JPH06197894A - Doppler diagnostic ultrasonic probe - Google Patents

Doppler diagnostic ultrasonic probe

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Publication number
JPH06197894A
JPH06197894A JP49293A JP49293A JPH06197894A JP H06197894 A JPH06197894 A JP H06197894A JP 49293 A JP49293 A JP 49293A JP 49293 A JP49293 A JP 49293A JP H06197894 A JPH06197894 A JP H06197894A
Authority
JP
Japan
Prior art keywords
surface acoustic
electrode
ultrasonic probe
acoustic wave
doppler
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
JP49293A
Other languages
Japanese (ja)
Other versions
JP2975493B2 (en
Inventor
Shoichi Yamashita
昇一 山下
Toshiyuki Matsunaka
敏行 松中
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 JP5000492A priority Critical patent/JP2975493B2/en
Publication of JPH06197894A publication Critical patent/JPH06197894A/en
Application granted granted Critical
Publication of JP2975493B2 publication Critical patent/JP2975493B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

PURPOSE:To eliminate a stand-off member which has been conventionally required for a conventional ultrasonic probe in the case of Doppler measurement. CONSTITUTION:The upper surface of a piezoelectric material 30 is sectioned into an electrode area and a waveguide area, and comb-shaped electrodes 34a, 34b meshed with each other are formed in the electrode area, and an absorbing cover 36 is formed on the upper surface thereof. An elastic surface wave generated at an electrode part 32 is transmitted to a wave guide part 33 abutting against an acoustic transmission medium from which the elastic wave is radiated in one oblique direction.

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、超音波ドプラ法によっ
て血流速度等を測定する際に用いられるドプラ診断用超
音波探触子に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an ultrasonic probe for Doppler diagnosis used when measuring a blood flow velocity and the like by an ultrasonic Doppler method.

【0002】[0002]

【従来の技術】超音波を生体内に送波し、生体内の運動
反射体(例えば血流)にてドプラシフトを受けた反射波
を受波し、受信信号に含まれるドプラ情報から前記運動
反射体の速度等を測定する超音波ドプラ診断装置が活用
されている。ここで、超音波の送受波は超音波振動子を
有する超音波探触子によって行われる。
2. Description of the Related Art An ultrasonic wave is transmitted into a living body, a reflected wave subjected to a Doppler shift by a moving reflector (for example, blood flow) in the living body is received, and the movement reflection is performed from the Doppler information included in the received signal. An ultrasonic Doppler diagnostic device that measures body speed and the like is used. Here, transmission and reception of ultrasonic waves are performed by an ultrasonic probe having an ultrasonic transducer.

【0003】一般に、従来の超音波振動子は、圧電材料
を2つの電極で挟んだ構造をなし、その両電極間に高周
波信号を印加することによって、圧電材料が周期的に歪
み、この結果、圧電材料の表面からその垂直方向に弾性
波である超音波が放射される。
Generally, a conventional ultrasonic transducer has a structure in which a piezoelectric material is sandwiched between two electrodes, and when a high frequency signal is applied between the two electrodes, the piezoelectric material is periodically distorted, and as a result, Ultrasonic waves, which are elastic waves, are emitted from the surface of the piezoelectric material in the vertical direction.

【0004】ところで、超音波がドプラシフトを受ける
ためには、原理上、運動反射体である血流等の運動方向
に対して超音波ビーム方向が直交していてはならず、あ
る程度以上の交差角度が必要である。
By the way, in order for an ultrasonic wave to undergo a Doppler shift, in principle, the ultrasonic beam direction should not be orthogonal to the direction of motion of the blood flow, which is a motion reflector, and the crossing angle of a certain degree or more. is necessary.

