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JPH0259732B2 - - Google Patents
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JPH0259732B2 - - Google Patents

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Publication number
JPH0259732B2
JPH0259732B2 JP60069936A JP6993685A JPH0259732B2 JP H0259732 B2 JPH0259732 B2 JP H0259732B2 JP 60069936 A JP60069936 A JP 60069936A JP 6993685 A JP6993685 A JP 6993685A JP H0259732 B2 JPH0259732 B2 JP H0259732B2
Authority
JP
Japan
Prior art keywords
signal
received
living body
receiver
wave
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
JP60069936A
Other languages
Japanese (ja)
Other versions
JPS61228835A (en
Inventor
Takashi Ito
Masanori Hirose
Chihiro Kasai
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 Ltd
Original Assignee
Aloka 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 Aloka Co Ltd filed Critical Aloka Co Ltd
Priority to JP6993685A priority Critical patent/JPS61228835A/en
Publication of JPS61228835A publication Critical patent/JPS61228835A/en
Publication of JPH0259732B2 publication Critical patent/JPH0259732B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は超音波診断装置、特に生体内に超音波
を送信しその透過波又は反射波を受信して生体内
の特質分布を測定し表示することのできる改良さ
れた超音波診断装置に関する。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to an ultrasonic diagnostic device, particularly an ultrasonic diagnostic device that transmits ultrasonic waves into a living body, receives the transmitted waves or reflected waves, and measures and displays characteristic distributions within the living body. The present invention relates to an improved ultrasonic diagnostic device that can perform

[従来技術] 生体内に超音波を送信し、そのエコー信号を測
定して生体内の断層像を表示する超音波診断装置
においては、パルスエコー法が多く用いられてお
り、これらの装置では、一般に配列型振動子を用
いて深度方向の各点に鋭い超音波ビームを送信す
るためダイナミツクフオーカスが行われている。
すなわち、深度方向を複数の領域に分割して各領
域に焦点が合うように超音波を送受信して各領域
ごとの超音波反射波を測定することにより広範囲
にわたり生体内の断層像が得られ、また一定範囲
における分割領域の数を増やせば生体内のより精
密な断層像を画像表示することができる。
[Prior Art] The pulse echo method is often used in ultrasound diagnostic devices that transmit ultrasound waves into a living body and measure the echo signals to display tomographic images of the inside of the living body. Dynamic focusing is generally performed using an array type transducer to transmit a sharp ultrasonic beam to each point in the depth direction.
That is, by dividing the depth direction into multiple regions, transmitting and receiving ultrasound so as to focus on each region, and measuring the ultrasound reflected waves for each region, a tomographic image of the inside of the body can be obtained over a wide range. Furthermore, by increasing the number of divided regions within a certain range, a more precise tomographic image of the inside of the body can be displayed.

しかしながら、前記分割領域を増やしていけば
超音波ビームを更に鋭くしなければならず、また
増やした数だけ超音波の送受信回数が増えること
から一断面の断層像の画像形成に時間がかかると
いう欠点が生じていた。このことから、レーダや
ソナーの応用分野で周知である合成開口法の技術
を超音波診断装置へ応用することが提案されてい
る。
However, if the number of divided regions is increased, the ultrasound beam must be made even sharper, and the number of transmission and reception of ultrasound increases by the number of divided regions, so it takes time to form a tomographic image of one cross section. was occurring. For this reason, it has been proposed to apply the synthetic aperture technique, which is well known in the fields of radar and sonar applications, to ultrasound diagnostic equipment.

この合成開口法とは、送受信を繰返しながら送
受信位置を移動させ生体内に超音波送受信を行
い、受信信号を位相を含めて記憶させた後に生体
内の各点に焦点が合うように受信波形を合成して
各点の画像信号を得る方法であり、第1図にその
波形合成の説明が示されている。
This synthetic aperture method involves transmitting and receiving ultrasonic waves inside a living body by repeatedly transmitting and receiving while moving the transmitting/receiving position, storing the received signal including the phase, and then converting the received waveform so that each point in the living body is focused. This is a method of synthesizing to obtain an image signal at each point, and an explanation of the waveform synthesis is shown in FIG.

