[go: up one dir, main page]

JPH04194767A - Oscillating device for rf pulse - Google Patents

Oscillating device for rf pulse

Info

Publication number
JPH04194767A
JPH04194767A JP2323333A JP32333390A JPH04194767A JP H04194767 A JPH04194767 A JP H04194767A JP 2323333 A JP2323333 A JP 2323333A JP 32333390 A JP32333390 A JP 32333390A JP H04194767 A JPH04194767 A JP H04194767A
Authority
JP
Japan
Prior art keywords
amplifier
harmonic
output
lpf
harmonic components
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
JP2323333A
Other languages
Japanese (ja)
Inventor
Takeshi Endo
剛 遠藤
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
Canon Medical Systems Corp
Original Assignee
Toshiba Corp
Toshiba Medical Systems Engineering Co 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 Toshiba Corp, Toshiba Medical Systems Engineering Co Ltd filed Critical Toshiba Corp
Priority to JP2323333A priority Critical patent/JPH04194767A/en
Publication of JPH04194767A publication Critical patent/JPH04194767A/en
Pending legal-status Critical Current

Links

Landscapes

  • Magnetic Resonance Imaging Apparatus (AREA)

Abstract

PURPOSE:To obtain an RF pulse containing little harmonic component by a construction wherein an RF amplifier is of a push-pull type and LPF has an attenuation pole at a frequency being equivalent to a tertiary harmonic generated from the RF amplifier. CONSTITUTION:In an output of an oscillator 1, i.e. an output signal at a point P1, only an RF signal of a frequency (f) exists. When the output passes through an RF amplifier 4 and is amplified thereby, thereafter, harmonic components are generated. Since the amplifier 4 employed herein is of a push-pull type, on the occasion, an odd-number-order harmonic component is large and an even-number-order harmonic component is small due to the characteristics of the amplifier. In an output of the amplifier 4, i.e. an output signal at a point P2, accordingly, the component of a tertiary harmonic 3f is large. LPF 5 is so set as to have an attenuation pole at the harmonic 3f, and therefore the harmonic components of the tertiary harmonic and around it can be removed. Accordingly, the RF signal hardly containing the harmonic components can be obtained for an output of the LPF 5, i.e. an output signal at a point P3.

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、MHI装置に用いられるRFパルス発振装置
に係り、特に、RFアンプから発生する高調波成分を除
去する技術に関する。
[Detailed Description of the Invention] [Object of the Invention] (Industrial Application Field) The present invention relates to an RF pulse oscillation device used in an MHI device, and particularly relates to a technique for removing harmonic components generated from an RF amplifier. .

(従来の技術) 一般に、MRI装置(磁気共鳴イメージング装置)には
、被検体に共鳴周波数の高周波を印加するためにRFコ
イルが設けられており、このRFコイルにRFパルスを
与えるためにRFパルス発振装置か備えられている。
(Prior Art) Generally, an MRI apparatus (magnetic resonance imaging apparatus) is provided with an RF coil for applying a high frequency wave at a resonance frequency to a subject, and an RF pulse is provided for applying an RF pulse to the RF coil. Equipped with an oscillator.

従来におけるRFパルス発振装置は、第4図に示すよう
に、発振器1と、全固体化型のRFアンプ2と、ローパ
スフィルタ3(以下、LPFという)から構成され、発
振器1から出力されるRF倍信号RFアンプ2て増幅さ
れた後、LPF3で高調波成分が除去されRFコイルに
出力されるようになっている。
As shown in FIG. 4, a conventional RF pulse oscillation device is composed of an oscillator 1, an all-solid-state RF amplifier 2, and a low-pass filter 3 (hereinafter referred to as LPF), and the RF pulse oscillator output from the oscillator 1 After being amplified by the double signal RF amplifier 2, harmonic components are removed by the LPF 3, and the signal is output to the RF coil.

(発明が解決しようとする課題) しかしなから、このような従来のRFパルス発振装置で
は、RFアンプ2として広帯域の全固体化形のものを使
用しているので、高調波歪が多く、波形をモニタする場
合非常に不便であるという欠点があった。また、高調波
成分を除去するLPF3は、急峻な減衰特性を持つもの
を使用しなければならないので、LPF3の回路構成が
複雑になるばかりでなく、調整操作が煩雑になってしま
うという課題かあった。
(Problem to be solved by the invention) However, in such conventional RF pulse oscillation devices, a broadband all-solid-state type is used as the RF amplifier 2, so there is a lot of harmonic distortion and the waveform The drawback was that it was very inconvenient to monitor. In addition, since the LPF 3 that removes harmonic components must have a steep attenuation characteristic, the LPF 3 circuit configuration is not only complicated, but also the adjustment operation becomes complicated. Ta.

この発明はこのような従来の課題を解決するためになさ
れたもので、その目的とするところは、簡単な回路で構
成されるLPFを用いて高調波成分の少ないRFパルス
を得ることのできるRFパルス発振装置を提供すること
にある。
This invention was made in order to solve such conventional problems, and its purpose is to provide an RF pulse that can obtain RF pulses with few harmonic components using an LPF configured with a simple circuit. An object of the present invention is to provide a pulse oscillation device.

