JPH0678399A - Composite piezoelectric body - Google Patents

Composite piezoelectric body

Info

Publication number
JPH0678399A
JPH0678399A JP22687192A JP22687192A JPH0678399A JP H0678399 A JPH0678399 A JP H0678399A JP 22687192 A JP22687192 A JP 22687192A JP 22687192 A JP22687192 A JP 22687192A JP H0678399 A JPH0678399 A JP H0678399A
Authority
JP
Japan
Prior art keywords
piezoelectric body
composite piezoelectric
composite
thickness
elements
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.)
Granted
Application number
JP22687192A
Other languages
Japanese (ja)
Other versions
JP2682342B2 (en
Inventor
Takayoshi Saito
孝悦 斉藤
Fusako Kikuchi
総子 菊地
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP22687192A priority Critical patent/JP2682342B2/en
Publication of JPH0678399A publication Critical patent/JPH0678399A/en
Application granted granted Critical
Publication of JP2682342B2 publication Critical patent/JP2682342B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Transducers For Ultrasonic Waves (AREA)

Abstract

PURPOSE:To obtain the composite piezoelectric body having a broad band frequency characteristic used for a sonar or an ultrasonic wave diagnostic device or the like. CONSTITUTION:In the composite piezoelectric body 11 in which lots of rod shaped piezoelectric elements 12 set vertically are arranged and an organic high polymer material 13 is packed in a gap between the piezoelectric elements 12, the thickness of the composite piezoelectric body 11 is ununiformized, and the thickness of the piezoelectric element 12 and the interval between adjacent piezoelectric elements 12 are set to be proportional to the thickness of the composite piezoelectric body 11, that is, the length of the piezoelectric elements 12. Thus, the vibration in the frequency mode corresponding to each thickness is generated and the composite piezoelectric body having a broad frequency band is obtained.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、ソナーや超音波診断装
置などのセンサとして用いる超音波探触子の複合圧電体
に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a composite piezoelectric body for an ultrasonic probe used as a sensor for a sonar or an ultrasonic diagnostic apparatus.

【0002】[0002]

【従来の技術】水や生体を対象とするソナーや超音波診
断装置などの超音波探触子に用いる圧電体の材料とし
て、最近、柱状の圧電セラミックスを多数配列し、間隙
に高分子材を充填したいわゆる1−3形複合圧電体の検
討が行われている。このような複合圧電体としては、Pr
o.IEEE,1985,U1trasonics Symp.p643〜647に記載のもの
がある。
2. Description of the Related Art Recently, a large number of columnar piezoelectric ceramics are arranged as a material for a piezoelectric body used in ultrasonic probes such as sonars and ultrasonic diagnostic devices for water and living bodies, and polymer materials are used in the gaps. A so-called 1-3 type composite piezoelectric material filled with the material has been studied. As such a composite piezoelectric material, Pr
o. IEEE, 1985, U1trasonics Symp. p643 to 647.

【0003】図3は従来の複合圧電体の構成を示す斜視
図である。図3に示すように一次元の形状を有する柱状
の圧電セラミックス2と圧電セラミックス2の間隙に三
次元的に設けた高分子材3とで複合圧電体1を構成し、
厚さを均一にしたものである。この複合圧電体は音響イ
ンピーダンスを小さくし、より被検体(生体の音響イン
ピーダンスは約1.6MRay1)の音響インピーダン
スに近付けることができ、しかも電気機械結合係数も大
きい値を有していることにより、効率良くかつ広帯域の
周波数特性を得ることができるため、高分解能の超音波
断層像を得ることが可能であるという特徴を有したもの
であった。
FIG. 3 is a perspective view showing the structure of a conventional composite piezoelectric body. As shown in FIG. 3, a composite piezoelectric body 1 is composed of a columnar piezoelectric ceramic 2 having a one-dimensional shape and a polymer material 3 three-dimensionally provided in a gap between the piezoelectric ceramics 2.
It has a uniform thickness. This composite piezoelectric body has a small acoustic impedance, and can be brought closer to the acoustic impedance of the subject (acoustic impedance of the living body is about 1.6 MRay1), and also has a large electromechanical coupling coefficient. Since it was possible to efficiently obtain frequency characteristics in a wide band, it was possible to obtain a high-resolution ultrasonic tomographic image.