図において、T1,T2,T3……Toを振動子と
し、この振動子から順次超音波パルスを送信する
と、同じ振動子で受信された受信波形はU1(t),
U2(t),U3(t)……Uo(t)で表される波形と
なつて得られる。この時に振動子T1,T2,T3
……Toからl1,l2,l3……lo離れた点Fに焦点を合
わせ、この点の測定をする場合は各振動子と点F
間を超音波が往復するのに要する時間τiだけ移動
させて加算した波形S(t)を求める。すなわち、 S(t)=oi=1 Ui(t+ti) ただしτi=2li/c(c:音速) で表わされ、これは図中の双曲線f上の振幅を加
算することに相当し大きな振幅を得ることができ
る。また他の点PについてはT1,T2,T3……To
と点Pとの位置関係に対応するUi(t)上のデー
タは双曲線p上の振幅となり、これらを加算すれ
ばこれらの振幅は互いに打ち消しあつて小さくな
る。
In the figure, when T 1 , T 2 , T 3 ...T o is a transducer and ultrasonic pulses are transmitted sequentially from this transducer, the received waveform received by the same transducer is U 1 (t),
The waveforms are obtained as U 2 (t), U 3 (t)...U o (t). At this time, the oscillators T 1 , T 2 , T 3 ,
...If you focus on a point F that is l 1 , l 2 , l 3 ...l o away from T o and measure this point, each transducer and point F
A waveform S(t) is obtained by moving the ultrasonic waves by the time τi required for the ultrasonic wave to reciprocate between the two and adding them. That is, S(t)= oi=1 Ui(t+ti) However, it is expressed as τi=2li/c (c: speed of sound), which corresponds to adding the amplitudes on the hyperbola f in the figure, and is a large You can get the amplitude. For other points P, T 1 , T 2 , T 3 ...T o
The data on Ui(t) corresponding to the positional relationship between and point P becomes the amplitude on the hyperbola p, and when these are added, these amplitudes cancel each other out and become smaller.

従つて、点Fに焦点を合わせればUi(t)のそ
れぞれの受信波は同一位相で加算され振幅は大き
くなるので、この焦点の位置を順次変えて構成す
れば高解像度の断層像が得られることが理解され
る。
Therefore, if the focus is focused on point F, each received wave of Ui(t) will be added in the same phase and the amplitude will become large, so if the position of this focus is sequentially changed, a high-resolution tomographic image can be obtained. That is understood.

しかしながら、前述した焦点以外の点Fの位置
によつては受信信号が同位相で加算される場合が
あり、これは焦点Fの各波形加算の際に仮想的な
音波の干渉が生じ、あたかも超音波ビームが放射
されてるように見える現像、一般にサイドローブ
といわれる現象が生じるという欠点があり、断層
画像の画質を劣化させるという問題があつた。
However, depending on the position of the point F other than the focal point mentioned above, the received signals may be added in the same phase. This method has the drawback of producing a phenomenon that gives the impression that a sound wave beam is being emitted, a phenomenon commonly referred to as a sidelobe, which has the problem of deteriorating the image quality of tomographic images.

[発明の目的] 本発明は前記従来の課題に鑑みなされたもので
あり、その目的は、合成開口法による超音波診断
装置におけるサイドローブを除去して生体内の特
質分布を良好に画像表示することのできる超音波
診断装置を提供することにある。
[Object of the Invention] The present invention has been made in view of the above-mentioned conventional problems, and its purpose is to remove side lobes in an ultrasonic diagnostic apparatus using a synthetic aperture method and to display a good image of characteristic distribution in a living body. The purpose of the present invention is to provide an ultrasonic diagnostic device that can perform

