JPH0219762A - Sample surface inclination adjusting device for ultrasonic microscope - Google Patents
Sample surface inclination adjusting device for ultrasonic microscopeInfo
- Publication number
- JPH0219762A JPH0219762A JP63169595A JP16959588A JPH0219762A JP H0219762 A JPH0219762 A JP H0219762A JP 63169595 A JP63169595 A JP 63169595A JP 16959588 A JP16959588 A JP 16959588A JP H0219762 A JPH0219762 A JP H0219762A
- Authority
- JP
- Japan
- Prior art keywords
- sample
- ultrasonic
- sample surface
- inclination
- transducer
- 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
Links
Landscapes
- Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
Abstract
Description
この発明は、試料表面に超音波ビームを照射し、得られ
た反射波から試料物質の性質を観察する超音波顕微鏡に
関し、特に超音波ビームの焦点走査平面と試料表面とを
平行に設定するための超音波顕微鏡の試料面傾斜調整装
置に関する。The present invention relates to an ultrasonic microscope that irradiates an ultrasonic beam onto the surface of a sample and observes the properties of the sample substance from the reflected waves obtained, and in particular, the invention relates to an ultrasonic microscope that irradiates the surface of a sample with an ultrasonic beam and observes the properties of the sample substance from the reflected waves obtained. This invention relates to a sample surface tilt adjustment device for an ultrasonic microscope.
従来のこの種の試料面傾斜調整装置として、試料表面を
超音波ビームで走査することにより、前記試料表面上の
複数箇所における超音波受信信号の基準時刻からの時間
遅れをそれぞれ検出し、それらの値が等しくなるように
試料保持台の傾斜を調整するものが知られている。
第3図はこのような試料面傾斜調整装置のシステムブロ
ック図を示すものである。第3図において、制御部1が
発生する一定周期のパルス信号によって制御される高周
波パルス発振器2の出力は、サーキュレータ3を通して
、圧電素子4aと音響レンズ4bとからなる送受波用超
音波トランスジューサ(以下、単にトランスジューサと
いう。)4に加えられ、超音波ビームを発生させる。こ
の超音波ビームは、音響媒体5の中を伝搬して試料6に
入射し反射波を発生させるが、この反射波は再びトラン
スジューサ4を通って電気信号に変換され、サーキュレ
ータ3を経て受信部7に受信される。遅れ時間検出部9
は、受信部7からの受信検波信号を制御部1からのパル
ス信号を基準にして送波からの時間遅れに対応したアナ
ログ信号に変換する。
一方、制御部1によりタイミング制御される走査部8は
トランスジューサ4を図示X方向に移動させ、超音波ビ
ームにより試料表面を走査させる。
そこで、試料表面の異なる2点での反射波の時間遅れに
対応する上記アナログ信号が遅れ時間検出部9から同時
に差動増幅器10に送られる。この差動増幅器10の出
力は傾斜調整機構11に送られ、この傾斜調整機構11
により試料保持台12のX方向についての傾斜が差動増
幅器10の出力が零になるように自動調整される。次い
で、試料保持台12を手動操作により90度回転させて
同様に傾斜が調整され、XY平面での傾斜の調整が完了
する。As a conventional sample surface tilt adjustment device of this type, by scanning the sample surface with an ultrasonic beam, the time delays of the ultrasonic reception signals from the reference time at multiple locations on the sample surface are detected, and the time delays are detected. A method is known in which the inclination of the sample holder is adjusted so that the values become equal. FIG. 3 shows a system block diagram of such a sample surface tilt adjustment device. In FIG. 3, the output of a high-frequency pulse oscillator 2 controlled by a pulse signal of a constant period generated by a control unit 1 is transmitted through a circulator 3 to an ultrasonic transducer for transmitting and receiving waves (hereinafter referred to as "wave transmitting/receiving ultrasonic transducer") consisting of a piezoelectric element 4a and an acoustic lens 4b. , simply referred to as a transducer) 4 to generate an ultrasound beam. This ultrasonic beam propagates through the acoustic medium 5 and enters the sample 6 to generate a reflected wave, but this reflected wave passes through the transducer 4 again and is converted into an electric signal, passes through the circulator 3, and then passes through the receiving section 7. will be received. Delay time detection section 9
converts the received detection signal from the receiving section 7 into an analog signal corresponding to the time delay from transmission using the pulse signal from the control section 1 as a reference. On the other hand, the scanning section 8 whose timing is controlled by the control section 1 moves the transducer 4 in the X direction shown in the figure to scan the sample surface with an ultrasonic beam. Therefore, the analog signals corresponding to the time delays of the reflected waves at two different points on the sample surface are simultaneously sent from the delay time detection section 9 to the differential amplifier 10. The output of this differential amplifier 10 is sent to a slope adjustment mechanism 11, and this slope adjustment mechanism 11
Accordingly, the inclination of the sample holding table 12 in the X direction is automatically adjusted so that the output of the differential amplifier 10 becomes zero. Next, the sample holding table 12 is manually rotated 90 degrees to adjust the inclination in the same manner, thereby completing the adjustment of the inclination in the XY plane.
