JPH0243495B2 - - Google Patents
Info
- Publication number
- JPH0243495B2 JPH0243495B2 JP57233515A JP23351582A JPH0243495B2 JP H0243495 B2 JPH0243495 B2 JP H0243495B2 JP 57233515 A JP57233515 A JP 57233515A JP 23351582 A JP23351582 A JP 23351582A JP H0243495 B2 JPH0243495 B2 JP H0243495B2
- Authority
- JP
- Japan
- Prior art keywords
- reception
- magnetic resonance
- control voltage
- voltage
- signal
- 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
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Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R33/00—Arrangements or instruments for measuring magnetic variables
- G01R33/20—Arrangements or instruments for measuring magnetic variables involving magnetic resonance
- G01R33/28—Details of apparatus provided for in groups G01R33/44 - G01R33/64
- G01R33/32—Excitation or detection systems, e.g. using radio frequency signals
- G01R33/36—Electrical details, e.g. matching or coupling of the coil to the receiver
- G01R33/3628—Tuning/matching of the transmit/receive coil
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N24/00—Investigating or analyzing materials by the use of nuclear magnetic resonance, electron paramagnetic resonance or other spin effects
- G01N24/08—Investigating or analyzing materials by the use of nuclear magnetic resonance, electron paramagnetic resonance or other spin effects by using nuclear magnetic resonance
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- Physics & Mathematics (AREA)
- High Energy & Nuclear Physics (AREA)
- General Physics & Mathematics (AREA)
- Chemical & Material Sciences (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Magnetic Resonance Imaging Apparatus (AREA)
Description
【発明の詳細な説明】
[発明の技術分野]
本発明は、磁気共鳴(以下「MR」と称する)
現象を用いて、生体である被検体中に存在するあ
る特定の原子核のスピン密度あるいは、緩和時定
数等の反映された画像を得る磁気共鳴イメージン
グ装置に関するものである。[Detailed Description of the Invention] [Technical Field of the Invention] The present invention relates to magnetic resonance (hereinafter referred to as "MR")
The present invention relates to a magnetic resonance imaging apparatus that uses phenomena to obtain images that reflect the spin density, relaxation time constant, etc. of a specific atomic nucleus present in a living subject.
[発明の技術的背景]
この種の磁気共鳴イメージング装置において、
MR現象により被検体より誘起される信号(これ
をMR信号と呼ぶ)を検出する部分は、被検体の
周囲に設置される鞍型のコイルおよび、これとと
もに共振回路を構成するコンデンサにより構成さ
れる。MR信号は非常に微弱であるため、信号を
効率良く検出するには、Q(クオリテイフアクタ)
の非常に大きな共振回路を必要とする。このため
上記共振回路の共振特性は、鋭くなる。従つて、
共振回路の容量成分のわずかな変化で、検出され
る信号の振幅、すなわち、検出器の感度が大きく
変化する。一方、被検体と検出コイルとの間には
浮遊容量が存在し、これは、被検体により異るた
め、被検体が変わる毎に上記コンデンサの静電容
量を変化させ、共振点に正確に同調させる必要が
ある。[Technical background of the invention] In this type of magnetic resonance imaging apparatus,
The part that detects the signal induced from the subject by the MR phenomenon (this is called an MR signal) consists of a saddle-shaped coil installed around the subject and a capacitor that together forms a resonant circuit. . Since the MR signal is very weak, in order to detect the signal efficiently, Q (Quality Actor) is required.
requires a very large resonant circuit. Therefore, the resonance characteristics of the above-mentioned resonance circuit become sharp. Therefore,
A slight change in the capacitance component of the resonant circuit significantly changes the amplitude of the detected signal, that is, the sensitivity of the detector. On the other hand, there is stray capacitance between the test object and the detection coil, and this varies depending on the test object, so the capacitance of the capacitor is changed each time the test object changes, and the capacitance is precisely tuned to the resonance point. It is necessary to do so.
[発明の目的]
本発明の目的とするところは、NMR信号収集
に際し自動的に検出部の同調をとることを可能と
する磁気共鳴イメージング装置を提供することに
ある。[Object of the Invention] An object of the present invention is to provide a magnetic resonance imaging apparatus that makes it possible to automatically tune a detection unit when collecting NMR signals.