[発明の構成] 前記目的を達成するために、本発明は、生体内
に送波された超音波パルスが生体内を透過した透
過波又は前記生体内から反射した反射波を受波す
る受波器と、前記受波器からの受信信号をA/D
変換するA/D変換器と、前記A/D変換された
受信信号をその受信信号ごとに格納するメモリ
と、を含み、前記メモリからそれぞれ前記受信信
号を読み出し、それぞれ位相を調整して合成加算
演算し、生体内の断層画像を形成する超音波診断
装置において、前記受波器と前記A/D変換器と
の間には、前記受波器からの受信信号をその受信
信号ごとに対数増幅する対数増幅器に設けられた
ことを特徴とする。
[Structure of the Invention] In order to achieve the above-mentioned object, the present invention provides a method for receiving transmitted waves transmitted through the living body or reflected waves reflected from the living body by ultrasonic pulses transmitted into the living body. and A/D the received signal from the receiver.
It includes an A/D converter for converting the A/D converter, and a memory for storing the A/D-converted received signals for each received signal, reads each of the received signals from the memory, adjusts the phase of each, and performs synthesis and addition. In an ultrasonic diagnostic apparatus that performs calculations to form tomographic images in a living body, between the wave receiver and the A/D converter, logarithmic amplification is performed for each received signal from the wave receiver. It is characterized in that it is provided in a logarithmic amplifier.

[作用] 上記構成によれば、A/D変換器の前に対数増
幅器が設けられているので、受信された受信信号
は対数増幅された後にA/D変換され、さらに合
成開口法に基づく合成加算演算されることにな
る。
[Operation] According to the above configuration, since the logarithmic amplifier is provided before the A/D converter, the received signal is logarithmically amplified and then A/D converted, and further synthesized based on the synthetic aperture method. An addition operation will be performed.

従つて、受信信号は圧縮された状態でA/D変
換される。また、各受信信号ごとに対数増幅され
合成加算されるので、メインローブとサイドロー
ブとの信号の大きさの差を増大させることができ
る。
Therefore, the received signal is A/D converted in a compressed state. Furthermore, since each received signal is logarithmically amplified and combined and added, it is possible to increase the difference in signal magnitude between the main lobe and the side lobe.

[実施例] 以下、図面に基づいて本発明の好適な実施例を
説明する。
[Embodiments] Hereinafter, preferred embodiments of the present invention will be described based on the drawings.

本発明において特徴的なことは、超音波受信信
号を非線形に増幅する対数増幅器を設けたので合
成開口法を適用した超音波診断装置において発生
するサイドローブを除去できることであり、まず
第2図に基づいてこのサイドローブ除去の説明を
する。
The characteristic feature of the present invention is that it is equipped with a logarithmic amplifier that nonlinearly amplifies the received ultrasound signal, so it is possible to remove sidelobes that occur in ultrasound diagnostic equipment that uses the synthetic aperture method. This sidelobe removal will be explained based on the following.

生体内のある点Fと点Pは振動子から十分遠方
にあり、T1,T2,T3……Toから点F,Pに結ぶ
線は平行とみなせることから図のように点P方向
は点F方向からθ角の方向にある場合を考える。
前記点Fに焦点を合わせた場合の点Pからのサイ
ドローブ信号が第2図左に示す波形であつたとす
ると各振動子で受信した受信波は時間τずつずれ
たものである。時間τは τ=2d/csinθ (d:振動子間距離、c:音速) で表わされ、これを変形した式cτ=2d sinθにお
いて、cτが波長λの整数倍になる場合(cτ=mλ)
に受信波は干渉する。この時の点Pの方向角θm
は θm=arc sin(mλ/2d) (m:整数) で表わされる。
A certain point F and point P in the living body are far enough away from the vibrator, and the lines connecting T 1 , T 2 , T 3 ...T o to points F and P can be considered parallel, so point P as shown in the figure Consider the case where the direction is at an angle θ from the direction of point F.
If the sidelobe signal from point P when focused on point F has the waveform shown on the left in FIG. 2, the received waves received by each vibrator are shifted by time τ. The time τ is expressed as τ=2d/csinθ (d: distance between transducers, c: sound speed), and in the modified formula cτ=2d sinθ, if cτ is an integral multiple of the wavelength λ (cτ=mλ )
The received waves interfere. At this time, the direction angle θm of point P
is expressed as θm=arc sin(mλ/2d) (m: integer).

すなわち、点Pがθm方向にある場合は点Pか
らの反射波が同位相で加算され(第2図C)大き
な振幅となつてサイドローブが現われ、m=1の
場合が最も強くなる。
That is, when the point P is in the θm direction, the reflected waves from the point P are added in the same phase (FIG. 2C), and a side lobe appears with a large amplitude, and is strongest when m=1.

次に、m=1の場合(θ1方向)のサイドローブ
について考える。
Next, consider the side lobe when m=1 (in the θ1 direction).

