generate an excitation rotating magnetic field is applied to the subject. In a high-frequency output adjustment method that adjusts the inclination angle of the spin-based magnetic moment to a predetermined value by changing it according to the attribute, the slice thickness when adjusting the inclination angle of the spin-based magnetic moment to a predetermined value is set to the maximum high-frequency A high frequency output adjustment method characterized by setting the thickness to include the entire uniform area of a coil.
JP1029330A 1989-02-08 1989-02-08 High frequency output adjustment method Granted JPH02209130A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1029330A JPH02209130A (en) 1989-02-08 1989-02-08 High frequency output adjustment method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1029330A JPH02209130A (en) 1989-02-08 1989-02-08 High frequency output adjustment method

Publications (2)

Publication Number Publication Date
JPH02209130A true JPH02209130A (en) 1990-08-20
JPH0572812B2 JPH0572812B2 (en) 1993-10-13

Family

ID=12273220

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1029330A Granted JPH02209130A (en) 1989-02-08 1989-02-08 High frequency output adjustment method

Country Status (1)

Country Link
JP (1) JPH02209130A (en)

Also Published As

Publication number Publication date
JPH0572812B2 (en) 1993-10-13

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