[発明の概要]
本発明は、共振回路を、受信コイルと外部から
与えられる制御電圧により容量値が設定される可
変容量要素を含む受信同調手段とで構成し、前記
可変容量要素にその容量を制御するための電圧を
供給する制御電圧発生手段と、共鳴周波数の連続
波を疑似受信信号として上記受信同調手段に印加
する連続波印加手段と、上記受信同調手段の出力
を包絡線検波する包絡線検波手段と、この包絡線
検波手段の出力が入出されこの信号入力に基づい
て上記制御電圧発生手段を制御し上記受信同調手
段の同調制御を行なう手段とを備えたことを特徴
としている。[Summary of the Invention] The present invention comprises a resonant circuit including a receiving coil and a receiving tuning means including a variable capacitance element whose capacitance value is set by a control voltage applied from the outside, and in which the capacitance is set to the variable capacitance element. control voltage generation means for supplying a voltage for control; continuous wave application means for applying a continuous wave at a resonant frequency to the reception tuning means as a pseudo reception signal; and an envelope for envelope detection of the output of the reception tuning means. The present invention is characterized in that it comprises a detection means, and a means into which the output of the envelope detection means is input/output and which controls the control voltage generation means based on the signal input and performs tuning control of the reception tuning means.
[発明の実施例]
第1図に本発明の一実施例におけるシステム全
体の構成を示す。[Embodiment of the Invention] FIG. 1 shows the configuration of the entire system in an embodiment of the present invention.
第1図において、1は送信コイルからなる送信
プローブヘツド、2は受信コイルからなる受信プ
ローブヘツドであり、これら送、受信プローブヘ
ツド1,2は図示のように鞍形の送受信コイルが
互いに直交する方向に配置された形のクロスコイ
ル方式のプローブヘツドを構成している。 In FIG. 1, 1 is a transmitting probe head consisting of a transmitting coil, and 2 is a receiving probe head consisting of a receiving coil. In these transmitting and receiving probe heads 1 and 2, saddle-shaped transmitting and receiving coils are orthogonal to each other as shown in the figure. It constitutes a cross-coil type probe head arranged in the direction.
尚、図示してないが、静磁場磁石や、傾斜磁場
コイルが備つており、これら静磁場磁石による静
磁場、傾斜磁場コイル及びその制御系によるMR
信号の位置情報を付与するための線型傾斜磁場、
プローブヘツド1,2による高周波励起パルス
(高周波磁場)がそれぞれ被検体に印加されるこ
とにより、特定の部位にMR現象が生じるように
なつている。 Although not shown, there are static magnetic field magnets and gradient magnetic field coils.
linear gradient magnetic field for imparting signal position information;
By applying high-frequency excitation pulses (high-frequency magnetic fields) from the probe heads 1 and 2 to the subject, an MR phenomenon occurs in a specific region.
上述した各磁場発生要素は、良く知られている
ように、医用診断用の磁気共鳴装置、つまり、こ
の種の磁気共鳴イメージング装置には、一般に備
つている要素である。送信同調部3は特定周波数
の高周波に同調し、送信部4の出力に応動して被
検体中の特定原子核に同調するような高周波励起
パルスを送信プローブヘツド1を介して電磁波と
して被検体に印加する。 As is well known, each of the magnetic field generating elements described above is an element generally included in a magnetic resonance apparatus for medical diagnosis, that is, this type of magnetic resonance imaging apparatus. The transmission tuning section 3 tunes to a high frequency of a specific frequency, and in response to the output of the transmitting section 4 applies a high frequency excitation pulse that tunes to a specific atomic nucleus in the subject through the transmission probe head 1 as an electromagnetic wave to the subject. do.