各振動子の指向性r(θ)とすれば従来装置に
おいては、各受信波形が合成開口法に基づく合成
演算される前に(例えば受波器のすぐ後で)線形
に加算されるのでθ1方向のサイドローブは、振幅
をa、振動子の数をnとすると nar(θ1) …(1) で表わされ、この指向性r(θ)は焦点F方向で
はθ=0であり通常r(0)=1に規格化されるか
ら、点Fでのメインローブは、 nar(0)=na …(2) となる。
If the directivity of each transducer is r(θ), in the conventional device, each received waveform is linearly added before being subjected to synthetic calculation based on the synthetic aperture method (for example, immediately after the receiver), so θ A side lobe in one direction is expressed as nar(θ 1 )...(1) where the amplitude is a and the number of oscillators is n, and this directivity r(θ) is θ=0 in the focal point F direction. Since it is normally normalized to r(0)=1, the main lobe at point F is nar(0)=na...(2).

そして、従来装置において前記線形増幅された
受信信号は合成開口法に基づく合成演算がされた
後に、一般的に、対数増幅が行われて画像表示さ
れる。つまり、各受信信号のレベル差が非常に大
きいため輝度変調して画像表示した場合に見ずら
くなるので、対数増幅が行われている。ここで、
対数増幅を行う場合には、一般的に、増幅器入力
信号viが雑音レベルδより小さい場合には出力は
0として処理され、大きい場合に限り入力信号は
対数増幅される。該増幅器出力v0を式で表わせ
ば、 βlog(vi/δ) …δvi v0=0 …δ<|vi| −βlog(|vi|/δ)…δvi (β:定数) となる。
In the conventional device, the linearly amplified received signal is subjected to a synthesis calculation based on the synthetic aperture method, and then logarithmically amplified and displayed as an image. In other words, logarithmic amplification is performed because the level difference between each received signal is so large that it becomes difficult to see when displaying an image by modulating the brightness. here,
When performing logarithmic amplification, generally, if the amplifier input signal v i is smaller than the noise level δ, the output is treated as 0, and only if it is larger, the input signal is logarithmically amplified. If the amplifier output v 0 is expressed by the formula, βlog(v i /δ)...δv i v 0 =0...δ<|v i | −βlog(|v i |/δ)...δv i (β: constant) becomes.

従つて、前述したサイドローブ(1)式とメインロ
ーブ(2)式を対数増幅すれば、(3)式のδviの時の
式v=δlog(vi/δ)に代入した式として表わす
ことができ、この差を求めると、 δlog(na/δ)−δlog{nar(θ1)/δ} =δlog{1/r(θ1)} …(4) となり、この(4)式はメインローブレベルとサイド
ローブレベルの差を表わすものである。
Therefore, by logarithmically amplifying the side lobe equation (1) and the main lobe equation (2) mentioned above, it can be expressed as an equation substituted into the equation v = δlog (v i /δ) when δv i in equation (3). and calculating this difference, δlog(na/δ)−δlog{nar(θ 1 )/δ} = δlog{1/r(θ 1 )} …(4), and this equation (4) is This represents the difference between the main lobe level and the side lobe level.

これに対し、本発明に係る装置においては各受
信信号をその受信信号ごとにそれぞれ別に対数増
幅した後に合成演算を行うものである。すなわ
ち、加算される前のサイドローブ信号はar(θ1
であり、メインローブ信号はa{ir(0)=1}で
あるからこれを(3)式により対数増幅すれば、それ
ぞれβlog{ar(θ1)/δ},βlog(a/δ)となる

そして、これらの信号を加算すればサイドローブ
レベルはnβlog{ar(θ1/δ}、メインローブレベル
はn log(a/δ)であるからこれらの差は、 nβlog(a/δ) −nβlog{ar(θ1)/δ} =βlog{1/r(θ1)}n …(5) となる。
On the other hand, in the apparatus according to the present invention, each received signal is logarithmically amplified separately and then the synthesis operation is performed. In other words, the sidelobe signal before being added is ar(θ 1 )
Since the main lobe signal is a{ir(0)=1}, if this is logarithmically amplified using equation (3), we get βlog{ar(θ 1 )/δ} and βlog(a/δ), respectively. Become.
Then, if these signals are added, the sidelobe level is nβlog{ar(θ 1 /δ}, and the mainlobe level is nlog(a/δ), so the difference between them is nβlog(a/δ) −nβlog {ar(θ 1 )/δ} = βlog{1/r(θ 1 )} n (5).

