JPH04338457A - High frequency signal frequency switching system for exciting nuclear magnetic resonance - Google Patents

High frequency signal frequency switching system for exciting nuclear magnetic resonance

Info

Publication number
JPH04338457A
JPH04338457A JP3110150A JP11015091A JPH04338457A JP H04338457 A JPH04338457 A JP H04338457A JP 3110150 A JP3110150 A JP 3110150A JP 11015091 A JP11015091 A JP 11015091A JP H04338457 A JPH04338457 A JP H04338457A
Authority
JP
Japan
Prior art keywords
frequency
magnetic resonance
phase
nuclear magnetic
bit
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.)
Pending
Application number
JP3110150A
Other languages
Japanese (ja)
Inventor
Kazutoshi Higuchi
和俊 樋口
Nobuhiko Aoki
信彦 青木
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.)
Hitachi Instruments Engineering Co Ltd
Hitachi Ltd
Original Assignee
Hitachi Instruments Engineering Co Ltd
Hitachi Ltd
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 Hitachi Instruments Engineering Co Ltd, Hitachi Ltd filed Critical Hitachi Instruments Engineering Co Ltd
Priority to JP3110150A priority Critical patent/JPH04338457A/en
Publication of JPH04338457A publication Critical patent/JPH04338457A/en
Pending legal-status Critical Current

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  • Stabilization Of Oscillater, Synchronisation, Frequency Synthesizers (AREA)
  • Magnetic Resonance Imaging Apparatus (AREA)

Abstract

PURPOSE:To control the frequency and phase of an output wave independently by generating output wave data from the sum of a reference oscillation output and frequency data. CONSTITUTION:An multiplier 3 computes a product of 20 bit reference data of counter 20 and 17 bit frequency data of a frequency data latch 7. A CPU 9 sends 8 bit phase data to a phase data latch 8 and an adder 4 adds the 8 bit phase data of the phase data latch 8 to a high order 8 bit of 12 bit frequency information of the multiplier 3 and the 12 bit frequency phase information is converted to an amplitude value with an ROM table 5. The ROM table 5 outputs sine wave data of one cycle with 12 bit resolutions to a 12 bit address and finally, the 12 bit sine wave data of the ROM table 5 are converted to voltages with a DA converter 6. Thus, the moment of starting counting with the counter 2 gives a phase reference (zero).

Description

【発明の詳細な説明】[Detailed description of the invention]

【0001】0001

【産業上の利用分野】本発明は生体などの被検物体の特
定部位の水素核などの核磁気共鳴物質を選択的に励起し
て得られる核磁気共鳴信号の強度が、生体内部の部位に
よる核磁気共鳴物質の濃度や性質の違いによって異なる
のを利用して、二次元あるいは三次元的な生体内部の核
磁気共鳴信号強度像あるいは特定部位の共鳴スペクトル
を計測する検査装置に係り、その選択的な核磁気共鳴励
起を正確に行なうために必要な精度の高い周波数スペク
トル形状を有する高周波電力の位相を制御する核磁気共
鳴励起用高周波信号発生装置の核磁気共鳴励起用高周波
信号周波数切換方式に関する。
[Industrial Application Field] The present invention is characterized in that the intensity of nuclear magnetic resonance signals obtained by selectively exciting nuclear magnetic resonance substances such as hydrogen nuclei in specific parts of a test object such as a living body depends on the parts inside the living body. The selection of inspection equipment that measures two-dimensional or three-dimensional nuclear magnetic resonance signal intensity images inside living organisms or resonance spectra of specific parts by utilizing the differences in concentration and properties of nuclear magnetic resonance substances. This invention relates to a high-frequency signal frequency switching method for nuclear magnetic resonance excitation of a high-frequency signal generator for nuclear magnetic resonance excitation that controls the phase of high-frequency power having a highly accurate frequency spectrum shape necessary for accurately performing nuclear magnetic resonance excitation. .