また、傾斜磁場コイル及びプローブヘツド1,
2は、パルスシーケンスと称されるイメージング
手順に従つて駆動される。そして、このパルスシ
ーケンスは、後述する計算機13に装備されてい
る。送信部4は、上記特定周波数すなわち共鳴周
波数の連続波を発生する発振器41、この発振器
41の出力をもとに励起パルスを作る変調器42
およびこの変調器42の出力を増幅する電力増幅
器43で構成されている。被検体におけるMR信
号は受信プローブヘツド2を介して受信同調部5
で受信し前置増幅器6で増幅し切換器7を介して
2個の位相検波器8A,8Bに与える。これら位
相検波器8A,8Bには、送信部4の発振器41
で発生した信号をもとに移相器9、90゜移相器1
0で生成した、MR信号と同じ周波数を有し且つ
位相が互いに90゜異なる2種の参照波が与えられ
る。位相検波器8A,8Bは受信したMR信号を
上記参照波でそれぞれ位相検波し、検波出力は増
幅器11A,11Bで各別に増幅し、各々ローパ
スフイルタ12A,12Bを介してA/D(アナ
ログ−デイジタル)変換器13A,13Bでデイ
ジタル化し計算機14に入力している。計算機1
4内では上記デイジタル化された2信号を用いて
所定の位相補正処理を行ないNMRエコー信号デ
ータとする。D/A(デイジタル−アナログ)変
換器15は計算機14の出力に応じた制御電圧vc
を受信調部5に与える制御電圧発生器を構成して
いる。抵抗16は送信部4の発振器41から出力
される共鳴周波数の連続波を切換器17を介して
導出し受信同調部5に供給する回路を構成してい
る。増幅器18は切換器7を介して前置増幅器6
からの信号を受け、これを増幅する。この増幅器
18で増幅した信号は包絡線検波器19で包絡線
検波しA/D変換器20でデイジタル化して計算
機14に入力する。切換器7および17は計算機
14により制御されて本構成の動作モードを切換
えるもので、同調制御時には、切換器7は前置増
幅器6の出力を増幅器18に与え、切換器17は
オンとなり、MR信号収集時には、前置増幅器6
の出力を位相検波器8A,8Bに与え、切換器7
はオフとなる。なお、送信部の発振器41および
変調器42もそれぞれ所要の動作をさせるべく計
算機14により制御される。 In addition, a gradient magnetic field coil and a probe head 1,
2 is driven according to an imaging procedure called a pulse sequence. This pulse sequence is installed in a computer 13, which will be described later. The transmitter 4 includes an oscillator 41 that generates a continuous wave at the specific frequency, that is, a resonance frequency, and a modulator 42 that generates an excitation pulse based on the output of the oscillator 41.
and a power amplifier 43 that amplifies the output of this modulator 42. The MR signal from the subject is transmitted to the reception tuning section 5 via the reception probe head 2.
The signal is received by a preamplifier 6, amplified by a preamplifier 6, and applied to two phase detectors 8A and 8B via a switch 7. These phase detectors 8A and 8B include an oscillator 41 of the transmitter 4.
Based on the signal generated by phase shifter 9, 90° phase shifter 1
Two types of reference waves generated at 0 and having the same frequency as the MR signal and having phases different from each other by 90° are provided. Phase detectors 8A and 8B phase-detect the received MR signal using the reference wave, and the detected outputs are amplified separately by amplifiers 11A and 11B, and converted into A/D (analog-digital) signal via low-pass filters 12A and 12B, respectively. ) The data is digitized by converters 13A and 13B and input to the computer 14. calculator 1
4, the two digitized signals are subjected to a predetermined phase correction process to obtain NMR echo signal data. A D/A (digital-analog) converter 15 outputs a control voltage v c according to the output of the computer 14.
This constitutes a control voltage generator that provides the reception tuning section 5 with the following. The resistor 16 constitutes a circuit that derives a continuous wave of the resonant frequency output from the oscillator 41 of the transmitting section 4 via the switch 17 and supplies it to the reception tuning section 5. The amplifier 18 is connected to the preamplifier 6 via the switch 7.
receives the signal from and amplifies it. The signal amplified by the amplifier 18 undergoes envelope detection by an envelope detector 19, is digitized by an A/D converter 20, and is input to the computer 14. Switches 7 and 17 are controlled by computer 14 to switch the operating mode of this configuration. During tuning control, switch 7 gives the output of preamplifier 6 to amplifier 18, switch 17 is turned on, and MR During signal acquisition, the preamplifier 6
The output of is given to phase detectors 8A and 8B, and
is off. It should be noted that the oscillator 41 and modulator 42 of the transmitting section are also controlled by the computer 14 so as to operate as required.
第2図は上述の構成における受信同調部5およ
びその周辺の部分を詳細に示すものである。 FIG. 2 shows in detail the reception tuning section 5 and its surrounding parts in the above-described configuration.