従つて、(4)式と(5)式を比較すると、 βlog{1/r(θ1)}n ≫βlog{1/r(θ1)} (∴0<r(θ)<1) であり、従来装置と本発明ではメインローブレベ
ルとサイドローブレベルの差は大きな違いが生じ
る。
Therefore, comparing equations (4) and (5), βlog{1/r(θ 1 )} n ≫βlog{1/r(θ 1 )} (∴0<r(θ)<1) There is a large difference between the main lobe level and the side lobe level between the conventional device and the present invention.

すなわち、本発明によればメインローブレベル
とサイドローブレベルの差を大きくすることがで
き、このことによりサイドローブ信号の除去が有
効に行えることが理解される。つまり、本発明に
よれば、合成演算を行う前に各受信信号を対数増
幅するため合成演算を行つた後に、メインローブ
レベルとサイドローブレベルとの大きな差を得ら
れる。
That is, it is understood that according to the present invention, the difference between the main lobe level and the side lobe level can be increased, and thereby the side lobe signal can be effectively removed. That is, according to the present invention, a large difference between the main lobe level and the side lobe level can be obtained after performing the combining operation to logarithmically amplify each received signal before performing the combining operation.

第3図には本発明に係る好適な実施例が示され
ている。
FIG. 3 shows a preferred embodiment of the invention.

超音波送受信器10には配列振動子12と、こ
の配列振動子の振動制御を行うマルチプレクサ1
4と、発振器16が設けられており、制御器18
の制御に基づいて発振器16から得られた電気信
号はドライバ20を介してマルチプレクサ14に
供給され、該電気信号は順次超音波に変換されて
生体内に送信される。また生体内からの反射波は
前記各振動子によつて受信され、各振動子の受信
波毎に対数増幅器22によつて対数増幅される。
The ultrasonic transmitter/receiver 10 includes an array transducer 12 and a multiplexer 1 for controlling vibration of the array transducer.
4, an oscillator 16, and a controller 18.
The electrical signals obtained from the oscillator 16 based on the control of the oscillator 16 are supplied to the multiplexer 14 via the driver 20, and the electrical signals are sequentially converted into ultrasonic waves and transmitted into the living body. Further, reflected waves from inside the living body are received by each of the vibrators, and each wave received by each vibrator is logarithmically amplified by the logarithmic amplifier 22.

そして、対数増幅された受信波信号は直交検波
器24に供給されホログラム変換が行われる。す
なわち、発振器16から出力された電気信号は移
送器26を介して乗算器28,30に供給され、
送信超音波の中心周波数を持つ余弦波と正弦波が
増幅された受信信号に乗算され、これを低域通過
フイルタ32,34に入力して搬送波を除去すれ
ば受信信号の振幅と位相の情報をもつ信号(ホロ
グラム)が得られる。
The logarithmically amplified received wave signal is then supplied to the orthogonal detector 24 and subjected to hologram conversion. That is, the electrical signal output from the oscillator 16 is supplied to the multipliers 28 and 30 via the transfer device 26,
A cosine wave and a sine wave having the center frequency of the transmitted ultrasound are multiplied by the amplified received signal, and by inputting this to the low-pass filters 32 and 34 and removing the carrier wave, information on the amplitude and phase of the received signal can be obtained. A signal (hologram) is obtained.

本実施例において前記対数増幅器は直交検波器
24の前に配置されているが、第4図cに示され
るように直交検波器24の後に配置することもで
きる。もちろん、上記対数増幅器は、メモリ40
の前に必ずしも配置されなくても良く、合成開口
法に基づく合成加算演算を行う前であれば、任意
な個所に配置可能である。しかしながら、後述す
るように、メモリ40の容量を減少させるために
は、対数増幅器をメモリ40の前、厳密にはその
前に設けられているA/D変換器の前に配置しな
ければならない。
In this embodiment, the logarithmic amplifier is placed before the quadrature detector 24, but it can also be placed after the quadrature detector 24, as shown in FIG. 4c. Of course, the logarithmic amplifier has memory 40
It does not necessarily need to be placed in front of , and can be placed at any location before the synthetic addition operation based on the synthetic aperture method is performed. However, as will be described later, in order to reduce the capacity of the memory 40, the logarithmic amplifier must be placed before the memory 40, or more precisely before the A/D converter provided in front of it.

