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JPH0331458B2 - - Google Patents
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JPH0331458B2 - - Google Patents

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Publication number
JPH0331458B2
JPH0331458B2 JP62217336A JP21733687A JPH0331458B2 JP H0331458 B2 JPH0331458 B2 JP H0331458B2 JP 62217336 A JP62217336 A JP 62217336A JP 21733687 A JP21733687 A JP 21733687A JP H0331458 B2 JPH0331458 B2 JP H0331458B2
Authority
JP
Japan
Prior art keywords
signal
received
received signals
sound ray
correlation
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
JP62217336A
Other languages
Japanese (ja)
Other versions
JPS6462134A (en
Inventor
Tooru Shimazaki
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.)
GE Healthcare Japan Corp
Original Assignee
Yokogawa Medical Systems 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 Yokogawa Medical Systems Ltd filed Critical Yokogawa Medical Systems Ltd
Priority to JP62217336A priority Critical patent/JPS6462134A/en
Priority to US07/465,166 priority patent/US5090412A/en
Priority to DE3854303T priority patent/DE3854303T2/en
Priority to EP88907807A priority patent/EP0394439B1/en
Priority to PCT/JP1988/000872 priority patent/WO1989001761A1/en
Publication of JPS6462134A publication Critical patent/JPS6462134A/en
Publication of JPH0331458B2 publication Critical patent/JPH0331458B2/ja
Granted legal-status Critical Current

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  • Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
  • Ultra Sonic Daignosis Equipment (AREA)

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明はトランスジユーサアレイにより超音波
パルスを送受波し、反射波を受波して画像表示す
る電子走査方式の超音波診断装置に関する。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to an electronic scanning ultrasonic diagnostic apparatus that transmits and receives ultrasonic pulses using a transducer array, receives reflected waves, and displays images.

(従来の技術) 超音波診断装置は超音波パルス信号を被検体内
に照射し、超音波の被検体に対する特性即ち減衰
や反射の度合が組織やその病変部により異なるこ
とを利用して反射波によつて形成される断層像を
陰極線管表示装置(以下CRTという)等の画像
表示装置に表示して診断する装置である。従来の
超音波診断装置の概略の構成を第4図に示す。図
において、高周波発振器1で発生した高周波信号
は、送信信号発生器2においてパルス変調されて
送波ビームフオーマ3に入力される。送波ビーム
フオーマ3は入力高周波信号に所定のプログラム
に従つて位相遅延を与え、超音波ビームを形成す
るように入力高周波信号を例えば64チヤネルの信
号に分離する。前記の64チヤネルの信号は、送信
用増幅器、送受切り替えスイツチ、受信用像幅器
等を含む送受信回路4で電力増幅されてトランス
ジユーサアレイ5に入力される。トランジユーサ
アレイ5は入力高周波パルス信号を超音波信号に
変換して被検体内に送波する。被検体内の反射体
から反射された超音波信号は再びトランスジユー
サアレイ5で受波されて高周波電気信号に変換さ
れ、送受信回路4を経て受波ビームフオーマ6に
入力される。64チヤネルの入力信号は受波ビーム
フオーマ6でそれぞれ位相遅延を受け整相加算さ
れて出力される。対数増幅器7は受信信号の広い
ダイナミツクレンジを圧縮して画像表示に適切な
レンジに対数圧縮する増幅器である。対数増幅器
7で圧縮増幅された信号は整流演算器8で検波さ
れ、デイジタルスキヤンコンバータ(以下DSC
という)9でテレビジヨンフオーマツトの信号に
変換されてCRT10で表示される。
(Prior art) Ultrasonic diagnostic equipment irradiates ultrasonic pulse signals into the subject, and detects reflected waves by utilizing the characteristics of ultrasonic waves for the subject, that is, the degree of attenuation and reflection that differs depending on the tissue and its lesion. This device performs diagnosis by displaying tomographic images formed by the CRT on an image display device such as a cathode ray tube display (hereinafter referred to as CRT). FIG. 4 shows a schematic configuration of a conventional ultrasonic diagnostic apparatus. In the figure, a high frequency signal generated by a high frequency oscillator 1 is pulse-modulated by a transmitting signal generator 2 and input to a transmitting beamformer 3. The transmission beam former 3 applies a phase delay to the input high frequency signal according to a predetermined program, and separates the input high frequency signal into signals of, for example, 64 channels so as to form an ultrasonic beam. The signals of the 64 channels described above are power amplified by a transmitting/receiving circuit 4 including a transmitting amplifier, a transmitting/receiving switch, a receiving image width filter, etc., and then inputted to a transducer array 5. The transducer array 5 converts the input high-frequency pulse signal into an ultrasonic signal and transmits it into the subject. The ultrasonic signal reflected from the reflector within the subject is received again by the transducer array 5 and converted into a high frequency electrical signal, which is input to the receiving beamformer 6 via the transmitting/receiving circuit 4. The input signals of the 64 channels are each subjected to a phase delay in the receiving beamformer 6, and are then outputted after being phased and summed. The logarithmic amplifier 7 is an amplifier that logarithmically compresses the wide dynamic range of the received signal to a range suitable for image display. The signal compressed and amplified by the logarithmic amplifier 7 is detected by the rectifier 8 and then converted to a digital scan converter (hereinafter referred to as DSC).
) 9, the signal is converted into a television format signal and displayed on a CRT 10.