【0002】0002

【従来の技術】従来、核磁気共鳴励起用高周波信号発生
装置の核磁気共鳴励起用高周波信号周波数切換に利用さ
れている Direct Digital Frequ
ency Synthesizer については、Ro
dger H. Hosking ; Direct 
Digital Frequency Synthes
is, RocklandSystems Corpo
ration, West Nyack, New Y
ork. または P.H.Saul D.G.Tay
lor ;A High Speed Direct 
Frequency Synthesizer, Pl
essy Research & Technolog
yResearch Review 1989. にお
いて論じられている。
[Prior Art] Direct Digital Frequency has conventionally been used to switch the frequency of a high-frequency signal for nuclear magnetic resonance excitation in a high-frequency signal generator for nuclear magnetic resonance excitation.
For ency Synthesizer, please refer to Ro
dger H. Hosking; Direct
Digital Frequency Synthes
is, Rockland Systems Corpo
ration, West Nyack, New Y
ork. or P. H. Saul D. G. Tay
lor ;A High Speed Direct
Frequency Synthesizer, Pl
essy Research & Technology
yResearch Review 1989. It is discussed in

【0003】動作原理は出力波の位相を記憶するラッチ
(位相加算器)の値をクロック発振器で決まる単位時間
ごとに周波数設定値だけ増加させ、その出力からROM
テーブルを用いてデータを正弦波に変換するというもの
である。
The principle of operation is that the value of a latch (phase adder) that stores the phase of the output wave is increased by the frequency setting value every unit time determined by the clock oscillator, and the output is stored in the ROM.
It uses a table to convert data into a sine wave.

【0004】0004

【発明が解決しようとする課題】上記従来技術は出力周
波数に比例する位相増加分がクロック発振器の周期ごと
に直線的に位相を増加させ、この位相を正弦波を記憶し
ているROMテーブルとDAコンバータを利用して対応
する電圧に変換するものであるので位相制御の点につい
て配慮がされておらず、出力周波数の位相は周波数を設
定した時間により一義的に定まり、周波数を切り換える
と位相もその都度切り換わってしまうという問題があっ
た。
[Problems to be Solved by the Invention] In the above prior art, the phase increment proportional to the output frequency linearly increases the phase for each cycle of the clock oscillator, and this phase is transferred between the ROM table storing the sine wave and the DA. Since it uses a converter to convert to the corresponding voltage, no consideration is given to phase control; the phase of the output frequency is uniquely determined by the time at which the frequency is set, and when the frequency is switched, the phase also changes. There was a problem that it would switch every time.

【0005】本発明の目的は出力波の周波数と位相を独
立に制御することにある。
An object of the present invention is to independently control the frequency and phase of the output wave.

【0006】[0006]

【課題を解決するための手段】上記目的は出力波データ
を基準発振出力と周波数データの積および位相データの
和により生成することにより達成される。
The above object is achieved by generating output wave data by the product of a reference oscillation output and frequency data and the sum of phase data.

【0007】[0007]

【作用】クロック発振器とカウンタは出力波の基準とな
る周波数ωtを発振する。乗算器を用いて周波数データ
αをこのωtに乗じて出力波の周波数(αωt)を決定
する。さらに加算器を用いて位相データβを加えて出力
波の周波数と位相(αωt+β)を決定する。ROMテ
ーブルは正弦波関数を発生するので出力データはsin
(αωt+β)のように変換される。このデジタルデー
タをDAコンバータで対応する電圧に変換する。このよ
うに位相の基準はクロック発振器とカウンタによって定
まるωtにあり、位相データは周波数データとは独立に
演算されるので出力波の位相は周波数と時間とに無関係
に設定することが出来るようになる。
[Operation] The clock oscillator and counter oscillate at a frequency ωt that is the reference of the output wave. This ωt is multiplied by the frequency data α using a multiplier to determine the frequency (αωt) of the output wave. Further, phase data β is added using an adder to determine the frequency and phase (αωt+β) of the output wave. Since the ROM table generates a sine wave function, the output data is sin
It is converted as (αωt+β). This digital data is converted into a corresponding voltage using a DA converter. In this way, the phase reference is ωt determined by the clock oscillator and counter, and the phase data is calculated independently of the frequency data, so the phase of the output wave can be set independently of frequency and time. .