このようにして得られたホログラムは、A/D
変換器36,38にてA/D変換されメモリ40
に供給されて一旦記憶される。一般にA/D変換
器やデジタルメモリは入力信号の変動幅が大きい
ほど、A/D変換器のビツト数が多くなりメモリ
容量も大となる。しかし本発明に係る装置は、対
数増幅器22の使用により前述したホログラムの
振幅変動範囲が圧縮されており、信号記録あるい
は処理が容易となる。
The hologram obtained in this way is
A/D converted by converters 36 and 38 and stored in memory 40
is supplied to and temporarily stored. Generally, in an A/D converter or a digital memory, the larger the fluctuation range of the input signal, the larger the number of bits in the A/D converter and the larger the memory capacity. However, in the apparatus according to the present invention, the amplitude variation range of the hologram described above is compressed by using the logarithmic amplifier 22, and signal recording or processing becomes easy.

次に、メモリ40で記録されたホログラムは乗
算器42,44によつて前述した余弦波と正弦波
が再度乗算され、加算器46にて直交検波前の受
信波信号に再生される。該加算器46の出力は演
算器48に入力され、各振動子の受信信号を適当
に時間間隔移動させて加算演算すれば生体内の各
焦点における情報が得られ、生体内の断層像は画
像メモリ50を介してTVモニタ52に画像形成
される。
Next, the hologram recorded in the memory 40 is multiplied again by the above-mentioned cosine wave and sine wave by the multipliers 42 and 44, and reproduced by the adder 46 into a received wave signal before orthogonal detection. The output of the adder 46 is input to the arithmetic unit 48, and by moving the received signals of each transducer by an appropriate time interval and performing an addition operation, information at each focal point within the living body can be obtained, and the tomographic image inside the living body is an image. An image is formed on a TV monitor 52 via a memory 50.

また、各振動子に対応するメモリ40の領域の
内容を更新することを繰り返すように制御すると
常に最新のホログラムが記憶され、TVモニタ5
2には、更新された新しい情報に基づく断層像を
適宜画像表示することが可能となる。
Furthermore, by repeatedly updating the contents of the area of the memory 40 corresponding to each vibrator, the latest hologram is always stored, and the TV monitor 5
2, it becomes possible to appropriately display a tomographic image based on updated new information.

なお、本実施例においては、送受信号は同一振
動子によつて行つているが、送信した振動子と別
の振動子で超音波を受信させたり、一対の振動子
を機械的に走査させることによつても超音波の送
受信を行うことができ、また受信する超音波は生
体内からの反射波に限らず透過波であつても同じ
効果を得ることができる。
In this example, the transmitted and received signals are transmitted using the same transducer, but the ultrasonic wave may be received by a transducer different from the transducer that transmitted it, or a pair of transducers may be mechanically scanned. Ultrasonic waves can also be transmitted and received, and the same effect can be obtained even when the received ultrasonic waves are not only reflected waves from inside the living body but also transmitted waves.

[発明の効果] 以上説明したように、本発明によれば、各振動
子により受信した生体内の超音波透過波あるいは
反射波を非線形に増幅して記録しているので、合
成開口技術にて生体内の各焦点における像を合成
する際に生じるサイドローブが除去され、送受波
した生体の高精度な断層画像を得ることができ、
病気の診断に有益な情報を提供することが可能と
なる。
[Effects of the Invention] As explained above, according to the present invention, since the ultrasonic transmitted waves or reflected waves in the living body received by each transducer are nonlinearly amplified and recorded, synthetic aperture technology can be used to The side lobes that occur when combining images at each focal point within a living body are removed, making it possible to obtain highly accurate tomographic images of the living body through transmitted and received waves.
It becomes possible to provide information useful for diagnosing diseases.