[発明の構成] (課題を解決するための手段) 上記目的を達成するため、本発明は、発振器から出力さ
れるRF倍信号RFアンプで増幅し、低域通過フィルタ
で高調波成分を除去した後、RFコイルに供給するRF
パルス発振装置において、前記RFアンプはプッシュプ
ル形であり、前記低域通過フィルタは、RFアンプから
発生する第三次高調波に相当する周波数に減衰極をもつ
ことが特徴である。
[Structure of the invention] (Means for solving the problem) In order to achieve the above object, the present invention amplifies the RF multiplied signal output from an oscillator with an RF amplifier, and removes harmonic components with a low-pass filter. After that, RF is supplied to the RF coil.
In the pulse oscillator, the RF amplifier is of a push-pull type, and the low-pass filter has an attenuation pole at a frequency corresponding to a third harmonic generated from the RF amplifier.

(作用) 上述の如く構成すれば、発振器から出力されるRFパル
スは、プッシュプル形のRFアンプて増幅される。そし
て、増幅後の信号には、奇数番目の高調波成分か多く含
まれ、偶数番目の高調波成分は少ない。従って、三次高
調波に減衰極をもつ低域通過フィルタを用いれば、はと
んどの高調波成分を除去することかでき、高調波歪の少
ないRFパルスを得ることができるようになる。
(Function) With the configuration as described above, the RF pulse output from the oscillator is amplified by the push-pull type RF amplifier. The amplified signal contains many odd-numbered harmonic components and few even-numbered harmonic components. Therefore, if a low-pass filter having an attenuation pole for the third harmonic is used, most of the harmonic components can be removed and an RF pulse with less harmonic distortion can be obtained.

(実施例) 第1図は本発明の一実施例を示す構成図である。同図に
示すRFパルス発振装置は、RF倍信号発振する発振器
1と、このRF倍信号増幅するプッシュプル形のRFア
ンプ4と、高調波成分を除去する低域通過フィルタ5(
以下、LPFという)から構成されている。
(Embodiment) FIG. 1 is a configuration diagram showing an embodiment of the present invention. The RF pulse oscillator shown in the figure includes an oscillator 1 that oscillates an RF multiplied signal, a push-pull type RF amplifier 4 that amplifies the RF multiplied signal, and a low-pass filter 5 that removes harmonic components.
(hereinafter referred to as LPF).

LPF5は、第2図に示すように、RF周波数fの三次
高調波3fに減衰極を持つ特性を有している。
As shown in FIG. 2, the LPF 5 has a characteristic of having an attenuation pole at the third harmonic 3f of the RF frequency f.

このような構成において、発振器1の出力、即ち点P1
における出力信号は、第3図(A)に示す如くであり、
周波数fのRF倍信号みが存在している。その後、RF
アンプ4を通過して増幅されると高調波成分が発生する
。このとき、RFアンプ4はプッシュプル形のものを用
いているので、その特性から、奇数番目の高調波成分か
大きく、偶数番目の高調波成分か小さくなる。従って、
RFアンプ4の出力、即ち点P2における出力信号は第
3図(B)に示す如くとなり、三次高調波3fの成分が
大きくなる。
In such a configuration, the output of oscillator 1, i.e. point P1
The output signal in is as shown in FIG. 3(A),
Only the RF multiplied signal of frequency f exists. After that, R.F.
When the signal passes through the amplifier 4 and is amplified, harmonic components are generated. At this time, since the RF amplifier 4 uses a push-pull type, due to its characteristics, odd-numbered harmonic components are large and even-numbered harmonic components are small. Therefore,
The output of the RF amplifier 4, that is, the output signal at point P2 becomes as shown in FIG. 3(B), and the third harmonic component 3f becomes large.

そして、前記したようにLPF5は三次高調波3fに減
衰極を持つように設定されているので、三次高調波を中
心に高調波成分を除去することかできる。従って、LP
F5の出力、即ち点P3における出力信号は第2図(C
)に示す如くとなり、はとんど高調波成分を含まないR
F倍信号得ることができる。
As described above, since the LPF 5 is set to have an attenuation pole at the third harmonic 3f, it is possible to remove harmonic components centered on the third harmonic. Therefore, L.P.
The output of F5, that is, the output signal at point P3 is shown in Figure 2 (C
), and R contains almost no harmonic components.
F times signal can be obtained.

このようにして、本実施例では、RFアンプ4としてプ
ッシュプル形のものを使用し、また、三次高調波3fに
減衰極をもつLPF5を用いて高調波成分を除去してい
るので、高調波成分が低減し、高調波歪の少ないRF倍
信号得ることかできる。また、三次高調波3fに減衰極
を持つLPF5は、簡単な回路で構成することができる
ので、省スペース化、省コスト化が図れるようになり、
調整操作も簡易化される。
In this way, in this embodiment, a push-pull type is used as the RF amplifier 4, and the LPF 5 having an attenuation pole at the third harmonic 3f is used to remove the harmonic component. It is possible to obtain an RF multiplied signal with reduced components and less harmonic distortion. In addition, the LPF 5, which has an attenuation pole at the third harmonic 3f, can be configured with a simple circuit, making it possible to save space and cost.
Adjustment operations are also simplified.