第2図において、逆方向印加電圧によりその静
電容量が変化する可変容量ダイオード51とこの
可変容量ダイオード51のカソード側に直列に設
けた大容量のコンデンサ52とで形成される直列
回路を図示のように受信プローブヘツド(コイ
ル)2に並列に設けてLCの並列共振回路を構成
する。ここで、コンデンサ52の静電容量は可変
容量ダイオード51のそれに比べて充分に大きく
設定し、両者の直列合成容量はほとんど可変容量
ダイオード51で決定されるようにする。この場
合、可変容量ダイオード51とコンデンサ52の
直列回路は可変容量ダイオード51のアノード側
を接地側として接続するものとしたが、この直列
回路を図示とは逆向きとしてコンデンサ52側を
接地側としてもよい。上記並列回路にさらに並列
に互いに逆並列接続した一対のダイオードからな
る逆並列ダイオード(「交叉ダイオード」と呼ば
れることもある)53を設ける。また、可変容量
ダイオード51とコンデンサ52の接続点は抵抗
54を介してD/A変換器14の出力側に接続さ
れ、D/A変換器14からの制御電圧vcが与えら
れる。抵抗54としては高周波の受信MR信号等
がD/A変換器6側へ流入するのを阻止するため
抵抗値の高いものを使用する。また、図示の場合
コンデンサ52により信号線はD/A変換器14
と直流的にしや断される。また、逆並列ダイオー
ド53は送信側から被検体に印加される大電力の
高周波励起パルスの受信側へのもれによる前置増
幅器6の入力部の破壊および可変容量ダイオード
51より発生する歪を防ぐものである。これら可
変容量ダイオード51、コンデンサ52、逆並列
ダイオード53、抵抗54により受信同調部5を
構成している。可変容量ダイオード51に印加す
る制御電圧vcはD/A変換器14より与えるが、
この電圧の調整設定は次のようにして行なう。 In FIG. 2, a series circuit formed by a variable capacitance diode 51 whose capacitance changes depending on a voltage applied in the reverse direction and a large capacitance capacitor 52 provided in series on the cathode side of this variable capacitance diode 51 is shown. The probe is connected in parallel to the receiving probe head (coil) 2 to form an LC parallel resonant circuit. Here, the capacitance of the capacitor 52 is set to be sufficiently larger than that of the variable capacitance diode 51, so that the series combined capacitance of both is almost determined by the variable capacitance diode 51. In this case, the series circuit of the variable capacitance diode 51 and the capacitor 52 was connected with the anode side of the variable capacitance diode 51 as the ground side, but this series circuit could also be connected in the opposite direction to the illustration, with the capacitor 52 side as the ground side. good. The parallel circuit is further provided with an anti-parallel diode (sometimes referred to as a "crossing diode") 53 consisting of a pair of diodes connected in anti-parallel to each other. Further, a connection point between the variable capacitance diode 51 and the capacitor 52 is connected to the output side of the D/A converter 14 via a resistor 54, and a control voltage v c from the D/A converter 14 is applied thereto. As the resistor 54, a resistor with a high resistance value is used to prevent high frequency received MR signals etc. from flowing into the D/A converter 6 side. In addition, in the case shown in the figure, the signal line is connected to the D/A converter 14 by the capacitor 52.
and is cut off by direct current. In addition, the anti-parallel diode 53 prevents damage to the input section of the preamplifier 6 due to leakage of high-power high-frequency excitation pulses applied to the subject from the transmitting side to the receiving side, and prevents distortion caused by the variable capacitance diode 51. It is something. The variable capacitance diode 51, the capacitor 52, the anti-parallel diode 53, and the resistor 54 constitute the reception tuning section 5. The control voltage v c applied to the variable capacitance diode 51 is given from the D/A converter 14,
This voltage adjustment setting is performed as follows.