(発明が解決しようとする問題点) 上記の超音波診断装置において被検体内の反射
体からの反射波による画像にはスペツクルノイズ
と称されるノイズが織物地又は梨地のように現れ
て、良好な画質の画像を得ることができない。こ
のノイズの発生原因は超音波の波長よりも小さい
散乱物体からの反射波が位相的に干渉して起こる
ものである。
(Problems to be Solved by the Invention) In the above-mentioned ultrasonic diagnostic apparatus, noise called speckle noise appears like a textile or satin material in an image generated by reflected waves from a reflector inside the subject. It is not possible to obtain images of good quality. This noise is caused by phase interference of reflected waves from a scattering object smaller than the wavelength of the ultrasonic wave.

第5図はコンパウンドスキヤンと称せらせるス
キヤン方式を示す図である。イ図は単一プローブ
21を被検体22に当てて観察している図で、こ
の単一プローブ21を21′の位置に動かすと散
乱体に対する角度が変つてスペツクルリダクシヨ
ンは有効である。ロ図はセクタスキヤン23で、
23′の位置にずらしてコンパウンドスキヤンを
している状態を示す図である。このコンパウンド
スキヤンという重ね書き手法はスペツクルリダク
シヨンには大変有効であるが、操作が難しく、速
い動きにはついて行けない等の問題があり、又、
スペツクルリダクシヨンだけのためにコンパウン
ドスキヤンを行うことはできない。
FIG. 5 is a diagram showing a scan method called a compound scan. Figure A is a diagram in which a single probe 21 is applied to a subject 22 for observation. When the single probe 21 is moved to the position 21', the angle relative to the scatterer changes and speckle reduction becomes effective. Figure B is Sector Scan 23,
23 is a diagram illustrating a state in which a compound scan is performed while shifting to the position 23'. This overwriting method called compound scan is very effective for speckle reduction, but it has problems such as being difficult to operate and not being able to keep up with fast movements.
A compound scan cannot be performed solely for speckle reduction.

本発明は上記の問題点に鑑みなされたもので、
その目的は、分解能を落すことなく、微小散乱体
の干渉によつて生ずるスペツクルノイズ及びホワ
イトノイズ等のノイズを減少させ、画質の改善さ
れた超音波診断装置を実現することにある。
The present invention was made in view of the above problems.
The purpose is to reduce noise such as speckle noise and white noise caused by interference of minute scatterers without reducing resolution, and to realize an ultrasonic diagnostic apparatus with improved image quality.