ところが、このような従来の試料面傾斜調整装置には次
のような欠点があった。
(1) 上記従来装置は、トランスジューサの音響レ
ンズと試料表面との間の距離の変化を受信検波信号の到
達時間の変化で検出するものであるが、集束超音波レン
ズの場合はこの距離の変化による受信検波信号の振幅変
化が大きく、試料表面が超音波ビーム焦点面から少しず
れただけでも振幅が著しく小さ(なり検出が困難となる
。例えば、200M七の高周波パルス信号の場合、試料
表面が10μm焦点面からずれるだけで、試料によって
は20dB以上も受信検波信号の振幅が落ちる。
(2)使用する超音波パルス幅に対する受信検波信号の
到達時間の変化幅の比は、音響レンズと試料表面との間
の距離が1波長分変化したとすると約l/20で、この
程度の到達時間の変化では検出がなかなか困難である。
すなわち、従来装置では試料面の傾斜に伴う信号の検出
レベルが低く、例えば干渉縞が1本も生じないように試
料面の傾斜を精密に調整することは困難であった。
この発明は、上記到達時間の変化によることなく別の手
段を講じ、超音波ビームの焦点走査面と試料表面との平
行度をより精度良く調整できるようにした超音波顕微鏡
の試料面傾斜調整装置を提供することを目的とするもの
である。However, such conventional sample surface tilt adjustment devices have the following drawbacks. (1) The conventional device described above detects changes in the distance between the acoustic lens of the transducer and the sample surface based on changes in the arrival time of the received detection signal, but in the case of a focused ultrasonic lens, changes in the distance The amplitude change of the received detection signal is large, and even if the sample surface deviates even slightly from the ultrasonic beam focal plane, the amplitude becomes extremely small (and detection becomes difficult. For example, in the case of a 200M7 high-frequency pulse signal, if the sample surface A shift of just 10 μm from the focal plane will reduce the amplitude of the received detection signal by more than 20 dB depending on the sample. (2) The ratio of the change width of the arrival time of the received detection signal to the ultrasonic pulse width used is the difference between the acoustic lens and the sample surface. If the distance between the sample surface and the sample surface changes by one wavelength, it is approximately 1/20, and detection is quite difficult with such a change in arrival time. For example, it has been difficult to precisely adjust the inclination of the sample surface so that no interference fringes occur.This invention takes other measures without depending on the above-mentioned change in arrival time, and the ultrasonic beam It is an object of the present invention to provide a sample surface tilt adjustment device for an ultrasonic microscope that can adjust the parallelism between the focal scanning plane and the sample surface with higher precision.