【0004】[0004]

【発明が解決しようとする課題】しかしながら、このよ
うな従来の複合圧電体では、圧電セラミックス単体から
なるものに比べて広い周波数帯域特性が得られるもの
の、まだ十分な周波数特性を得ることはできていなかっ
た。
However, with such a conventional composite piezoelectric body, although a wider frequency band characteristic can be obtained as compared with a piezoelectric ceramic single body, it is still possible to obtain a sufficient frequency characteristic. There wasn't.

【0005】本発明は、このような従来の問題を解決す
るものであり、さらに一層の広帯域周波数特性を有する
優れた複合圧電体を提供することを目的とする。
The present invention solves such conventional problems, and an object of the present invention is to provide an excellent composite piezoelectric body having further wide band frequency characteristics.

【0006】[0006]

【課題を解決するための手段】上記目的を達成するため
に本発明は、縦断面形状の相似な棒状の形態を有する多
数の圧電素子と前記圧電素子の間隙に充填された有機高
分子材とを備えた複合圧電体において、厚さを不均一と
し、それぞれの厚さに対応した周波数の振動モードを発
生することができる構成にしたものである。
In order to achieve the above object, the present invention provides a large number of piezoelectric elements having a rod-like shape having a similar vertical cross section and an organic polymer material filled in the gaps between the piezoelectric elements. In the composite piezoelectric body including the above, the thickness is made non-uniform and a vibration mode having a frequency corresponding to each thickness can be generated.

【0007】[0007]

【作用】本発明は上記構成により、複合圧電体の部分に
それぞれの厚みに対応した周波数の振動モードが発生す
るため、広い周波数帯域を有する特性を得ることができ
る。したがって、本発明の複合圧電体を用いた超音波探
触子は、極めて短いパルス応答波形を得ることができる
ため、被検深度が深く、かつ分解能の高い超音波画像を
得ることができる。
According to the present invention, with the above structure, vibration modes having frequencies corresponding to respective thicknesses are generated in the portion of the composite piezoelectric body, so that a characteristic having a wide frequency band can be obtained. Therefore, since the ultrasonic probe using the composite piezoelectric body of the present invention can obtain an extremely short pulse response waveform, it is possible to obtain an ultrasonic image with a deep test depth and high resolution.

【0008】[0008]

【実施例】以下本発明の一実施例について図面を参照な
しがら説明する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to the drawings.

【0009】図1は、本発明の一実施例の複合圧電体の
断面図である。また図2は、本発明の一実施例の複合圧
電体の圧電素子の幅と長さ(複合圧電体の厚さ)の形状
比と電気機械結合係数の関係を示す図である。
FIG. 1 is a sectional view of a composite piezoelectric body according to an embodiment of the present invention. FIG. 2 is a diagram showing the relationship between the shape ratio of the width and length (thickness of the composite piezoelectric body) of the piezoelectric element of the composite piezoelectric body of one embodiment of the present invention and the electromechanical coupling coefficient.

【0010】図1において、11は複合圧電体であり、
一方の面は平坦であり、他方の面は凹面形状である。1
2は棒状をした複数個の圧電素子であり、PZT系,P
bTiO3系などの圧電セラミックスやLiNbO3等の
単結晶が使用される。13はこれら圧電素子12の間隙
に三次元的に充填されてこれらを互いに結合する有機高
分子材であり、例えばシリコーンゴム,エポキシ樹脂あ
るいはウレタン樹脂などが使用される。14,15は複
合圧電体11の両面に設けられた電極であり、メッキ,
蒸着,あるいは焼付けなどの方法により設けられる。な
おここでは図示していないが必要に応じて複合圧電体1
1の電極14面上に背面負荷材を設け、さらに複合圧電
体11の電極15面上には音響整合層もしくは保護膜の
ようなものを設けてもよい。そしてこれら電極14,1
5に電圧を印加することにより複合圧電体11が機械振
動してそれぞれの厚さに対応した周波数の超音波を発生
させる。
In FIG. 1, 11 is a composite piezoelectric body,
One surface is flat and the other surface is concave. 1
Reference numeral 2 denotes a plurality of rod-shaped piezoelectric elements, which are PZT system, P
Piezoelectric ceramics such as bTiO 3 system and single crystals such as LiNbO 3 are used. Reference numeral 13 is an organic polymer material which three-dimensionally fills the gaps between the piezoelectric elements 12 and bonds them together, and for example, silicone rubber, epoxy resin or urethane resin is used. Electrodes 14 and 15 are provided on both surfaces of the composite piezoelectric body 11, which are plated,
It is provided by a method such as vapor deposition or baking. Although not shown here, the composite piezoelectric body 1 may be used if necessary.
A back load material may be provided on the surface of the first electrode 14 and an acoustic matching layer or a protective film may be provided on the surface of the electrode 15 of the composite piezoelectric body 11. And these electrodes 14, 1
When a voltage is applied to 5, the composite piezoelectric body 11 mechanically vibrates to generate an ultrasonic wave having a frequency corresponding to each thickness.