【0008】[0008]

【実施例】以下、本発明の一実施例を図1により説明す
る。
[Embodiment] An embodiment of the present invention will be explained below with reference to FIG.

【0009】図1は本発明のブロック図を示すものであ
る。このデジタル周波数シンセサイザでは周波数の分解
能が10Hz、設定が10Hzから1310710Hz
 で位相の設定が約1.4度 のSIN波形を発振する
ものである。
FIG. 1 shows a block diagram of the present invention. This digital frequency synthesizer has a frequency resolution of 10Hz and settings from 10Hz to 1310710Hz.
It oscillates a SIN waveform with a phase setting of approximately 1.4 degrees.

【0010】クロック発振器1は、10485760H
zを発振する。カウンタ2は、20ビットのバイナリカ
ウンタで20ビットの出力をもち、クロック発振器1に
よりループカウンタを形成し10Hzの基準周波数デー
タを出力する。一方、CPU9より周波数データラッチ
7に17ビット(0から131071)の周波数データ
を送る。乗算器3はカウンタ2の20ビットの基準周波
数データと周波数データラッチ7の17ビットの周波数
データの積を演算する。乗算器3の出力は37ビットと
なるが周波数分解能が10Hzであるので20ビットを
越えるオーバーフローは切り捨て、さらに最終的な出力
で必要かつ十分な分解能とスプリアス強度を得るには1
2ビットのデータで十分であるので下位8ビットも切り
捨てる。したがって乗算器3以降の演算は乗算器3の3
7ビットの出力の9ビットから20ビットの間の12ビ
ットを用いる。また、CPU9は位相データラッチ8に
8ビット(位相の分解能は約1.4度 となる)の位相
データを送る。加算器4は乗算器3の12ビット周波数
情報の上位8ビットに位相データラッチ8の8ビットの
位相データを加算する。ここでも12ビットを越えるオ
ーバフローは切り捨てる。以上のようにして得られた1
2ビットの周波数位相情報をROMテーブル5により振
幅値に変換する。ROMテーブル5は12ビットのアド
レスに対して12ビット分解能の1周期分の正弦波デー
タを出力する。最後にDAコンバータ6によりROMテ
ーブル5の12ビット正弦波データを電圧変換する。
Clock oscillator 1 is 10485760H
z oscillates. Counter 2 is a 20-bit binary counter with a 20-bit output, forms a loop counter with clock oscillator 1, and outputs reference frequency data of 10 Hz. On the other hand, the CPU 9 sends 17 bits (0 to 131071) of frequency data to the frequency data latch 7. The multiplier 3 calculates the product of the 20-bit reference frequency data of the counter 2 and the 17-bit frequency data of the frequency data latch 7. The output of multiplier 3 will be 37 bits, but since the frequency resolution is 10 Hz, any overflow exceeding 20 bits will be truncated, and in order to obtain the necessary and sufficient resolution and spurious intensity in the final output, the frequency resolution will be 10 Hz.
Since 2 bits of data is sufficient, the lower 8 bits are also discarded. Therefore, the calculation after multiplier 3 is 3 of multiplier 3.
12 bits between bits 9 and 20 of the 7-bit output are used. Further, the CPU 9 sends 8-bit phase data (the phase resolution is approximately 1.4 degrees) to the phase data latch 8. The adder 4 adds the 8-bit phase data of the phase data latch 8 to the upper 8 bits of the 12-bit frequency information of the multiplier 3. Here too, any overflow exceeding 12 bits is truncated. 1 obtained as above
The 2-bit frequency phase information is converted into an amplitude value using the ROM table 5. The ROM table 5 outputs one cycle of sine wave data with 12-bit resolution for a 12-bit address. Finally, the 12-bit sine wave data in the ROM table 5 is converted into voltage by the DA converter 6.