また、対数増幅器を受波器とA/D変換器との
間に設けたので、A/D変換器のビツト数を減少
させても精度の高い受信情報を得ることができ、
加えて、メモリの容量を減少させることができ、
このようなことから迅速な受信信号の合成演算処
理が可能である。
Furthermore, since a logarithmic amplifier is provided between the receiver and the A/D converter, highly accurate reception information can be obtained even if the number of bits of the A/D converter is reduced.
In addition, memory capacity can be reduced,
Because of this, it is possible to quickly perform synthetic arithmetic processing on received signals.

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

第1図は合成開口法の説明図、第2図はサイド
ローブの説明図、第3図は本発明に係る超音波診
断装置の好適な実施例を示す説明図、第4図は対
数増幅器の配置の説明図である。 10……送受信器、12……配列振動子、18
……制御器、22……対数増幅器、40……メモ
リ、48……演算器、52……TVモニタ。
Fig. 1 is an explanatory diagram of the synthetic aperture method, Fig. 2 is an explanatory diagram of the side lobe, Fig. 3 is an explanatory diagram showing a preferred embodiment of the ultrasonic diagnostic apparatus according to the present invention, and Fig. 4 is an explanatory diagram of the logarithmic amplifier. It is an explanatory diagram of arrangement. 10...Transmitter/receiver, 12...Array transducer, 18
...Controller, 22...Logarithmic amplifier, 40...Memory, 48...Arithmetic unit, 52...TV monitor.

Claims (1)

【特許請求の範囲】 1 生体内に送波された超音波パルスが生体内を
透過した透過波又は前記生体内から反射した反射
波を受波する受波器と、 前記受波器からの受信信号をA/D変換する
A/D変換器と、 前記A/D変換された受信信号をその受信信号
ごとに格納するメモリと、 を含み、 前記メモリからそれぞれ前記受信信号を読み出
し、それぞれ位相を調整して合成加算演算し、生
体内の断層画像を形成する超音波診断装置におい
て、 前記受波器と前記A/D変換器との間には、 前記受波器からの受信信号をその受信信号ごと
に対数増幅する対数増幅器が設けられたことを特
徴とする超音波診断装置。
[Scope of Claims] 1. A receiver for receiving a transmitted wave transmitted through the living body or a reflected wave reflected from the living body by an ultrasonic pulse transmitted into the living body, and reception from the receiver. an A/D converter that A/D converts a signal; and a memory that stores the A/D converted received signal for each received signal, reads each of the received signals from the memory, and calculates the phase of each of the received signals. In an ultrasonic diagnostic apparatus that adjusts and performs synthesis and addition operations to form a tomographic image of an in-vivo body, between the wave receiver and the A/D converter, the reception signal from the wave receiver is connected to the receiver. An ultrasonic diagnostic device characterized by being provided with a logarithmic amplifier that logarithmically amplifies each signal.
JP6993685A 1985-04-04 1985-04-04 Ultrasonic diagnostic apparatus Granted JPS61228835A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6993685A JPS61228835A (en) 1985-04-04 1985-04-04 Ultrasonic diagnostic apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6993685A JPS61228835A (en) 1985-04-04 1985-04-04 Ultrasonic diagnostic apparatus

Publications (2)

Publication Number Publication Date
JPS61228835A JPS61228835A (en) 1986-10-13
JPH0259732B2 true JPH0259732B2 (en) 1990-12-13

Family

ID=13417045

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6993685A Granted JPS61228835A (en) 1985-04-04 1985-04-04 Ultrasonic diagnostic apparatus

Country Status (1)

Country Link
JP (1) JPS61228835A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63228288A (en) * 1987-03-17 1988-09-22 富士通株式会社 Automatic public funds processor
JP5473381B2 (en) * 2008-06-23 2014-04-16 キヤノン株式会社 Ultrasonic device

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59137040A (en) * 1983-01-28 1984-08-06 株式会社東芝 Opening synthesis method ultrasonic diagnostic apparatus
JPS6048736A (en) * 1983-08-29 1985-03-16 株式会社東芝 Ultrasonic diagnostic apparatus
JPS6080444A (en) * 1983-10-07 1985-05-08 富士通株式会社 Ultrasonic diagnostic apparatus
JPS61335A (en) * 1984-06-12 1986-01-06 富士通株式会社 Ultrasonic diagnostic apparatus

Also Published As

Publication number Publication date
JPS61228835A (en) 1986-10-13

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