【0011】以下具体例を用いて説明する。圧電素子1
2の幅wと長さ(複合圧電体11の厚さ)tとの形状比
(w/t)により、複合圧電体11の電気機械結合係数
kは、図2に示すような関係がある。図2は圧電素子1
2として富士セラミックス社のPZT系圧電セラミック
スC−6、有機高分子材13としてエポキシ樹脂を用い
て、圧電素子12の複合圧電体11に対する体積比率を
約25%としたときの形状比(w/t)と電気機械結合
係数kとの関係を示したものである。図2の関係から明
らかなように複合圧電体11の圧電素子12の形状比に
よって電気機械係合係数kが変化することがわかる。こ
のことは図1に示したように複合圧電体11に不均一な
厚さを持たせ、かつ従来のように圧電素子12を同じ間
隔で配列した場合、厚みの薄い部分(図では中央付近)
と厚い部分(図では外周部分)とでは圧電素子12の形
状比が大きく変化する。すなわち、それぞれの厚さの部
分の電気機械結合係数kが変わることになり、周波数特
性が劣化することを意味する。例えば図1において、複
合圧電体11の直径を20mmに、複合圧電体11の一方
の面を平面に、他方の面の曲率半径を80mmの凹面形状
とし、中央部の最も薄い部分の厚みを0.2mm、最外周
部の最も厚い部分を0.82mm、そして圧電素子12を
等間隔で、圧電素子12の幅を一定の0.15mmにした
場合、中央部の最も薄い部分の圧電素子12の形状比は
0.75に、そして最外周部の最も厚い部分の圧電素子
12の形状比は0.18となる。このことは図2に示し
たように電気機械結合係数kは圧電素子12の形状比が
0.75から0.18の範囲において変化していること
になり、特に形状比0.3以下になると電気機械結合係
数kの低下が顕著になってくる。
A specific example will be described below. Piezoelectric element 1
The electromechanical coupling coefficient k of the composite piezoelectric body 11 has a relationship as shown in FIG. 2 depending on the shape ratio (w / t) between the width w of 2 and the length (thickness of the composite piezoelectric body 11) t. FIG. 2 shows the piezoelectric element 1.
2 is a PZT-based piezoelectric ceramic C-6 manufactured by Fuji Ceramics Co., Ltd., and epoxy resin is used as the organic polymer material 13, and the shape ratio (w / It shows the relationship between t) and the electromechanical coupling coefficient k. As is clear from the relationship in FIG. 2, it is understood that the electromechanical engagement coefficient k changes depending on the shape ratio of the piezoelectric element 12 of the composite piezoelectric body 11. This means that when the composite piezoelectric body 11 has a non-uniform thickness as shown in FIG. 1 and the piezoelectric elements 12 are arranged at the same intervals as in the conventional case, a thin portion (around the center in the figure).
The shape ratio of the piezoelectric element 12 significantly changes between the thick portion and the thick portion (outer peripheral portion in the figure). That is, it means that the electromechanical coupling coefficient k of each thickness portion changes, and the frequency characteristics deteriorate. For example, in FIG. 1, the diameter of the composite piezoelectric body 11 is 20 mm, one surface of the composite piezoelectric body 11 is a flat surface, and the other surface has a concave shape with a radius of curvature of 80 mm. .2 mm, the thickest portion of the outermost peripheral portion is 0.82 mm, and the piezoelectric elements 12 are equally spaced and the width of the piezoelectric element 12 is fixed to 0.15 mm. The shape ratio is 0.75, and the piezoelectric element 12 in the thickest part of the outermost peripheral part has a shape ratio of 0.18. This means that the electromechanical coupling coefficient k changes in the shape ratio of the piezoelectric element 12 in the range of 0.75 to 0.18 as shown in FIG. The decrease of the electromechanical coupling coefficient k becomes remarkable.