【0011】上記の構成によりカウンタ2が計数を開始
した時点が位相の基準(零)となる。したがって出力の
周波数を任意の時間において切り換えてもその周波数に
おける位相はカウンタ2の位相基準によって決まりその
時間において切り換えた周波数に固有の位相を有するこ
とになる。また位相データによって出力の位相を切り換
えても位相基準はカウンタ2に保存されているので出力
の位相を元に戻したい場合は位相データをクリアするこ
とにより簡単に行うことができる。
With the above configuration, the time point at which the counter 2 starts counting becomes the phase reference (zero). Therefore, even if the output frequency is switched at any given time, the phase at that frequency is determined by the phase reference of the counter 2 and has a phase unique to the frequency switched at that time. Furthermore, even if the phase of the output is switched according to the phase data, the phase reference is stored in the counter 2, so if it is desired to return the phase of the output to its original state, it can be easily done by clearing the phase data.

【0012】本実施例によればデジタル周波数シンセサ
イザの周波数を切り換えても位相の基準は変化しないと
いう効果がある。
According to this embodiment, there is an advantage that even if the frequency of the digital frequency synthesizer is switched, the phase reference does not change.

【0013】[0013]

【発明の効果】本発明によれば、一つの周波数を発生す
る基準信号発生器の周波数を任意の時間に切り換えても
その周波数における位相はある位相基準によって決まる
その周波数に固有の位相を有するので核磁気共鳴信号強
度像あるいは特定部位の共鳴スペクトルを計測する検査
装置において磁気共鳴物質を選択的に励起して得られる
核磁気共鳴信号の位相を制御することができるので、核
磁気共鳴信号の位相情報を有効に利用した各種の信号計
測方法を実施することができる効果がある。
According to the present invention, even if the frequency of a reference signal generator that generates one frequency is switched at any time, the phase at that frequency has a phase specific to that frequency determined by a certain phase reference. The phase of the nuclear magnetic resonance signal obtained by selectively exciting the magnetic resonance substance in an inspection device that measures the nuclear magnetic resonance signal intensity image or the resonance spectrum of a specific region can be controlled, so the phase of the nuclear magnetic resonance signal can be controlled. This has the effect of being able to implement various signal measurement methods that effectively utilize information.

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

【図1】本発明の一実施例のブロックダイヤグラムを示
す図である。
FIG. 1 is a diagram showing a block diagram of an embodiment of the present invention.

【符号の説明】[Explanation of symbols]

1…クロック発振器、2…カウンタ、3…乗算器、4…
加算器、5…ROMテーブル、6…DAコンバータ、7
…周波数データラッチ、8…位相データラッチ、9…C
PU。
1... Clock oscillator, 2... Counter, 3... Multiplier, 4...
Adder, 5...ROM table, 6...DA converter, 7
...Frequency data latch, 8...Phase data latch, 9...C
P.U.