(問題点を解決するための手段) 前記の問題点を解決する本発明は、トランスジ
ユーサアレイにより超音波パルスを送受波し、反
射波を受波して画像表示する電子走査方式の超音
波診断装置において、ビーム分解能より小さい角
度又は走査ピツチ単位で掃引する超音波ビーム発
生手段と、受波信号を整相加算する受波ビーム形
式手段と、整相加算された受波信号を略対数関数
で増幅する増幅手段と、受信信号を一時格納する
記憶手段と、該記憶手段からの信号と1音線分遅
れて受信した受信信号との相関関係を求める演算
手段とを具備し、1走査線に対応する受波信号を
複数の相関性の強い受信信号から合成することを
特徴とするものである。
(Means for Solving the Problems) The present invention, which solves the above-mentioned problems, uses an electronic scanning type ultrasound system that transmits and receives ultrasound pulses using a transducer array, receives reflected waves, and displays images. In the diagnostic device, there is an ultrasonic beam generating means that sweeps in an angle or scanning pitch unit smaller than the beam resolution, a receiving beam formatting means that performs phasing and summation of received signals, and a receiving beam formatting means that performs phasing and summation of the received signals, and converts the phasing and summation of the received signals into a substantially logarithmic function. , an amplification means for amplifying the received signal, a storage means for temporarily storing the received signal, and an arithmetic means for calculating the correlation between the signal from the storage means and the received signal received with a delay of one sound line. This method is characterized in that a received signal corresponding to the above is synthesized from a plurality of highly correlated received signals.

(作用) ビーム分解能より小さい角度単位で送波した音
線に基づく受信信号を整相加算し、対数増幅後記
憶手段に一時格納し、次の音線に基づく受信信号
と相関演算を行う。
(Operation) Received signals based on sound rays transmitted in angular units smaller than the beam resolution are phased and summed, temporarily stored in a storage means after logarithmic amplification, and a correlation calculation is performed with a received signal based on the next sound ray.

(実施例) 以下、図面を参照して本発明の実施例を詳細に
説明する。
(Example) Hereinafter, an example of the present invention will be described in detail with reference to the drawings.

第1図は本発明のセクタ走査における一実施例
のブロツク図である。図において、第4図と同等
の部分には同一の符号を付してある。図中、11
はアナログ信号をデイジタル信号に変換するAD
変換器で、そのデイジタル信号は音線1ライン分
のデータを一時格納する1ラインバツフアメモリ
12に入力されると共に、相関演算器13にも入
力される。相関演算器13は1ラインバツフアメ
モリ12に格納された前回のデータとAD変換器
11からの今回のデータとを加算平均する。
FIG. 1 is a block diagram of one embodiment of the sector scanning of the present invention. In the figure, parts equivalent to those in FIG. 4 are given the same reference numerals. In the figure, 11
is an AD that converts analog signals into digital signals.
The digital signal of the converter is input to a one-line buffer memory 12 that temporarily stores data for one line of sound rays, and is also input to a correlation calculator 13. The correlation calculator 13 adds and averages the previous data stored in the 1-line buffer memory 12 and the current data from the AD converter 11.

次に上記のように構成された実施例の装置の動
作を説明する。高周波発振器1で発生した高周波
信号が送信信号発生器2でパルス変調され、送波
ビームフオーマ3において遅延処理を受け、送受
信回路4を経てトランスジユーサアレイ5から送
波されるまでは第4図の従来の装置で説明したの
と同様である。トランスジユーサアレイ5は例え
ば第1音線Aを送波し、次に僅かにビームを振ら
せて、最小ピンターゲツトを識別し得るビーム分
解能より小さい音響行路差を有する第2音線Bを
送波し、遂次角度を変えて断層面を走査する。
Next, the operation of the apparatus of the embodiment configured as described above will be explained. The high-frequency signal generated by the high-frequency oscillator 1 is pulse-modulated by the transmitting signal generator 2, subjected to delay processing in the transmitting beam former 3, and transmitted from the transducer array 5 via the transmitting/receiving circuit 4 as shown in FIG. This is the same as described for the conventional device. The transducer array 5 transmits, for example, a first acoustic ray A, then swings the beam slightly and transmits a second acoustic ray B having an acoustic path difference smaller than the beam resolution that can identify the smallest pin target. waves and scans the tomographic plane by changing the angle one after another.