【0012】電気機械結合係数kは周波数特性と感度と
に大きく関係しているものであり、電気機械結合係数k
を低下させると周波数帯域特性も低下して狭帯域にな
り、かつ感度も低下するという比例関係にあることは既
に知られている。したがって、圧電素子12の形状比の
値を変化させる。この場合は電気機械結合係数kを低下
させることは周波数特性を劣化させることになるので好
ましくないことである。
The electromechanical coupling coefficient k is greatly related to the frequency characteristic and the sensitivity, and the electromechanical coupling coefficient k
It is already known that there is a proportional relationship in that the frequency band characteristic deteriorates to become a narrow band and the sensitivity also decreases when is decreased. Therefore, the value of the shape ratio of the piezoelectric element 12 is changed. In this case, lowering the electromechanical coupling coefficient k is not preferable because it deteriorates the frequency characteristic.

【0013】このような問題を解決して周波数特性をさ
らに広帯域にするのが、本実施例の特徴である。
It is a feature of the present embodiment that such a problem is solved and the frequency characteristic is further widened.

【0014】例えば図1において、複合圧電体11の直
径を20mm、複合圧電体11の一方の面を平面に、他方
の面を曲率半径が80mmの凹面形状にし、中央部の最も
薄い部分の厚さを0.2mm、最外周部の最も厚い部分を
0.82mmとして、圧電素子12の形状比(w/t)を
どの場所においても一定となる値、例えば0.5という
値に設定した場合には、中央部の最も薄い部分の圧電素
子12の幅w1は0.1mmに、そして最外周部の最も厚
い部分の圧電素子12の幅w2は0.41mmとなる。こ
のように圧電素子12の縦断面形状を一定で配列すると
いうことは、複合圧電体11の圧電素子12の配列間隔
も変えていくということになる。圧電素子の幅が中央部
から外側にいくにしたがって広くなっていることから、
圧電素子12の配列間隔もまた中央部から外側にいくに
したがって広くなっていくことになる。また、複合圧電
体11の中間の厚さをもつ部分の圧電素子12の幅は順
次変えて圧電素子12の形状比(w/t)を約0.5に
なるようにすれば良い。
For example, in FIG. 1, the diameter of the composite piezoelectric body 11 is 20 mm, one surface of the composite piezoelectric body 11 is a flat surface, and the other surface is a concave surface with a radius of curvature of 80 mm. When the thickness is 0.2 mm and the thickest part of the outermost circumference is 0.82 mm, and the shape ratio (w / t) of the piezoelectric element 12 is set to a constant value at any place, for example, a value of 0.5 The width w 1 of the piezoelectric element 12 in the thinnest portion of the central portion is 0.1 mm, and the width w 2 of the piezoelectric element 12 in the thickest portion of the outermost peripheral portion is 0.41 mm. Thus, arranging the piezoelectric elements 12 in a constant vertical cross-sectional shape means changing the arrangement interval of the piezoelectric elements 12 of the composite piezoelectric body 11. Since the width of the piezoelectric element becomes wider from the center to the outside,
The arrangement interval of the piezoelectric elements 12 also becomes wider from the central portion to the outside. Further, the width of the piezoelectric element 12 in the portion having the intermediate thickness of the composite piezoelectric body 11 may be sequentially changed so that the shape ratio (w / t) of the piezoelectric element 12 becomes about 0.5.