まず、被検体を送受信プローブヘツド1,2内
においた状態で、切換器7,17を同調制御モー
ドすなわち図示のような接続とする。この状態に
おいて受信プローブヘツド2は送信部4の発振器
41に接続されており、電力増幅器43によつて
増幅される以前の低電圧の共鳴周波数の連続波が
受信プローブヘツド(コイル)2に印加される。
ここで抵抗16の抵抗値が充分に大きいものとす
ると、第3図a,bに示す等価回路のように検出
部の共振回路(可変容量ダイオード51とコンデ
ンサ52の直列回路を可変容量CVとする。)に、
共鳴周波数の電流源ISが接続されたものと等価に
なる。共振回路の端子間に生ずる電圧は、切換器
7により増幅器18に与えられ、増幅された電圧
は包絡線検波器19に与えられる。この検波器1
9は、ダイオードによる包絡線検波器等を用いて
構成され、入力された共鳴周波数の信号の包絡線
成分すなわち入力信号の振幅に比例した直流電圧
を出力として得るものである。この直流電圧は
A/D変換器20によりデイジタル量に変換され
計算機14に入力される。当初は、D/A変換器
15の出力電圧vcは予め定めた制御範囲の最小値
V0に設定しておく。受信同調部6の共振回路に
生ずる電圧は増幅、検波され、A/D変換器13
A,13Bを通して計算機14に入力される。こ
の電圧値をP0とし、これを計算機14内の記憶
装置に記録する。この電圧P0は、可変容量ダイ
オード51の制御電圧vcをV0とした時の共振回
路に生ずる電圧の振幅に対応する。次にD/A変
換器15の出力制御電圧vcをV1=V0+ΔV(V←
V0+ΔV)として、上述と同様にして検波出力電
圧を記録し、その値をP1とする。さらに順次V2
=V1+ΔV…Vo=Vo-1+ΔVのように制御電圧を
増加しその時の検波出力電圧をP2…Poとする。 First, with the subject placed in the transmitting/receiving probe heads 1 and 2, the switching devices 7 and 17 are set to the tuning control mode, that is, connected as shown. In this state, the receiving probe head 2 is connected to the oscillator 41 of the transmitting section 4, and a low voltage continuous wave at a resonant frequency before being amplified by the power amplifier 43 is applied to the receiving probe head (coil) 2. Ru.
Here, assuming that the resistance value of the resistor 16 is sufficiently large, the resonant circuit of the detection section (the series circuit of the variable capacitance diode 51 and the capacitor 52 is defined as the variable capacitance CV) as shown in the equivalent circuit shown in FIGS. 3a and 3b. ),
This is equivalent to connecting a current source IS at the resonant frequency. The voltage generated between the terminals of the resonant circuit is applied to the amplifier 18 by the switch 7, and the amplified voltage is applied to the envelope detector 19. This detector 1
Reference numeral 9 is constructed using an envelope detector using a diode, etc., and outputs a DC voltage proportional to the envelope component of the input signal at the resonant frequency, that is, the amplitude of the input signal. This DC voltage is converted into a digital quantity by the A/D converter 20 and input to the computer 14. Initially, the output voltage v c of the D/A converter 15 is the minimum value of the predetermined control range.
Set it to V 0 . The voltage generated in the resonant circuit of the reception tuning section 6 is amplified and detected, and then sent to the A/D converter 13.
It is input to the computer 14 through A and 13B. This voltage value is set as P 0 and is recorded in the storage device within the computer 14. This voltage P 0 corresponds to the amplitude of the voltage generated in the resonant circuit when the control voltage v c of the variable capacitance diode 51 is set to V 0 . Next, the output control voltage v c of the D/A converter 15 is set as V 1 =V 0 +ΔV(V←
V 0 +ΔV), record the detected output voltage in the same manner as described above, and set the value as P 1 . Further sequentially V 2
=V 1 +ΔV…V o =V o-1 The control voltage is increased as +ΔV, and the detected output voltage at that time is P 2 …P o .
ここで最初の制御電圧vc=V0が充分に小さけ
れば、これは可変容量ダイオード51の静電容量
を受信同調部5の共振条件を満足する値とするた
めの制御電圧(得ようとする制御電圧)vc=VR
よりも小さく、制御電圧vcを増加させることによ
り、共振条件に近づき、検波出力は共鳴点に達す
るまで単調増加する。制御電圧vc=Vnを印加し
て検波出力Pnを得た時、これを1つ前の検波出
力Pn-1と比較しPn>Pn-1であるかぎり制御電圧
vcをΔV増加させるという操作を繰り返しPk<
Pk-1となるまで続ける。この時検波出力Pk-1に対
応する制御電圧vc=Vk-1が、同調部の共振条件を
与える値であり、これを固定化する。 Here, if the first control voltage v c =V 0 is sufficiently small, this is the control voltage (to be obtained control voltage) v c = V R
By increasing the control voltage v c , the resonance condition is approached, and the detection output increases monotonically until reaching the resonance point. When the control voltage v c = V n is applied and the detection output P n is obtained, this is compared with the previous detection output P n-1, and as long as P n > P n-1, the control voltage is
Repeating the operation of increasing v c by ΔV until P k <
Continue until P k-1 . At this time, the control voltage v c =V k-1 corresponding to the detected output P k-1 is a value that provides the resonance condition of the tuning section, and is fixed.