【0005】従って、従来においては、超音波探触子を
体表に当接させて体表下を流れる体表に平行な血管内の
血流速度を測定しようとする場合、超音波ビームを体表
に対して斜めに設定する必要から、超音波振動子を体表
に対して斜めに配置する必要がある。それゆえ、従来に
おいては、図6に示すように、超音波振動子10と体表
100との間に、生体と音響インピーダンスがほぼ等し
いくさび形のスタンドオフ材12を介在配置させる必要
があった。これは、図7に示すように、生体内の血管1
02に直接当接して血流104の速度を測定する術中超
音波探触子や術後に生体内に留置する超音波探触子につ
いても同様であり、スタンドオフ材12が必要となって
いた。
Therefore, conventionally, when an ultrasonic probe is brought into contact with the body surface to measure the blood flow velocity in a blood vessel flowing under the body surface and parallel to the body surface, the ultrasonic beam is applied to the body surface. Since it is necessary to set the ultrasonic transducer obliquely with respect to the surface, it is necessary to dispose the ultrasonic transducer obliquely with respect to the body surface. Therefore, conventionally, as shown in FIG. 6, it is necessary to interpose a wedge-shaped standoff material 12 having substantially the same acoustic impedance as that of the living body between the ultrasonic transducer 10 and the body surface 100. . As shown in FIG. 7, this is a blood vessel 1 in a living body.
The same applies to the intraoperative ultrasonic probe that directly contacts the blood vessel 02 to measure the velocity of the blood flow 104 and the ultrasonic probe that is placed in the living body after the operation, and the stand-off member 12 was necessary. .

【0006】一方、体腔内や血管内に挿入される超音波
探触子においては、血流と平行に超音波ビームを形成す
るときにドプラシフトが最も大きくなるため、本来、挿
入管の先端前面に超音波振動子を配置することが望まし
い。
On the other hand, in an ultrasonic probe inserted into a body cavity or a blood vessel, the Doppler shift becomes the largest when an ultrasonic beam is formed parallel to the blood flow. It is desirable to place an ultrasonic transducer.

【0007】しかし、図8に示されるように、その挿入
管14が筒構造をなし、その内部空洞に例えばガイドワ
イヤ16が通される超音波探触子においては、先端前面
に開口が形成されるため、超音波振動子18の中央に開
口を形成しなければならず、加工、製作が困難であり、
更に超音波振動子18の有効面積が小さくなり、特性の
劣化を生じるという不都合がある。
However, as shown in FIG. 8, in the ultrasonic probe in which the insertion tube 14 has a tubular structure and the guide wire 16 is passed through the internal cavity, an opening is formed in the front surface of the tip. Therefore, an opening must be formed in the center of the ultrasonic transducer 18, which is difficult to process and manufacture.
Further, there is a disadvantage that the effective area of the ultrasonic transducer 18 is reduced and the characteristics are deteriorated.

【0008】一方、超音波振動子の開口形成を回避する
ため、図9に示されるように、挿入管14の側部に超音
波振動子20を斜めに配置する場合には、管を部分的に
肥大させてしまい、挿入困難及び製作困難という問題が
生じる。
On the other hand, in order to avoid the formation of the opening of the ultrasonic transducer, when the ultrasonic transducer 20 is obliquely arranged on the side of the insertion tube 14 as shown in FIG. This causes the problem of difficulty in insertion and manufacturing.

【0009】[0009]

【発明が解決しようとする課題】以上のように、従来に
おいてドプラ計測を行う場合、体表当接型及び血管当接
型のドプラ診断用超音波探触子においてはスタンドオフ
材が必要となり、体腔内挿入型の超音波探触子において
は製作困難な構造になってしまうという問題があった。
As described above, in the conventional Doppler measurement, a stand-off material is required in the body surface contact type and blood vessel contact type Doppler diagnostic ultrasonic probes. The ultrasonic probe of the body cavity insertion type has a problem that the structure is difficult to manufacture.

【0010】本発明は、上記従来の課題に鑑みなされた
ものであり、その目的は、超音波を発生させる素子を斜
めに配置することなくドプラ計測を行うことのできるド
プラ診断用超音波探触子を提供することにある。
The present invention has been made in view of the above conventional problems, and an object thereof is an ultrasonic probe for Doppler diagnosis capable of performing Doppler measurement without obliquely disposing an element for generating ultrasonic waves. To provide a child.

【0011】[0011]

【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、超音波探触子において超音波を送受波す
る素子として、弾性表面波素子(以下SAW(Surf
ace Acoustic Wave)素子ともいう)
を用いたことを特徴とする。
In order to achieve the above object, the present invention provides a surface acoustic wave element (hereinafter SAW (Surf) as an element for transmitting and receiving ultrasonic waves in an ultrasonic probe.
ace Acoustic Wave) element)
Is used.