上記目的を達成するために、この発明は、送受波用超音
波トランスジューサからの超音波ビームの焦点走査平面
と試料表面とを平行に設定するための超音波顕微鏡の試
料面傾斜調整装置において、送受波用超音波トランスジ
ューサからの超音波ビームで試料表面を一方向に直線的
に走査させる走査部と、走査中における前記試料表面の
各点での超音波受信信号値とこれらの中の最大値との差
を積分して出力する検出部とを備えるものとする。In order to achieve the above object, the present invention provides a sample surface tilt adjustment device for an ultrasound microscope for setting the focal scanning plane of an ultrasonic beam from an ultrasonic transducer for transmitting and receiving waves parallel to the sample surface. a scanning unit that linearly scans a sample surface in one direction with an ultrasonic beam from an ultrasonic wave transducer; and an ultrasonic reception signal value at each point on the sample surface during scanning and a maximum value among these; and a detection unit that integrates and outputs the difference between the two.
超音波ビームで試料表面を一方向に直線的に走査したと
きの試料表面の各点での超音波受信信号値とこれらの中
の最大値との差を積分したものを試料面の傾斜信号とす
ることにより、試料面の傾斜を超音波受信信号の変化と
して直接検出することができる。そして、この傾斜信号
値が零値を示すように試料保持台あるいはトランスジュ
ーサの傾斜を調整することによって、超音波ビームの焦
点走査面と試料表面との平行度を容易に精度良(調整す
ることができる。When the sample surface is linearly scanned in one direction with an ultrasonic beam, the difference between the ultrasonic reception signal value at each point on the sample surface and the maximum value among these values is integrated, and the result is called the sample surface tilt signal. By doing so, the inclination of the sample surface can be directly detected as a change in the ultrasonic reception signal. By adjusting the inclination of the sample holder or transducer so that this inclination signal value shows a zero value, the parallelism between the focal scanning plane of the ultrasonic beam and the sample surface can be easily adjusted with high precision. can.
【実施例]
第1図はこの発明の実施例のシステムブロック図を示す
ものである。第1図において、1は一定周期のパルス信
号によりタイミング制御を行う制御部、2は高周波パル
ス発振器、3はサーキュレータ、4は圧電素子4a及び
音響レンズ4bとからなるトランスジューサ、5は音響
媒体、6は試料、12は試料保持台で、これらは第3図
の従来装置におけるものと本質的に同じものである。
13はトランスジューサ4からの超音波ビームで試料6
の表面を一方向(図示X方向)に直線的に走査させる走
査部である。また、14は反射波の電気信号を受信して
増幅検波する受信SH回路、15は標準電圧発生器、1
6は差動増幅器、17は積分回路で、これらは走査中に
おける試料表面の各点での超音波受信信号値とこれらの
中の最大値との差を積分して出力する検出部を構成する
ものである。さらに、18は積分回路17からの出力を
表示する表示装置である。
このような構成において、まず、走査をしない状態で試
料保持台12を図示X方向に移動させ、試料6の表面を
音響レンズ4bの焦点走査平面に設定する。このとき、
受信S H回路14の超音波受信信号は最大となる。そ
の状態で走査部13によりトランスジューサ4をX方向
に直線的に移動させると、試料6の表面が音響レンズ4
aの焦点走査平面と平行でない場合は、試料6の表面の
一方の側は音響レンズ4bに近づき、他方の側は逆に遠
ざかる。したがって、受信38回路14に受信される超
音波受信信号は、試料6の両端に近い点におけるものほ
ど音響レンズ4bの焦点走査平面から外れた信号となり
低い値となる。
そこで、走査をしない状態、すなわら、試料6の表面を
音響レンズ4bの焦点走査平面に設定した状態での標〈
桿電圧発生器15の出力をそのときの受信38回路14
の超音波受信信号と等しくなるように設定しておき、試
料表面をX方向に直線的に走査すれば、差動増幅器16
の出力は超音波受信信号が試料6の端部に近い点におけ
るものほど、また試料表面の平行度が悪いほど大きくな
る。
この差動増幅器16の出力は、走査部13によるX方向
の走査周期でリセットされる積分回路17に入力され、
その出力は表示装置1日に入力される。
したがって、表示装置18の表示が小さくなるように手
動で試料保持台12のX方向の傾斜を調整することによ
り、X方向での焦点走査面と試料表面との平行度を調整
することができる。X方向については、試料保持台12
を90度面回転せ同様にして調整する。
第2図はこの発明の別の実施例のシステムブロック図で
ある。この実施例と第1図の実施例との相違は、傾斜調
整機構19を設け、試料保持台12の傾斜を自動調整す
るようにした点である。すなわち、第2図においては制
御部lに傾斜調整機構19の制御機能を付加し、この制
御部1に積分回路17の出力を入力し、この積分回路1
7の出力が最も小さい値になるように傾斜調整機構19
を制御し、試料保持台12の傾斜調整を自動化したもの
である。
【発明の効果】
この発明によれば、超音波ビームの焦点走査平面と試料
表面との平行度を超音波受信信号の強度変化として直接
検出し、試料表面の各点での検出値を積分して出力する
ようにしたので、信号レベルが試料表面の傾斜を受信検
波信号の到達時間の変化で検出する場合に比べて格段に
大きくなる。
したがって、試料表面の微細なずれも確実に検出するこ
とができ、この検出信号値が零値を示すように試料保持
台を調整することにより試料を容易に精度良く設定する