次に、撮影のためのパルスシーケンスの実行に
より、MR断層画像を得るための信号収集をする
ために切換器7,17をMR信号収集モードに切
換える。すなわち切換器17は開放され、前置増
幅器6の出力は位相検波器8A,8B以下の受信
系回路に接続される。このとき、可変容量ダイオ
ード51には、上述の操作で決定した制御電圧を
与えておく。つまり、制御電圧vcを固定化してお
く。この状態で送信プローブヘツド1に高周波励
起パルスを印加し、NMR信号の収集を行なう。
以上の操作を、被検体が変わるたびに行うごとに
より、受信同調部5の同調は常に維持される。 Next, by executing a pulse sequence for imaging, the switchers 7 and 17 are switched to MR signal acquisition mode in order to acquire signals for obtaining an MR tomographic image. That is, the switch 17 is opened, and the output of the preamplifier 6 is connected to the receiving system circuits below the phase detectors 8A and 8B. At this time, the control voltage determined by the above operation is applied to the variable capacitance diode 51. In other words, the control voltage v c is fixed. In this state, a high frequency excitation pulse is applied to the transmitting probe head 1 to collect NMR signals.
By performing the above operation every time the subject changes, the tuning of the reception tuning section 5 is always maintained.
尚、撮影のためのパルスシーケンスにおいて
は、送信系と、傾斜磁場コイル及びその制御系と
が起動される。前述したように、撮影に先立つて
行われるチユーニング時にあつては、送信系のみ
が起動され且つ励起パルスを被検体に印加しない
で、単に疑似受信信号を生成し、これを受信同調
部5に与えるものとしている。しかも、制御電圧
を変えながら、その1回に前記疑似受信信号は連
続波として受信同調部5に連続的に与えられるこ
とにより、単時間にて、同調条件を与える制御電
圧vcを見つけだすことができる。 In addition, in the pulse sequence for imaging, the transmission system, the gradient magnetic field coil, and its control system are activated. As mentioned above, during tuning performed prior to imaging, only the transmitting system is activated and without applying an excitation pulse to the subject, a pseudo reception signal is simply generated and this is applied to the reception tuning section 5. I take it as a thing. Moreover, by continuously applying the pseudo reception signal as a continuous wave to the reception tuning unit 5 at one time while changing the control voltage, it is possible to find the control voltage v c that provides the tuning condition in a single time. can.
このようにした場合、被検体より得られる
NMR信号を用いて制御を行うのではなく、連続
波を受信プローブヘツド(コイル)2に印加し
て、同調条件を調整設定するため、短時間で、最
適な同調条件が得られる。 When done in this way, the
Rather than performing control using NMR signals, a continuous wave is applied to the receiving probe head (coil) 2 to adjust and set the tuning conditions, so optimal tuning conditions can be obtained in a short time.
なお、本発明は上述し且つ図面に示す実施例に
のみ限定されることなくその要旨を変更しない範
囲内で種々変形して実施することができる。 Note that the present invention is not limited to the embodiments described above and shown in the drawings, but can be implemented with various modifications without changing the gist thereof.
例えば上述の実施例においては、共鳴周波数の
連続波を受信プローブヘツド2に印加するように
したが、上記実施例のようにクロスコイル方式の
場合には、第5図に示すごとく共鳴周波数の信号
を変調器42および電力増幅器43を通さずに切
換器21を介して送信プローブヘツドに印加する
ようにし、受信プローブヘツドに誘導される微少
なもれ電圧を増幅、検波しても上述とほぼ同様に
して同調をとることができる。 For example, in the above embodiment, a continuous wave at the resonant frequency was applied to the receiving probe head 2, but in the case of the cross coil method as in the above embodiment, the continuous wave at the resonant frequency is applied as shown in FIG. Even if the voltage is applied to the transmitting probe head via the switch 21 without passing through the modulator 42 and power amplifier 43, and the minute leakage voltage induced in the receiving probe head is amplified and detected, the result is almost the same as described above. You can synchronize by doing this.
また第2図に示したコンデンサ52に代えても
う1つの可変容量ダイオードを、カソード同士が
接続される方向として直列接続し、同調の微調整
を可能としてもよく、もちろん、先に述べたよう
に第2図の可変容量ダイオード51とコンデンサ
52の直列回路を図示とは逆向きとしてもよい。 Further, instead of the capacitor 52 shown in FIG. 2, another variable capacitance diode may be connected in series with the cathodes connected to each other to enable fine adjustment of the tuning.Of course, as described above, The series circuit of the variable capacitance diode 51 and the capacitor 52 in FIG. 2 may be arranged in the opposite direction from that shown.
