JPS61186850A - Acoustic wave probe - Google Patents

Acoustic wave probe

Info

Publication number
JPS61186850A
JPS61186850A JP2626085A JP2626085A JPS61186850A JP S61186850 A JPS61186850 A JP S61186850A JP 2626085 A JP2626085 A JP 2626085A JP 2626085 A JP2626085 A JP 2626085A JP S61186850 A JPS61186850 A JP S61186850A
Authority
JP
Japan
Prior art keywords
lens
edge
sample
acoustic
acoustic 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.)
Pending
Application number
JP2626085A
Other languages
Japanese (ja)
Inventor
Koshi Umemoto
梅本 講司
Nobuyuki Nakajima
中島 暢之
Masao Takai
高井 正生
Katsuji Ikenaga
池永 勝次
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
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 Ltd filed Critical Hitachi Ltd
Priority to JP2626085A priority Critical patent/JPS61186850A/en
Publication of JPS61186850A publication Critical patent/JPS61186850A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N29/00Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object
    • G01N29/04Analysing solids
    • G01N29/06Visualisation of the interior, e.g. acoustic microscopy

Abstract

PURPOSE:To prevent deterioration in SN ratio and to obtain a sharp image by forming an acoustic wave used for an ultrasonic microscope concavely, and making the edge of the spherical surface acute. CONSTITUTION:The acoustic lens 1 has a concave spherical part 8 formed at an end surface side facing a sample. The edge 16 between the spherical surface part 8 and a slanting part 17 which starts right at the spherical surface part is finished acutely. Then, a pulse is applied to the piezoelectric element 2 of the acoustic wave lens 1 to oscillate an ultrasonic wave, which is made incident on the sample from the concave surface part 8; and a reflected wave from the sample is received and made into an image by a receiver. In this case, the edge 16 of the spherical surface part 8 of the acoustic wave lens is made acute to prevent a converged ultrasonic beam from striking on the acoustic lens except at a lens aperture part. Thus, multiple reflection in the lens is prevented, so deterioration in SN ratio is prevented and the image is made sharp.

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は、音波探触子に係り、特に超音波顕微鏡に使用
される音波探触子に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to a sonic probe, and particularly to a sonic probe used in an ultrasound microscope.

〔発明の背景〕[Background of the invention]

超音波顕微鏡に使用される音波探触子の音波レンズの球
面部の縁が平担であると、この部分からも超音波が媒質
中に漏洩、放射されて集束超音波ビームの信号か有効に
利用てきないためS/Nが劣化する。そこで、S/N劣
化防止のため音波レンズの球面部の縁に吸音材をはると
いったことも考案されている(実公昭58−31200
号公報)が、現実には周波数が高く、焦点距離が短かい
音波レンズになると吸音材と試料が接触するといった不
具合がある。
If the edge of the spherical part of the sonic lens of a sonic probe used in an ultrasound microscope is flat, ultrasound will leak into the medium from this part and be radiated, resulting in the signal of the focused ultrasound beam becoming effective. Since it is not used, the S/N deteriorates. Therefore, in order to prevent S/N deterioration, it has been devised to put a sound absorbing material on the edge of the spherical part of the sonic lens (Utility Model Publication No. 58-31200).
However, in reality, when using a sound wave lens with a high frequency and a short focal length, there is a problem that the sound absorbing material and the sample come into contact with each other.

〔発明の目的〕[Purpose of the invention]

本発明の目的は、音波レンズの球面部の縁に吸音材をは
ることなく、S/N劣化を防止し鮮明な画像を得ること
にあり、音波レンズ開口部以外からの超音波の不要輻射
がなく凹面体の半球穴部のみから超音波を吸音するよう
な音波探触子を提供することIこある。
The purpose of the present invention is to prevent S/N deterioration and obtain a clear image without putting a sound absorbing material on the edge of the spherical part of the sonic lens, and to prevent unnecessary radiation of ultrasonic waves from other than the aperture of the sonic lens. It is an object of the present invention to provide a sonic probe that absorbs ultrasonic waves only from the hemispherical hole of the concave body without any hemispherical holes.