ことができる。Embodiment FIG. 1 shows a system block diagram of an embodiment of the present invention. In FIG. 1, 1 is a control unit that performs timing control using pulse signals of a constant period, 2 is a high-frequency pulse oscillator, 3 is a circulator, 4 is a transducer consisting of a piezoelectric element 4a and an acoustic lens 4b, 5 is an acoustic medium, and 6 1 is a sample, and 12 is a sample holder, which are essentially the same as those in the conventional apparatus shown in FIG. 13 is the ultrasonic beam from the transducer 4 that
This is a scanning unit that linearly scans the surface of the camera in one direction (X direction in the drawing). Further, 14 is a receiving SH circuit that receives and amplifies and detects the electrical signal of the reflected wave, 15 is a standard voltage generator, and 1
6 is a differential amplifier, and 17 is an integration circuit, which constitute a detection unit that integrates and outputs the difference between the ultrasonic reception signal value at each point on the sample surface during scanning and the maximum value among them. It is something. Furthermore, 18 is a display device that displays the output from the integrating circuit 17. In such a configuration, first, the sample holding table 12 is moved in the X direction in the figure without scanning, and the surface of the sample 6 is set at the focal scanning plane of the acoustic lens 4b. At this time,
The ultrasonic reception signal of the reception SH circuit 14 becomes maximum. In this state, when the transducer 4 is moved linearly in the X direction by the scanning unit 13, the surface of the sample 6 is
If it is not parallel to the focal scanning plane of a, one side of the surface of the sample 6 approaches the acoustic lens 4b, and the other side moves away from it. Therefore, the ultrasonic reception signal received by the receiver 38 circuit 14 at a point closer to both ends of the sample 6 is a signal farther from the focal scanning plane of the acoustic lens 4b and has a lower value. Therefore, the target <
The output of the rod voltage generator 15 is sent to the receiving 38 circuit 14 at that time.
If the sample surface is scanned linearly in the X direction, the differential amplifier 16
The output becomes larger as the ultrasonic reception signal is closer to the edge of the sample 6 and as the parallelism of the sample surface becomes worse. The output of this differential amplifier 16 is input to an integrating circuit 17 that is reset at the scanning period in the X direction by the scanning section 13.
Its output is input to the display device 1. Therefore, by manually adjusting the inclination of the sample holder 12 in the X direction so that the display on the display device 18 becomes smaller, the parallelism between the focal scanning plane and the sample surface in the X direction can be adjusted. For the X direction, the sample holding table 12
Rotate the plane by 90 degrees and adjust in the same way. FIG. 2 is a system block diagram of another embodiment of the invention. The difference between this embodiment and the embodiment shown in FIG. 1 is that a tilt adjustment mechanism 19 is provided to automatically adjust the tilt of the sample holding table 12. That is, in FIG. 2, the control function of the inclination adjustment mechanism 19 is added to the control section 1, and the output of the integrating circuit 17 is inputted to the control section 1.