【0012】すなわち、請求項1記載の発明は、圧電素
子の上面に電極が形成され前記圧電素子上面にて弾性表
面波が発生される弾性表面波素子を超音波探触子に配設
し、前記弾性表面波素子を音響伝搬媒体に当接させたこ
とを特徴とする。
That is, according to the first aspect of the invention, a surface acoustic wave element having electrodes formed on the upper surface of the piezoelectric element and surface acoustic waves generated on the upper surface of the piezoelectric element is disposed in the ultrasonic probe, The surface acoustic wave element is brought into contact with an acoustic propagation medium.

【0013】また、請求項2記載の発明は、弾性表面波
素子を有するドプラ診断用超音波探触子であって、前記
弾性表面波素子は、上面が電極領域と導波領域とに区分
された圧電材料と、前記電極領域上に形成された電極部
と、で構成され、前記電極部は、一方の櫛型電極と、そ
れに噛み合う他方の櫛形電極と、それらの両電極を覆う
吸収カバーと、で構成されたことを特徴とする。
According to a second aspect of the present invention, there is provided a Doppler diagnostic ultrasonic probe having a surface acoustic wave element, wherein the surface acoustic wave element has an upper surface divided into an electrode region and a waveguide region. A piezoelectric material and an electrode portion formed on the electrode region, the electrode portion includes one comb-shaped electrode, the other comb-shaped electrode that meshes with the comb-shaped electrode, and an absorption cover that covers both electrodes. It is characterized by being constituted by.

【0014】[0014]

【作用】上記請求項1記載の構成によれば、SAW素子
が音響伝搬媒体に当接されているので、SAW素子の上
面で弾性表面波が生じると、漏れ弾性表面波が、SAW
素子の音速に対する音響伝搬媒体中の音速の比に従った
角度で音響伝搬媒体内へ斜めに放射されることになる。
ここで、音響伝搬媒体は、生体組織又は生体等価物質で
ある。SAW素子に当接された音響伝搬媒体が生体組織
である場合には漏れ弾性表面波が直接的に生体内へ放射
され、SAW素子に当接された音響伝搬媒体が生体等価
物質の場合には、その生体等価物質を介して生体内へ漏
れ弾性表面波が放射される。一方、以上とは逆に、生体
内の運動反射体にてドプラシフトを受けた反射波は、S
AW素子にて受波される。
According to the structure of the first aspect, since the SAW element is in contact with the acoustic propagation medium, when a surface acoustic wave is generated on the upper surface of the SAW element, the leaky surface acoustic wave causes the SAW element.
The light is obliquely radiated into the acoustic propagation medium at an angle according to the ratio of the acoustic velocity in the acoustic propagation medium to the acoustic velocity of the element.
Here, the acoustic propagation medium is a biological tissue or a biological equivalent substance. When the acoustic propagation medium contacted with the SAW element is biological tissue, the leaky surface acoustic waves are directly radiated into the living body, and when the acoustic propagation medium contacted with the SAW element is a biological equivalent substance. , Surface acoustic waves are radiated into the living body through the biological equivalent substance. On the other hand, conversely to the above, the reflected wave subjected to the Doppler shift by the motion reflector in the living body is S
Received by the AW element.

【0015】このように、ドプラ診断用の素子としてS
AW素子を用いれば、素子を傾けることなく、超音波
(弾性波)を素子表面から斜めに放射させることが可能
となる。
As described above, S is used as an element for Doppler diagnosis.
By using the AW element, it becomes possible to radiate ultrasonic waves (elastic waves) obliquely from the element surface without tilting the element.