【0015】以上のように不均一な厚みを有する複合圧
電体11の圧電素子12の形状比(w/t)をほぼ同じ
値にし、かつ圧電素子12の配列間隔を変えることによ
り、複合圧電体11の中央部から最外周部にわたって電
気機械結合係数kがほぼ一定で、かつ高い値を有するこ
ととなり、広い周波数特性を有するものが得られ、しか
も設計が容易になる。また、凹面形状を有しているた
め、この形状に沿って超音波ビームを集束させることも
同時にできるという特徴を有している。
As described above, the shape ratio (w / t) of the piezoelectric elements 12 of the composite piezoelectric body 11 having a non-uniform thickness is made substantially the same value, and the arrangement interval of the piezoelectric elements 12 is changed, whereby the composite piezoelectric body is changed. Since the electromechanical coupling coefficient k is substantially constant and has a high value from the central portion to the outermost peripheral portion of 11, a wide frequency characteristic can be obtained, and the design is easy. Further, since it has a concave shape, it has the feature that it is possible to focus the ultrasonic beam along this shape at the same time.

【0016】したがって、本発明の複合圧電体を用いた
超音波深触子は、きわめて短いパルス応答波形を得るこ
とができるため、被検深度が深く、かつ分解能の高い超
音波画像を得ることができる。
Therefore, since the ultrasonic deep probe using the composite piezoelectric material of the present invention can obtain an extremely short pulse response waveform, it is possible to obtain an ultrasonic image having a deep test depth and high resolution. it can.

【0017】なお、本実施例においては、複合圧電体1
1の一方の面をある曲率をもたせた凹面形状構成の場合
について説明したが、この他に、凸面形状や両面に曲面
形状をもたせる、もしくは非球面のような複数の曲率半
径をもたせた曲面の形状にすることによっても同様に広
帯域の周波数特性を得ることができる。
In this embodiment, the composite piezoelectric body 1
The case of the concave surface configuration in which one surface of 1 has a certain curvature has been described. Similarly, by forming the shape, a wide band frequency characteristic can be obtained.

【0018】なお、本実施例においては、複合圧電体1
1の形状が円板状の場合について説明したが、この他に
複合圧電体11にアレイ状に電極を設けたいわゆるアレ
イタイプのアレイ電極方向に直交する方向に対して本実
施例を用いても同様に広帯域の周波数特性を得ることが
できる。
In this embodiment, the composite piezoelectric body 1
Although the case where the shape of 1 is a disk shape has been described, in addition to this, the present embodiment is also used in a direction orthogonal to the direction of an array electrode of a so-called array type in which electrodes are provided in the composite piezoelectric body 11 in an array. Similarly, a wide band frequency characteristic can be obtained.

【0019】[0019]

【発明の効果】以上の説明から明らかなように本発明
は、棒状の圧電素子を垂直に多数配列し、前記圧電素子
の周辺に有機高分子材を充填してなる複合圧電体におい
て、前記複合圧電体の厚さを不均一とし、前記圧電素子
の太さと長さをほぼ一定比率とし、かつ前記圧電素子の
配列間隔を不均一とすることにより、それぞれの厚みに
対応した周波数の振動モードを均一に発生することがで
き、複合圧電体の厚みの範囲に対応した広い周波数帯域
特性を得ることができる。したがって、本発明の複合圧
電体を用いた超音波探触子は、きわめて短いパルス応答
波形を得ることができるため、被検深度が深く、かつ分
解能の高い超音波画像を得ることができる。
As is apparent from the above description, the present invention provides a composite piezoelectric body in which a large number of rod-shaped piezoelectric elements are vertically arranged and an organic polymer material is filled around the piezoelectric elements. By making the thickness of the piezoelectric body non-uniform, making the thickness and length of the piezoelectric element substantially constant, and making the arrangement interval of the piezoelectric elements non-uniform, vibration modes of frequencies corresponding to the respective thicknesses can be obtained. It can be generated uniformly, and a wide frequency band characteristic corresponding to the thickness range of the composite piezoelectric body can be obtained. Therefore, since the ultrasonic probe using the composite piezoelectric body of the present invention can obtain an extremely short pulse response waveform, it is possible to obtain an ultrasonic image with a deep test depth and high resolution.

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

【図1】本発明の一実施例における複合圧電体の概略構
成を示す断面図
FIG. 1 is a sectional view showing a schematic configuration of a composite piezoelectric body according to an embodiment of the present invention.