Tilt adjustment mechanism 19 so that the output of 7 becomes the smallest value.
The tilt adjustment of the sample holding table 12 is automated. [Effects of the Invention] According to the present invention, the parallelism between the focal scanning plane of the ultrasound beam and the sample surface is directly detected as a change in the intensity of the ultrasound reception signal, and the detected values at each point on the sample surface are integrated. Therefore, the signal level is much higher than that in the case where the slope of the sample surface is detected by a change in the arrival time of the received detection signal. Therefore, even minute deviations on the sample surface can be reliably detected, and by adjusting the sample holder so that this detection signal value shows a zero value, the sample can be easily set with high precision.
第1図はこの発明の実施例のシステムブロック図、第2
図はこの発明の別の実施例のシステムブロック図、第3
図は従来装置のシステムブ「1ツク図である。
■・・・制御部、2・・・高周波パルス発振器、3・・
・サーキュレータ、4・・・送受波用超音波トランスジ
ューサ、5・・・音響媒体、6・・・試料、12・・・
試料保持台、13・・・走査部、14・・・受信38回
路、15・・・標準電圧発生器、16・・・差動増幅器
、17・・・積分回路、18・・・表示装置、19・・
・傾斜調整機構。Figure 1 is a system block diagram of an embodiment of this invention, Figure 2 is a system block diagram of an embodiment of this invention.
Figure 3 is a system block diagram of another embodiment of this invention.
The figure is a system block diagram of a conventional device. ■...Control unit, 2...High frequency pulse oscillator, 3...
・Circulator, 4... Ultrasonic transducer for transmitting and receiving waves, 5... Acoustic medium, 6... Sample, 12...
Sample holding table, 13... Scanning section, 14... 38 receiving circuits, 15... Standard voltage generator, 16... Differential amplifier, 17... Integrating circuit, 18... Display device, 19...
・Tilt adjustment mechanism.
Claims (1)
ムの焦点走査平面と試料表面とを平行に設定するための
超音波顕微鏡の試料面傾斜調整装置において、送受波用
超音波トランスジューサからの超音波ビームで試料表面
を一方向に直線的に走査させる走査部と、走査中におけ
る前記試料表面の各点での超音波受信信号値とこれらの
中の最大値との差を積分して出力する検出部とを備える
ことを特徴とする超音波顕微鏡の試料面傾斜調整装置。1) In the specimen surface tilt adjustment device of an ultrasound microscope for setting the focal scanning plane of the ultrasonic beam from the ultrasonic transducer for transmitting and receiving parallel to the sample surface, the ultrasonic beam from the ultrasonic transducer for transmitting and receiving a scanning unit that linearly scans the sample surface in one direction; and a detection unit that integrates and outputs the difference between the ultrasonic reception signal value at each point on the sample surface during scanning and the maximum value among these values. A sample surface tilt adjustment device for an ultrasonic microscope, comprising:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63169595A JPH0219762A (en) | 1988-07-07 | 1988-07-07 | Sample surface inclination adjusting device for ultrasonic microscope |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63169595A JPH0219762A (en) | 1988-07-07 | 1988-07-07 | Sample surface inclination adjusting device for ultrasonic microscope |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0219762A true JPH0219762A (en) | 1990-01-23 |
Family
ID=15889401
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63169595A Pending JPH0219762A (en) | 1988-07-07 | 1988-07-07 | Sample surface inclination adjusting device for ultrasonic microscope |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0219762A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102419439A (en) * | 2011-08-18 | 2012-04-18 | 上海华碧检测技术有限公司 | Method for judging inclination of plastic package element chip |
-
1988
- 1988-07-07 JP JP63169595A patent/JPH0219762A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102419439A (en) * | 2011-08-18 | 2012-04-18 | 上海华碧检测技术有限公司 | Method for judging inclination of plastic package element chip |
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