さらに、上述の実施例では第1図に示したよう
な鞍型の受信コイルを用いた場合について示した
が、ループコイル型の受信コイルを用いた場合に
おいても上述と全く同様の方式を適用することが
可能である。 Furthermore, although the above-mentioned embodiment shows the case where a saddle-shaped receiving coil as shown in FIG. Is possible.
また同実施例では送信コイル、受信コイルが互
いに直交する形のクロスコイル方式を用いた場合
を示したが、第4図に示すように送信コイル、受
信コイルを1つのコイルで兼ねて送受信プローブ
ヘツド22を構成したシングルコイル方式におい
ても上述とほぼ同様な実施が可能である。第4図
において、23は送信用電力増幅群、24は誤動
作防止用の逆並列ダイオード、25は同調用可変
コンデンサ、26は補助コイルである。 Furthermore, in the same embodiment, a cross-coil method was used in which the transmitting coil and the receiving coil were perpendicular to each other, but as shown in FIG. Almost the same implementation as described above is also possible in a single coil system in which 22 is configured. In FIG. 4, 23 is a power amplifier group for transmission, 24 is an anti-parallel diode for preventing malfunction, 25 is a variable capacitor for tuning, and 26 is an auxiliary coil.
[発明の効果]
本発明によれば、MR信号収集に際し自動的に
且つすみやかに検出部の同調をとることの可能な
磁気共鳴イメージング装置を提供することができ
る。[Effects of the Invention] According to the present invention, it is possible to provide a magnetic resonance imaging apparatus that can automatically and quickly synchronize a detection unit when collecting MR signals.
第1図は本発明の一実施例の全体構成を示すブ
ロツク図、第2図は同実施例の要部構成を示す回
路構成図、第3図a,bは同実施例の作用を説明
するための等価回路図、第4図および第5図は本
発明のそれぞれ異なる他の実施例の構成を示す回
路図およびブロツク図である。
1……送信プローブヘツド、2……受信プロー
ブヘツド、3……送信同調部、4……送信部、5
……受信同調部、6……前置増幅器、7,17,
21……切換器、8A,8B……位相検波器、9
……移相器、10……90゜移相器、11A,11
B,18……増幅器、12A,12B……ローパ
スフイルタ、13A,13B,20……A/D変
換器、14……計算機、15……D/A変換器、
16……抵抗、19……包絡線検波器、22……
送受信プローブヘツド、23,43……電力増幅
器、24,53……逆並列ダイオード(交叉ダイ
オード)、25……可変コンデンサ、26……補
助コイル、41……発振器、42……変調器、5
1……可変容量ダイオード、52……コンデン
サ、54……抵抗。
Fig. 1 is a block diagram showing the overall configuration of an embodiment of the present invention, Fig. 2 is a circuit diagram showing the main structure of the embodiment, and Figs. 3 a and b explain the operation of the embodiment. FIGS. 4 and 5 are circuit diagrams and block diagrams showing the configurations of other different embodiments of the present invention, respectively. DESCRIPTION OF SYMBOLS 1...Transmission probe head, 2...Reception probe head, 3...Transmission tuning section, 4...Transmission section, 5
... Reception tuning section, 6 ... Preamplifier, 7, 17,
21...Switcher, 8A, 8B...Phase detector, 9
...Phase shifter, 10...90° phase shifter, 11A, 11
B, 18...Amplifier, 12A, 12B...Low pass filter, 13A, 13B, 20...A/D converter, 14...Computer, 15...D/A converter,
16...Resistor, 19...Envelope detector, 22...
Transmission/reception probe head, 23, 43... Power amplifier, 24, 53... Anti-parallel diode (crossing diode), 25... Variable capacitor, 26... Auxiliary coil, 41... Oscillator, 42... Modulator, 5
1... Variable capacitance diode, 52... Capacitor, 54... Resistor.