【0016】上記請求項2記載の構成によれば、電極部
において弾性表面波が生じるが、この場合、吸収カバー
がなければ、電極部から前後の2つの斜め方向に弾性表
面波が生じようとする。しかし、それらの斜め方向の弾
性表面波は、吸収カバーによって吸収される。従って、
弾性表面波が電極部から水平方向に導波領域へ伝達さ
れ、その際、導波領域に音響伝搬媒体が当接されていれ
ば、上述同様に、斜め方向に弾性表面波が放射されるこ
とになる。ただし、この場合には、弾性表面波の伝達方
向のみについて斜めに弾性表面波が放射される。すなわ
ち、前後2つの斜め方向への弾性表面波の放射が回避さ
れ、前方(電極部から見て導波領域がある方向)にのみ
斜めに弾性表面波が放射される。なお、受波も導波領域
によって行われる。
According to the structure described in claim 2, surface acoustic waves are generated in the electrode portion. In this case, however, if there is no absorbing cover, surface acoustic waves are generated in two oblique directions, front and rear, from the electrode portion. To do. However, those oblique surface acoustic waves are absorbed by the absorbing cover. Therefore,
If the surface acoustic wave is transmitted from the electrode part to the waveguide area in the horizontal direction and the acoustic propagation medium is in contact with the waveguide area at that time, the surface acoustic wave is emitted in the oblique direction as described above. become. However, in this case, the surface acoustic waves are radiated obliquely only in the propagation direction of the surface acoustic waves. That is, the emission of the surface acoustic waves in the front and rear two oblique directions is avoided, and the surface acoustic waves are obliquely emitted only in the front direction (the direction in which the waveguide region is seen from the electrode portion). In addition, the wave reception is also performed by the waveguide region.

【0017】[0017]

【実施例】以下、本発明の好適な実施例を図面に基づい
て説明する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT A preferred embodiment of the present invention will be described below with reference to the drawings.

【0018】(A)原理説明 まず、前提説明としてSAW素子の原理について説明す
る。図3には、一般的なSAW素子20の上面図が示さ
れている。SAW素子20は、圧電材料22の上面に、
互いに噛み合う櫛形の一方の電極24aと他方の電極2
4bとを形成してなるものである。なお、従来、このS
AW素子はアナログ遅延線などとしても用いられてい
る。
(A) Description of Principle First, as a premise, the principle of the SAW element will be described. FIG. 3 shows a top view of a general SAW element 20. The SAW element 20 is provided on the upper surface of the piezoelectric material 22,
Comb-shaped one electrode 24a and the other electrode 2 that mesh with each other
4b is formed. Incidentally, conventionally, this S
The AW element is also used as an analog delay line or the like.

【0019】このSAW素子の一般的な使用態様におい
ては、電極間に高周波信号を印加すると、圧電材料の上
面(電極面)に弾性表面波が生じる。
In a general use mode of this SAW element, when a high frequency signal is applied between the electrodes, a surface acoustic wave is generated on the upper surface (electrode surface) of the piezoelectric material.

【0020】しかし、図4に示すように、生体等の音響
伝搬媒体106に電極面を当接させると、圧電材料22
におけるSAWA素子の音速に対する音響伝搬媒体10
6中の音速の比に従った角度で漏れ弾性表面波が音響伝
搬媒体内へ斜めに放射される。
However, as shown in FIG. 4, when the electrode surface is brought into contact with the acoustic propagation medium 106 such as a living body, the piezoelectric material 22
Acoustic medium 10 for sound velocity of SAWA device in
The leaky surface acoustic waves are obliquely radiated into the acoustic propagation medium at an angle according to the ratio of the sound velocities in 6.

【0021】すなわち、図5に示すように、電極面の法
線に対して弾性表面波が放射される角度をθとすると、 θ=Sin-1((音響伝搬媒体の音速V1)/(SAW素子の音速V2)) …(1) となる。従って、このSAW素子を用いれば、従来のよ
うに、超音波振動子を斜めに配置する際の問題点を解消
できる。
That is, as shown in FIG. 5, when the angle at which the surface acoustic wave is radiated with respect to the normal to the electrode surface is θ, θ = Sin -1 ((sound velocity V1 of acoustic propagation medium) / (SAW The sound velocity of the element V2)) (1). Therefore, by using this SAW element, it is possible to solve the problem when the ultrasonic transducer is obliquely arranged as in the conventional case.

【0022】ところが、図3に示したSAW素子20
は、前後方向(紙面左右方向)に斜めに2つの弾性表面
波が放射されるため、そのままでは、ドプラシフトが正
負両方向に生じ、ドプラ計測を行うことは困難な場合が
ある。そこで、一方向のみに斜めに弾性波を生じさせる
ことが必要となる。
However, the SAW element 20 shown in FIG.
Since two surface acoustic waves are radiated obliquely in the front-back direction (left-right direction on the paper surface), Doppler shift may occur in both positive and negative directions without doing so, and it may be difficult to perform Doppler measurement. Therefore, it is necessary to generate elastic waves diagonally in only one direction.