【図2】本発明の複合圧電体の圧電体素子の形状比と電
気機械結合係数との関係を示す図
FIG. 2 is a diagram showing the relationship between the shape ratio of the piezoelectric element of the composite piezoelectric body of the present invention and the electromechanical coupling coefficient.

【図3】従来の複合圧電体の概略構成を示す斜視図FIG. 3 is a perspective view showing a schematic configuration of a conventional composite piezoelectric body.

【符号の説明】[Explanation of symbols]

11 複合圧電体 12 圧電素子 13 有機高分子材 14,15 電極 11 Composite Piezoelectric Body 12 Piezoelectric Element 13 Organic Polymer Material 14, 15 Electrode

Claims (5)

【特許請求の範囲】[Claims] 【請求項1】 棒状の圧電素子を垂直に多数配列し、前
記圧電素子の間隙に有機高分子材を充填してなる複合圧
電体において、前記複合圧電体の厚さを不均一とし、前
記圧電素子の太さと長さをほぼ一定比率とし、かつ前記
圧電素子の配列間隔を不均一としたことを特徴とする複
合圧電体。
1. A composite piezoelectric body in which a large number of rod-shaped piezoelectric elements are vertically arranged, and a gap between the piezoelectric elements is filled with an organic polymer material. A composite piezoelectric body, characterized in that the thickness and the length of the elements are set to a substantially constant ratio, and the arrangement intervals of the piezoelectric elements are made nonuniform.
【請求項2】 一方の面が平坦で、他方の面が曲面形状
であることを特徴とする請求項1記載の複合圧電体。
2. The composite piezoelectric body according to claim 1, wherein one surface is flat and the other surface is curved.
【請求項3】 両面がそれぞれ違う曲面形状であること
を特徴とする請求項1記載の複合圧電体。
3. The composite piezoelectric body according to claim 1, wherein both surfaces have different curved surface shapes.
【請求項4】 曲面が凹面形状であることを特徴とする
請求項1記載の複合圧電体。
4. The composite piezoelectric body according to claim 1, wherein the curved surface has a concave shape.
【請求項5】 圧電素子の配列間隔が中央部では狭く、
外側に行くにしたがって広くなるように構成したことを
特徴とする請求項1記載の複合圧電体。
5. The arrangement interval of the piezoelectric elements is narrow in the central portion,
The composite piezoelectric body according to claim 1, wherein the composite piezoelectric body is configured so as to become wider toward the outside.
JP22687192A 1992-08-26 1992-08-26 Composite piezoelectric Expired - Fee Related JP2682342B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22687192A JP2682342B2 (en) 1992-08-26 1992-08-26 Composite piezoelectric

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22687192A JP2682342B2 (en) 1992-08-26 1992-08-26 Composite piezoelectric

Publications (2)

Publication Number Publication Date
JPH0678399A true JPH0678399A (en) 1994-03-18
JP2682342B2 JP2682342B2 (en) 1997-11-26

Family

ID=16851884

Family Applications (1)

Application Number Title Priority Date Filing Date
JP22687192A Expired - Fee Related JP2682342B2 (en) 1992-08-26 1992-08-26 Composite piezoelectric

Country Status (1)

Country Link
JP (1) JP2682342B2 (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6247368B1 (en) 1999-01-04 2001-06-19 International Business Machines Corporation CMP wet application wafer sensor
JP2002209292A (en) * 2001-01-11 2002-07-26 Matsushita Electric Ind Co Ltd Ultrasonic probe
JP2002232995A (en) * 2001-02-06 2002-08-16 Matsushita Electric Ind Co Ltd Ultrasonic wave probe and its manufacturing method
US7213460B2 (en) * 2005-01-19 2007-05-08 Denso Corporation Ultrasonic sensor

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6247368B1 (en) 1999-01-04 2001-06-19 International Business Machines Corporation CMP wet application wafer sensor
JP2002209292A (en) * 2001-01-11 2002-07-26 Matsushita Electric Ind Co Ltd Ultrasonic probe
JP2002232995A (en) * 2001-02-06 2002-08-16 Matsushita Electric Ind Co Ltd Ultrasonic wave probe and its manufacturing method
US7213460B2 (en) * 2005-01-19 2007-05-08 Denso Corporation Ultrasonic sensor

Also Published As

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