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】核磁気共鳴を励起するための高周波信号を
予め設計された低周波信号波形で振幅変調することによ
り、特定した周波数帯域内のスペクトル成分のみの高周
波信号を発生させ、これを電力増幅して核磁気共鳴励起
信号とし被検体に照射することにより核磁気共鳴周波数
が前記特定周波数帯域内にある核スピンの核磁気共鳴の
みを選択的に励起するようにした核磁気共鳴励起用高周
波信号発生装置の高周波の周波数を決定する基準信号発
生器において、一つの周波数を発生する基準信号発生器
の周波数を任意の時間において変化させてもその周波数
における位相はある位相基準によって決まるその周波数
に固有の位相を有することを特徴とする核磁気共鳴励起
用高周波信号周波数切換方式。
Claim 1: By amplitude-modulating a high-frequency signal for exciting nuclear magnetic resonance with a pre-designed low-frequency signal waveform, a high-frequency signal with only spectral components within a specified frequency band is generated, and this is used to generate electric power. A high frequency for nuclear magnetic resonance excitation that selectively excites only the nuclear magnetic resonance of nuclear spins whose nuclear magnetic resonance frequency is within the specific frequency band by amplifying the signal and irradiating it to the subject as a nuclear magnetic resonance excitation signal. In a reference signal generator that determines the high frequency of a signal generator, even if the frequency of the reference signal generator that generates one frequency is changed at any time, the phase at that frequency remains the same as that frequency determined by a certain phase reference. A high-frequency signal frequency switching method for nuclear magnetic resonance excitation characterized by having a unique phase.
【請求項2】請求項1の核磁気共鳴励起用高周波信号発
生装置の高周波の周波数を決定する基準信号発生器にお
いて、一つの周波数を発生する基準信号発生器として設
定周波数の切換分解能に等しい周波数を発振する基準発
振ループカウンタの出力と周波数を設定する定数を乗算
しその積を正弦波関数変換した後DA変換するデジタル
周波数シンセサイザーを構成することを特徴とする核磁
気共鳴励起用高周波信号周波数切換方式。
2. In the reference signal generator for determining the frequency of the radio frequency of the radio frequency signal generator for nuclear magnetic resonance excitation according to claim 1, the reference signal generator for generating one frequency has a frequency equal to the switching resolution of the set frequency. A high-frequency signal frequency switch for nuclear magnetic resonance excitation, comprising a digital frequency synthesizer that multiplies the output of a reference oscillation loop counter that oscillates by a constant that sets the frequency, converts the product into a sine wave function, and then converts it from digital to analog. method.
【請求項3】請求項2のデジタル周波数シンセサイザー
において基準発振ループカウンタの出力と周波数を設定
する定数を乗算した後その積と位相オフセットを設定す
る定数の和を正弦波関数変換した後DA変換することに
より核磁気共鳴励起用高周波信号発生装置の高周波の位
相を任意に設定することができることを特徴とする核磁
気共鳴励起用高周波信号周波数切換方式。
3. In the digital frequency synthesizer according to claim 2, the output of the reference oscillation loop counter is multiplied by a constant for setting the frequency, and then the sum of the product and the constant for setting the phase offset is converted into a sine wave function and then DA converted. 1. A high-frequency signal frequency switching system for nuclear magnetic resonance excitation, characterized in that the phase of the high-frequency wave of a high-frequency signal generator for nuclear magnetic resonance excitation can be arbitrarily set.
JP3110150A 1991-05-15 1991-05-15 High frequency signal frequency switching system for exciting nuclear magnetic resonance Pending JPH04338457A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3110150A JPH04338457A (en) 1991-05-15 1991-05-15 High frequency signal frequency switching system for exciting nuclear magnetic resonance

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3110150A JPH04338457A (en) 1991-05-15 1991-05-15 High frequency signal frequency switching system for exciting nuclear magnetic resonance

Publications (1)

Publication Number Publication Date
JPH04338457A true JPH04338457A (en) 1992-11-25

Family

ID=14528322

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3110150A Pending JPH04338457A (en) 1991-05-15 1991-05-15 High frequency signal frequency switching system for exciting nuclear magnetic resonance

Country Status (1)

Country Link
JP (1) JPH04338457A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007111502A (en) * 2005-09-22 2007-05-10 Ge Medical Systems Global Technology Co Llc Direct digital synthesizer, direct digital synthesizer for transmission and detection, and mri apparatus

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007111502A (en) * 2005-09-22 2007-05-10 Ge Medical Systems Global Technology Co Llc Direct digital synthesizer, direct digital synthesizer for transmission and detection, and mri apparatus

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