前記の第1音線Aに基づく反射波(以下第1音
線A信号という)はトランスジユーサアレイ5で
受波されて、送受信回路4を経て受波ビームフオ
ーマ6で整相加算される。この出力信号は対数増
幅器4で対数圧縮増幅され、AD変換器11でデ
イジタル信号に変換されて、1ラインバツフアメ
モリ12に一時格納されると共に、相関演算器1
3にも入力される。次に第2音線Bに基づく受信
信号(以下2音線B信号という)がAD変換器1
1においてデイジタル信号に変換されて、1ライ
バツフアメモリ12に入力される。この入力によ
つて前回格納されていた第1音線A信号のデータ
は相関演算器13に押し出され、AD変換器11
から相関演算器13に入力された第2音線B信号
と単純加算平均される。この加算平均された信号
は整流演算器8で包絡線検波され、DSC9でテ
レビジヨンフオーマツトの信号に変換されて
CRT10で表示される。
The reflected wave based on the first acoustic ray A (hereinafter referred to as the first acoustic ray A signal) is received by a transducer array 5, passes through a transmitting/receiving circuit 4, and is phased and summed by a receiving beamformer 6. This output signal is logarithmically compressed and amplified by the logarithmic amplifier 4, converted into a digital signal by the AD converter 11, and temporarily stored in the 1-line buffer memory 12.
3 is also input. Next, the received signal based on the second sound ray B (hereinafter referred to as the second sound ray B signal) is sent to the AD converter 1.
1, it is converted into a digital signal and input to the 1-li buffer memory 12. By this input, the data of the first sound ray A signal previously stored is pushed out to the correlation calculator 13, and the data of the first sound ray A signal stored previously is pushed out to the correlation calculator 13,
, and the second acoustic ray B signal inputted to the correlation calculator 13. This averaged signal is envelope-detected by the rectifier 8 and converted to a television format signal by the DSC 9.
Displayed on CRT10.

上記の信号処理の状況を説明する。第2図は第
1音線A信号と第2音線B信号の信号処理の説明
図である。イはトランジユーサ5から送波される
第1音線A信号と第2音線B信号とを示す図、ロ
図は前記第1音線Aに送波している時のトランス
ジユーサ5の指向特性で受波ビームの受波感度を
示している。ハ図は第1図に示すp点、q点及び
r点における信号波形である。図において、15
は送波ビームの最小分解能より大きいピンターゲ
ツトで、音線Aと音線Bのなす角度Δθはピンタ
ーゲツト15を見る角度より小さい。16はピン
ターゲツト15の反射信号の波形、17は微小散
乱体の反射によるスペツクルノイズ波形、18は
包絡線検波された信号波形である。第1音線A信
号のp点における波形をハ図aに示してある。ス
ペツクルノイズ17は比較的大きく現れている。
ハ図bは第2音線B信号のp点における波形で、
ピンターゲツト反射信号16はハ図aの場合と略
同じ大きさで、スペツクルノイズ17も大差なく
現れている。ハ図cはq点における第1音線A信
号と第2音線B信号を相関演算器13で加算平均
した出力波形である。この波形においては、ピン
ターゲツト反射信号16は変りはないが、スペツ
クルノイズ17は減少している。ハ図dは整流演
算器8で包絡線検波された信号波形である。
The situation of the above signal processing will be explained. FIG. 2 is an explanatory diagram of signal processing of the first sound ray A signal and the second sound ray B signal. A is a diagram showing the first sound ray A signal and a second sound ray B signal transmitted from the transducer 5, and B is a diagram showing the orientation of the transducer 5 when transmitting to the first sound ray A. The characteristics indicate the reception sensitivity of the reception beam. Figure C shows signal waveforms at point p, point q, and point r shown in FIG. In the figure, 15
is a pin target larger than the minimum resolution of the transmitted beam, and the angle Δθ formed by sound ray A and sound ray B is smaller than the angle at which the pin target 15 is viewed. 16 is a waveform of a reflected signal from the pin target 15, 17 is a speckle noise waveform due to reflection from a minute scatterer, and 18 is a signal waveform subjected to envelope detection. The waveform of the first sound ray A signal at point p is shown in Figure C a. Speckle noise 17 appears relatively large.
Figure b is the waveform of the second sound ray B signal at point p,
The pin target reflection signal 16 has approximately the same magnitude as in the case of FIG. Figure c is an output waveform obtained by adding and averaging the first sound ray A signal and the second sound ray B signal at point q by the correlation calculator 13. In this waveform, the pin target reflection signal 16 remains unchanged, but the speckle noise 17 is reduced. Figure d shows a signal waveform envelope-detected by the rectifier 8.