[発明の効果] 以上説明したように、本発明では、プッシュプル形のR
FアンプてRF倍信号増幅し、三次高調波に減衰極をも
つ低減通過フィルタ(L P F)で高調波成分を除去
している。従って、高調波成分か低減し、高周波歪の少
ないRFパルス信号を得ることができる。また、簡単な
回路で低域通過フィルタを構成でき、調整操作が簡易化
されるという効果が得られる。
[Effect of the invention] As explained above, in the present invention, the push-pull type R
The F amplifier amplifies the RF signal, and a low pass filter (LPF) having an attenuation pole at the third harmonic removes the harmonic component. Therefore, it is possible to reduce harmonic components and obtain an RF pulse signal with less high frequency distortion. Further, the low-pass filter can be configured with a simple circuit, and the adjustment operation can be simplified.

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

第1図は本発明の一実施例を示す構成図、第2図はLP
Fの特性図、第3図は各点p、、p2゜P3における出
力信号を示す図、第4図は従来例を示す構成図である。 1・・・発振器      4・・・RFアンプ5・・
・低域通過フィルタ(L P F)第1図
Figure 1 is a configuration diagram showing an embodiment of the present invention, Figure 2 is an LP
FIG. 3 is a diagram showing the output signals at each point p, . . . p2°P3, and FIG. 4 is a diagram showing a conventional example. 1... Oscillator 4... RF amplifier 5...
・Low pass filter (LPF) Figure 1

Claims (1)

【特許請求の範囲】 発振器から出力されるRF信号をRFアンプで増幅し、
低域通過フィルタで高調波成分を除去した後、RFコイ
ルに供給するRFパルス発振装置において、 前記RFアンプはプッシュプル形であり、前記低域通過
フィルタは、RFアンプから発生する第三次高調波に相
当する周波数に減衰極をもつことを特徴とするRFパル
ス発振装置。
[Claims] Amplifying the RF signal output from the oscillator with an RF amplifier,
In an RF pulse oscillation device that supplies harmonic components to an RF coil after removing harmonic components with a low-pass filter, the RF amplifier is of a push-pull type, and the low-pass filter removes third-order harmonic components generated from the RF amplifier. An RF pulse oscillation device characterized by having an attenuation pole at a frequency corresponding to a wave.
JP2323333A 1990-11-28 1990-11-28 Oscillating device for rf pulse Pending JPH04194767A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2323333A JPH04194767A (en) 1990-11-28 1990-11-28 Oscillating device for rf pulse

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2323333A JPH04194767A (en) 1990-11-28 1990-11-28 Oscillating device for rf pulse

Publications (1)

Publication Number Publication Date
JPH04194767A true JPH04194767A (en) 1992-07-14

Family

ID=18153628

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2323333A Pending JPH04194767A (en) 1990-11-28 1990-11-28 Oscillating device for rf pulse

Country Status (1)

Country Link
JP (1) JPH04194767A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2015058632A1 (en) * 2013-10-21 2015-04-30 江苏多维科技有限公司 Push-pull bridge-type magnetic sensor for high-intensity magnetic fields

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2015058632A1 (en) * 2013-10-21 2015-04-30 江苏多维科技有限公司 Push-pull bridge-type magnetic sensor for high-intensity magnetic fields
US9857434B2 (en) 2013-10-21 2018-01-02 MultiDimension Technology Co., Ltd. Push-pull bridge-type magnetic sensor for high-intensity magnetic fields

Similar Documents

Publication Publication Date Title
JP2007336434A (en) PLL oscillator circuit
JPS62132434A (en) Gate circuit
JP3695938B2 (en) Buffer amplifier circuit
JPH04194767A (en) Oscillating device for rf pulse
KR100366836B1 (en) Signal frequency conversion circuit
JPH0514054A (en) Signal generator
JPS63219209A (en) voltage controlled oscillation circuit
JPH04159803A (en) Power amplifier
JP3804209B2 (en) Phase-locked oscillator
JPH0754892B2 (en) Filter circuit
JP2592941Y2 (en) Switching power supply for MR device
JPH1076947A (en) Intermittent control type signal selection device
KR20010064308A (en) Crystal oscillation circuit
JP2006051239A (en) Ultrasonic diagnostic equipment and ultrasonic probes
JPH0621842A (en) Am electronic synchronization tuner
JPH0865050A (en) Oscillator
JP2001077628A (en) Crystal oscillation circuit
JP2811310B2 (en) Oscillation circuit
JPH0537268A (en) Interface circuit for audio signal
JPH0511519U (en) Crystal oscillator circuit
JP3610080B2 (en) Arm-mounted radio
SU1195481A1 (en) Quadratic sweep unit
JPH09232871A (en) Multiplier circuit
JPS58164303A (en) Oscillating circuit
JP2007243530A (en) Voice amplification method and voice amplification apparatus