〔発明の概要〕[Summary of the invention]

音波探触子は、それ自体が音波伝搬媒体としての役目を
果すことから、内外部の欠陥等がないようにすることは
もちろんであるが、寸法や仕上精度上も細心の注意を払
うことが必要である。しかし、通常の作業で音波レンズ
の凹面体の球面部の縁を鋭角に仕上げても、実際には縁
に丸みがあったり、平担部が残ったりし、50μm以上
が残るのが普通である。レンズ開口部以外に傾斜部を設
けることにより、集束超音波ビームの媒体への入射を阻
止すると共Iこ、レンズ内の多重反射を緩和しているが
、周波数が高くなれば減衰が大きいため、設計上、音波
レンズの球面部の曲率半径をQJmm以下にしなければ
ならない。しかし、こうした微小寸法に対し音波レンズ
の球面部の縁の平担部の割合が大きくなれば、集束超音
波ビームのS/Nが劣化し、鮮明な画像が得られないと
いったことを実験により確認している。本発明はこの音
波レンズの球面部の縁の残りをさらに小さくおさえるこ
とにより鮮明な画像を得ようとするものである。
Since the sonic probe itself serves as a sound wave propagation medium, it is necessary to ensure that there are no internal or external defects, but also to pay close attention to the dimensions and finishing accuracy. is necessary. However, even if the edges of the spherical part of the concave body of a sound wave lens are finished at an acute angle through normal work, in reality, the edges are rounded or flat, and it is normal for 50 μm or more to remain. . By providing a sloped portion other than the lens opening, the focused ultrasonic beam is prevented from entering the medium and multiple reflections within the lens are alleviated, but as the frequency increases, the attenuation increases. In design, the radius of curvature of the spherical portion of the acoustic lens must be equal to or less than QJmm. However, it has been confirmed through experiments that if the proportion of the flat edge of the spherical part of the acoustic lens increases in relation to these minute dimensions, the S/N of the focused ultrasound beam deteriorates, making it impossible to obtain a clear image. are doing. The present invention aims to obtain clear images by further reducing the remaining edge of the spherical portion of the acoustic wave lens.

〔発明の実施例〕[Embodiments of the invention]

以下、本発明の一実施例を第1図、第2図により説明す
る。第1図は超音波顕微鏡の主要構成部を示す図である
。超音波の集束及び送受は音波レンズ1により行なって
いるが、その構造は円柱状の溶融石英等をもちいた物質
の一面を光学研磨し、その上に圧電素子(znO等)2
を上部電極3と下部電極4によりはさむ、このようにサ
ンドインチ構造になっている圧電素子2に、パルス発振
器5から発生されたパルス6を印加して、超音波7を発
生させる。また、他端部は口径は0.1mmφへ13、
Qmmφ程度の凹面体の球面部8が形成されており、こ
の球面部8と試料9に伝播させるための媒質(たとえば
水)10が満たされている。
An embodiment of the present invention will be described below with reference to FIGS. 1 and 2. FIG. 1 is a diagram showing the main components of an ultrasound microscope. The focusing, transmission and reception of ultrasonic waves is carried out by a sonic lens 1, whose structure consists of optically polishing one side of a material made of cylindrical fused silica, etc., and placing a piezoelectric element (ZnO etc.) 2 on top of it.
A pulse 6 generated from a pulse oscillator 5 is applied to the piezoelectric element 2, which has a sandwich structure in which the piezoelectric element 2 is sandwiched between an upper electrode 3 and a lower electrode 4, to generate an ultrasonic wave 7. In addition, the diameter of the other end is 0.1 mmφ13,
A concave spherical part 8 of approximately Qmmφ is formed, and is filled with a medium (for example, water) 10 for propagating the light to the spherical part 8 and the sample 9.

圧電素子2によって発生した超音波7は円柱の中を平面
波となって伝播する。この平面波が球面部8に達すると
石英(音速6ooom/s)と水(音速1500m/s
)との音速の差により屈折作用が生じ、試料9面上に集
束した超音波7を照射することができる。逆に、試料9
から反射されてくる超音波は音波レンズ1により集音整
相され、平面波となって圧電素子2に達し、ここでRF
信号11に変換される。このRF信号11を受信器12
で受信し、ここでダイオード検波してビデオ信号13に
変換し、CRTディスプレイ14の入力信号として用い
ている。
The ultrasonic wave 7 generated by the piezoelectric element 2 propagates in the cylinder as a plane wave. When this plane wave reaches the spherical surface part 8, quartz (sound velocity 6ooom/s) and water (sound velocity 1500m/s
), a refraction effect occurs due to the difference in sound speed between the sample 9 and the sample 9, and the focused ultrasonic waves 7 can be irradiated onto the surface of the sample 9. On the contrary, sample 9
The ultrasonic waves reflected from the
It is converted into signal 11. This RF signal 11 is transmitted to the receiver 12
The video signal is received by a video signal 13, which is diode-detected and converted into a video signal 13, which is used as an input signal for a CRT display 14.