第3図に信号処理のシーケンスを示す。イ図は
トランスジユーサ5から遂次送波される音線を示
している。ロ図はイ図の各音線による反射信号の
時分割多重処理の状態を示す図で、音線A信号は
1ラインバツフアメモリ12に格納され、音線B
信号到来後相関演算器13で演算され、同時に音
線B信号は1ラインバツフアメモリ12に格納さ
れる。次に音線C信号到来と共に音線B信号は相
関演算器13に出力され、音線C信号とが加算平
均される。
FIG. 3 shows the signal processing sequence. Figure A shows sound rays successively transmitted from the transducer 5. Figure B is a diagram showing the state of time-division multiplexing of the reflected signals from each sound ray in Figure A. The sound ray A signal is stored in the 1-line buffer memory 12, and the sound ray B signal is stored in the 1-line buffer memory 12.
After the signal arrives, it is calculated by the correlation calculator 13, and at the same time, the sound ray B signal is stored in the 1-line buffer memory 12. Next, when the sound ray C signal arrives, the sound ray B signal is output to the correlation calculator 13, and the sound ray C signal and the sound ray C signal are averaged.

ピンターゲツト15はビーム幅相当の大きさが
あつてビーム幅内で多少変つても振幅位相に十分
に大きな相関があるので殆ど変化のない信号が得
られるが、スペツクルノイズの原因である微小散
乱体による反射は波長よりも小さい物体からの反
射であつて第1音線Aと第2音線Bに同じパター
ンで存在することは少ない。本実施例による相関
演算処理は加算平均であるが、対数増幅器7で増
幅された信号なので実質的には乗算であつて更に
高周波で位相情報も含む処理であるため、各音線
に同時に存在しないスペツクルノイズの積は相関
演算器13よる演算で消滅してしまう。ホワイト
ノイズも又相関関係がなく同様に加算平均処理で
消滅してしまう。従つて、ピンターゲツトを識別
し得る程度の良好な分解能を維持しつつ、スペツ
クルノイズやホワイトノイズの極めて少ない良好
な画質の画像がCRTに表示される。
The pin target 15 has a size equivalent to the beam width, and even if the amplitude and phase change slightly within the beam width, there is a sufficiently large correlation in the amplitude and phase, so a signal with almost no change can be obtained. The reflection from the body is a reflection from an object that is smaller than the wavelength, and the first sound ray A and the second sound ray B rarely have the same pattern. The correlation calculation process according to this embodiment is an arithmetic average, but since the signal is amplified by the logarithmic amplifier 7, it is essentially a multiplication, and the process also includes high frequency and phase information, so it does not exist in each sound ray at the same time. The product of speckle noise disappears in the calculation by the correlation calculator 13. White noise also has no correlation and is similarly eliminated by averaging processing. Therefore, a high-quality image with extremely low speckle noise and white noise is displayed on the CRT while maintaining a high enough resolution to identify the pin target.

尚、本発明は上記実施例に限定されるものでは
ない。信号を一時格納するために用いた1ライン
バツフアメモリは複数ラインバツフアメモリを用
いれば多音線の相関処理を行う等よりフレキシブ
ルに用いることができる。相関演算器は単純加算
平均を行うものを示したが、重み付き加算にして
もよく、更に、深さと共に相関関数の変化する演
算器を用いてもよい。
Note that the present invention is not limited to the above embodiments. The one-line buffer memory used for temporarily storing signals can be used more flexibly by using a plurality of line buffer memories, such as for correlation processing of polyphonic lines. Although the correlation calculator is shown as one that performs simple addition and averaging, weighted addition may be used, and furthermore, an operator whose correlation function changes with depth may be used.

検波は包絡線検波で説明したが、他の検波方式
で行つてもよい。更にスキヤン方法はリニヤスキ
ヤン、セクタスキヤン、コンベツクススキヤン等
各種のスキヤンに適用されることは勿論である。
Detection has been explained using envelope detection, but other detection methods may be used. Furthermore, it goes without saying that the scan method can be applied to various scans such as linear scan, sector scan, and convex scan.

(発明の効果) 以上詳細に説明したように、本発明によれば、
固定目標からの受波信号に影響なく、相関のない
ホワイトノイズは抑圧されてSN比が向上し、又、
スペツクルノイズも消去されて画質が改善され、
実用上の効果は大きい。
(Effects of the Invention) As explained in detail above, according to the present invention,
Uncorrelated white noise is suppressed without affecting the received signal from the fixed target, improving the SN ratio, and
Speckle noise is also removed and image quality is improved.
The practical effects are significant.