Claims (1)
れる磁気共鳴信号を用いて前記被検体中の特定原
子核のスピン密度及び緩和時定数の少なくとも一
方が反映された画像をイメージングする磁気共鳴
イメージング装置において、高周波励起パルスを
前記被検体に印加する送信系と、前記磁気共鳴信
号を受信する受信コイルと、この受信コイルと共
に共振回路を形成するものであつて外部から与え
られる制御電圧値に応じてその静電容量値が設定
される可変容量要素を含む受信同調手段と、前記
受信コイル及び前記受信同調手段を介して得られ
る磁気共鳴信号を用いて画像を生成するイメージ
ング処理手段と、チユーニングのため前記送信系
から生成される特定原子核の共鳴周波数を有する
連続波を疑似受信信号として前記受信同調手段に
入力する連続波印加手段と、予め定めた初期値
V0から始り経時的に増加分ΔVを加えた電圧V←
V0+ΔVを前記受信同調手段に対し制御電圧とし
て与える制御電圧発生手段と、前記疑似受信信号
が前記受信同調手段に入力され且つ前記受信同調
手段に対し一つの制御電圧Vが与えられている下
で前記受信同調手段の出力を包絡線検波して直流
電圧を得る包絡線検波手段と、この包絡線検波手
段により得られる直流電圧値を記憶する記憶手段
と、前記制御電圧発生手段を制御することによつ
て制御電圧Vを変えながら前記疑似受信信号を前
記受信同調手段に入力して前記記憶部に記憶され
ている各直流電圧値に基づいて前記直流電圧値の
最大値を判定し該判定のときの前記制御電圧値V
を固定化する制御手段とを具備したことを特徴と
する磁気共鳴イメージング装置。1. In a magnetic resonance imaging apparatus that uses magnetic resonance signals induced from a subject in which a magnetic resonance phenomenon is occurring to image an image in which at least one of the spin density and relaxation time constant of a specific atomic nucleus in the subject is reflected. , a transmission system that applies a high-frequency excitation pulse to the subject, a reception coil that receives the magnetic resonance signal, and a resonant circuit that forms a resonant circuit together with the reception coil. a receiving tuning means including a variable capacitance element in which a capacitance value is set; an imaging processing means for generating an image using a magnetic resonance signal obtained via the receiving coil and the receiving tuning means; continuous wave applying means for inputting a continuous wave having a resonance frequency of a specific atomic nucleus generated from a transmission system to the reception tuning means as a pseudo reception signal; and a predetermined initial value.
Voltage V that starts from V 0 and adds an increase ΔV over time ←
control voltage generation means for supplying V 0 +ΔV as a control voltage to the reception tuning means; an envelope detection means for envelope-detecting the output of the reception tuning means to obtain a DC voltage; a storage means for storing a DC voltage value obtained by the envelope detection means; and controlling the control voltage generation means. inputting the pseudo reception signal to the reception tuning means while changing the control voltage V by the controller, determining the maximum value of the DC voltage value based on each DC voltage value stored in the storage unit; The control voltage value V when
A magnetic resonance imaging apparatus comprising: a control means for immobilizing the magnetic resonance imaging apparatus.
Priority Applications (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57233515A JPS59122938A (en) | 1982-12-28 | 1982-12-28 | Nuclear magnetic resonance apparatus |
| US06/565,539 US4602213A (en) | 1982-12-28 | 1983-12-27 | Automatic tuning circuit for nuclear magnetic resonance apparatus |
| EP83113150A EP0114405B1 (en) | 1982-12-28 | 1983-12-27 | Nuclear magnetic resonance diagnostic apparatus |
| DE8383113150T DE3374813D1 (en) | 1982-12-28 | 1983-12-27 | Nuclear magnetic resonance diagnostic apparatus |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57233515A JPS59122938A (en) | 1982-12-28 | 1982-12-28 | Nuclear magnetic resonance apparatus |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59122938A JPS59122938A (en) | 1984-07-16 |
| JPH0243495B2 true JPH0243495B2 (en) | 1990-09-28 |
Family
ID=16956233
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57233515A Granted JPS59122938A (en) | 1982-12-28 | 1982-12-28 | Nuclear magnetic resonance apparatus |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59122938A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH01155255A (en) * | 1987-12-11 | 1989-06-19 | Jeol Ltd | Tuning device of probe of nuclear magnetic resonance apparatus |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5945097B2 (en) * | 1977-02-08 | 1984-11-02 | 日本電子株式会社 | High frequency circuit of nuclear magnetic resonance apparatus |
-
1982
- 1982-12-28 JP JP57233515A patent/JPS59122938A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59122938A (en) | 1984-07-16 |
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