上記のように構成された装置において試料9が試料台駆
動電源15によりX−Y平面内で2次元に走査している
試料の走査にともなう試料面からの反射の強弱が2次元
的にCRT面14に表示される。以上述べた基本構成に
より超音波顕微像が得られる。第4図は本発明の音波レ
ンズの断面図である。傾斜部17は凹面体の球面部8か
らすぐに始まり、縁16は鋭角に仕上げてあり、球面部
8の曲率半径が0.1.mm壓ので、縁16の平担部寸
法が20μm以下となるように仕上げたものである。音
波レンズは周波数により、球面部8の曲率半径を幾通り
かに分けて使用しており、縁16の平担部寸法が異なれ
ば当然、各周波数ごとにS/N劣化も違もてくる。従っ
て周波数50MH2〜IGH2の音波レンズにおいては
縁16の平担部を50μm〜20μmにおさえるように
鋭角にしだものである。このように、音波レンズの球面
部の縁を鋭角に仕上げることにより、レンズ開口部以外
からの超音波の不要輻射がなく、凹面体の球面部のみか
ら超音波が発射され、凹面体の球面部のみから超音波を
吸音するようにし、集束超音波ビームのS/Nの劣化を
防止することができる。従って、音波レンズの球面部の
縁に吸音材をはる必要がないので、周波数が高く、焦点
距離が短かい場合にも特に不具合を生じない。
In the apparatus configured as described above, the sample 9 is scanned two-dimensionally within the X-Y plane by the sample stage drive power supply 15.The intensity of reflection from the sample surface as the sample is scanned is two-dimensionally reflected from the CRT surface. 14. An ultrasonic microscopic image can be obtained with the basic configuration described above. FIG. 4 is a sectional view of the acoustic lens of the present invention. The slope 17 starts immediately from the spherical part 8 of the concave body, the edge 16 is finished at an acute angle, and the radius of curvature of the spherical part 8 is 0.1. mm diameter, so the flat portion of the edge 16 is finished to have a dimension of 20 μm or less. The acoustic lens uses several different radii of curvatures of the spherical portion 8 depending on the frequency, and if the dimensions of the flat portion of the edge 16 differ, the S/N deterioration will naturally differ for each frequency. Therefore, in a sound wave lens having a frequency of 50 MH2 to IGH2, the flat portion of the edge 16 is formed at an acute angle so as to be limited to 50 μm to 20 μm. In this way, by finishing the edges of the spherical part of the sonic lens with an acute angle, there is no unnecessary radiation of ultrasonic waves from other than the lens opening, and the ultrasonic waves are emitted only from the spherical part of the concave body. By absorbing ultrasonic waves from only the ultrasonic beam, it is possible to prevent deterioration of the S/N of the focused ultrasonic beam. Therefore, since there is no need to apply sound absorbing material to the edge of the spherical portion of the acoustic wave lens, no particular problem occurs even when the frequency is high and the focal length is short.

〔発明の効果〕〔Effect of the invention〕

本発明は、以上説明したように、音波レンズの球面部の
縁を鋭角に仕上げることでレンズ開口部以外Iこ集束超
音波ビームの媒体への入射を阻止すると共にレンズ内の
多重反射を防止できるので、音波レンズの球面部の縁に
吸音材をはることなく集束超音波ビームのS/Nの劣化
を防止でき鮮明な画像を得ることができるという効果が
ある。
As explained above, the present invention makes it possible to prevent the focused ultrasonic beam from entering the medium other than the lens opening by finishing the edge of the spherical part of the acoustic lens with an acute angle, and also to prevent multiple reflections within the lens. Therefore, it is possible to prevent deterioration of the S/N of the focused ultrasonic beam and obtain a clear image without applying a sound absorbing material to the edge of the spherical portion of the acoustic lens.

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

第1図は、本発明による音波探触子の一実施例を示すも
ので、本発明による音波探触子を用いた超音波顕微鏡の
構成図、第2図は、第1図の音波探触子の音波レンズの
縦断面図である。
FIG. 1 shows an embodiment of the sonic probe according to the present invention, and FIG. 2 is a block diagram of an ultrasound microscope using the sonic probe according to the present invention. FIG. 3 is a longitudinal cross-sectional view of a second acoustic lens.

Claims (1)

【特許請求の範囲】[Claims] 1、音波伝搬媒体の一端面に凹面球状に形成された音波
レンズを有し、該音波レンズの球面部の縁を鋭角にした
ことを特徴とする音波探触子。
1. A sonic probe characterized in that it has a sonic lens formed into a concave spherical shape on one end surface of a sonic wave propagation medium, and the edge of the spherical portion of the sonic lens has an acute angle.
JP2626085A 1985-02-15 1985-02-15 Acoustic wave probe Pending JPS61186850A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2626085A JPS61186850A (en) 1985-02-15 1985-02-15 Acoustic wave probe

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2626085A JPS61186850A (en) 1985-02-15 1985-02-15 Acoustic wave probe

Publications (1)

Publication Number Publication Date
JPS61186850A true JPS61186850A (en) 1986-08-20

Family

ID=12188294

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2626085A Pending JPS61186850A (en) 1985-02-15 1985-02-15 Acoustic wave probe

Country Status (1)

Country Link
JP (1) JPS61186850A (en)

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