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

第1図は本発明の一実施例の構成ブロツク図、
第2図は2音線による信号処理の説明図、第3図
は信号処理のシーケンスを示す図、第4図は従来
の超音波診断装置の概略構成図、第5図はコンパ
ウンドスキヤンの説明図である。 3……送波ビームフオーマ、5……トランスジ
ユーサアレイ、6……受波ビームフオーマ、7…
…対数増幅器、8……整流演算器、9……DSC、
10……CRT、11……AD変換器、12……1
ラインバツフアメモリ、13……相関演算器、1
5……ピンターゲツト、16……ピンターゲツト
反射信号、17……スペツクルノイズ。
FIG. 1 is a block diagram of an embodiment of the present invention.
Fig. 2 is an explanatory diagram of signal processing using two sound lines, Fig. 3 is a diagram showing the sequence of signal processing, Fig. 4 is a schematic diagram of a conventional ultrasonic diagnostic device, and Fig. 5 is an explanatory diagram of compound scan. It is. 3... Transmission beam former, 5... Transducer array, 6... Receiving beam former, 7...
... Logarithmic amplifier, 8 ... Rectifier, 9 ... DSC,
10...CRT, 11...AD converter, 12...1
Line buffer memory, 13... Correlation calculator, 1
5... Pin target, 16... Pin target reflected signal, 17... Speckle noise.

Claims (1)

【特許請求の範囲】[Claims] 1 トランスジユーサアレイにより超音波パルス
を送受波し、反射波を受波して画像表示する電子
走査方式の超音波診断装置において、ビーム分解
能より小さい角度又は走査ピツチ単位で掃引する
超音波ビーム発生手段と、受波信号を整相加算す
る受波ビーム形成手段と、整相加算された受波信
号を略対数関数で増幅する増幅手段と、受信信号
を一時格納する記憶手段と、該記憶手段からの信
号と1音線分遅れて受信した受信信号との相関関
係を求める演算手段とを具備し、1走査線に対応
する受波信号を複数の相関性の強い受信信号から
合成することを特徴とする超音波診断装置。
1 In electronic scanning ultrasound diagnostic equipment that transmits and receives ultrasound pulses using a transducer array, receives reflected waves, and displays images, ultrasound beam generation that sweeps at an angle or scanning pitch unit smaller than the beam resolution means, receiving beam forming means for phasing and adding the received signals, amplifying means for amplifying the phasing and adding received signals by a substantially logarithmic function, storage means for temporarily storing the received signals, and the storage means. and a calculation means for calculating the correlation between the signal from the source and the received signal received with a delay of one sound line, and is capable of synthesizing the received signal corresponding to one scanning line from a plurality of highly correlated received signals. Features of ultrasonic diagnostic equipment.
JP62217336A 1987-08-31 1987-08-31 Ultrasonic diagnostic apparatus Granted JPS6462134A (en)

Priority Applications (5)

Application Number Priority Date Filing Date Title
JP62217336A JPS6462134A (en) 1987-08-31 1987-08-31 Ultrasonic diagnostic apparatus
US07/465,166 US5090412A (en) 1987-08-31 1988-08-31 Ultrasonic diagnosis apparatus
DE3854303T DE3854303T2 (en) 1987-08-31 1988-08-31 ULTRASONIC DIAGNOSTIC DEVICE.
EP88907807A EP0394439B1 (en) 1987-08-31 1988-08-31 Ultrasonic diagnostic apparatus
PCT/JP1988/000872 WO1989001761A1 (en) 1987-08-31 1988-08-31 Ultrasonic diagnostic apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62217336A JPS6462134A (en) 1987-08-31 1987-08-31 Ultrasonic diagnostic apparatus

Publications (2)

Publication Number Publication Date
JPS6462134A JPS6462134A (en) 1989-03-08
JPH0331458B2 true JPH0331458B2 (en) 1991-05-07

Family

ID=16702581

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62217336A Granted JPS6462134A (en) 1987-08-31 1987-08-31 Ultrasonic diagnostic apparatus

Country Status (1)

Country Link
JP (1) JPS6462134A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5922337B2 (en) * 2011-03-31 2016-05-24 ジーイー・メディカル・システムズ・グローバル・テクノロジー・カンパニー・エルエルシー Ultrasonic diagnostic apparatus and control program therefor

Also Published As

Publication number Publication date
JPS6462134A (en) 1989-03-08

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