【0023】(B)実施例の説明 図1には、本発明に係るドプラ診断用超音波探触子の好
適な実施例が示されており、図1(A)は上面図、
(B)は側断面図である。
(B) Description of Embodiment FIG. 1 shows a preferred embodiment of the ultrasonic probe for Doppler diagnosis according to the present invention. FIG. 1 (A) is a top view,
(B) is a side sectional view.

【0024】図示されるように、圧電材料30の上面3
0aのうち片側が導波領域とされ、もう一方の片側が電
極領域とされている。本実施例において、導波領域は外
部に露出しており、弾性波を送受波する導波部33とな
っている。もちろん、導波領域上に生体組織と音響イン
ピーダンスが等しい組織等価物質の層を形成し、それを
導波部33としてもよい。
As shown, the upper surface 3 of the piezoelectric material 30.
One side of 0a is a waveguide region, and the other side is an electrode region. In this embodiment, the waveguide region is exposed to the outside and serves as a waveguide portion 33 that transmits and receives elastic waves. Of course, a layer of a tissue-equivalent substance having the same acoustic impedance as that of the biological tissue may be formed on the waveguiding region and used as the waveguiding section 33.

【0025】電極領域上の電極部32は、電極34と吸
収カバー36とで構成されている。電極34は、2つの
電極34aと電極34bとで構成され、それらの電極は
櫛形に形成され、互いに対向して噛み合っている。これ
らの両電極間には高周波信号が印加される。なお、図示
されてはいないが、各電極には信号線が接続され、外部
回路と電気的に接続されている。
The electrode portion 32 on the electrode region is composed of an electrode 34 and an absorption cover 36. The electrode 34 is composed of two electrodes 34a and 34b, and these electrodes are formed in a comb shape and face each other and mesh with each other. A high frequency signal is applied between these two electrodes. Although not shown, a signal line is connected to each electrode and electrically connected to an external circuit.

【0026】この電極34は、その全面が吸収カバー3
6で覆われている。ここで、吸収カバー36は、弾性表
面波の発生を阻害せずに、電極部32から直接斜め方向
への漏れ弾性表面波を阻止・吸収するものであり、例え
ば、粘着テープや発泡ウレタン材などが用いられる。
The entire surface of the electrode 34 is the absorption cover 3
Covered with 6. Here, the absorption cover 36 blocks and absorbs the leaking surface acoustic waves directly in the oblique direction from the electrode portion 32 without hindering the generation of the surface acoustic waves. For example, an adhesive tape or a urethane foam material. Is used.

【0027】以上の構成とすることにより、高周波信号
印加により電極部32にて弾性表面波が生じると、電極
部32から直接的に斜め方向に漏れ弾性表面波は生じ
ず、弾性表面波が、電極部32から導波部33に伝達さ
れ、ここで音響伝搬媒体に導波部が当接されているた
め、上述した第1式に従った角度で弾性表面波が斜め方
向に放射される。その場合、伝達方向と逆の方向への斜
め放射はなく、前方斜め方向への放射のみを実現でき
る。
With the above structure, when a surface acoustic wave is generated in the electrode portion 32 by applying a high frequency signal, the surface acoustic wave does not directly leak from the electrode portion 32 in an oblique direction and the surface acoustic wave is generated. The surface acoustic wave is transmitted from the electrode portion 32 to the waveguide portion 33, and the waveguide portion is in contact with the acoustic propagation medium here, so that the surface acoustic wave is radiated in an oblique direction at an angle according to the above-described first equation. In that case, there is no oblique radiation in the direction opposite to the transmission direction, and only radiation in the forward diagonal direction can be realized.

【0028】図2には、本実施例のSAW素子を超音波
送受波素子として用いた場合の概念が示されている。図
示されるように、生体表面108に平行にSAW素子3
1を当接させれば、斜め方向に弾性表面波(超音波)が
放射され、素子自体を傾ける必要はない。よって、スタ
ンドオフ材を用いる必要がない。
FIG. 2 shows a concept when the SAW element of this embodiment is used as an ultrasonic wave transmitting / receiving element. As shown, the SAW element 3 is arranged parallel to the living body surface 108.
If 1 is abutted, surface acoustic waves (ultrasonic waves) are radiated in an oblique direction, and it is not necessary to tilt the element itself. Therefore, it is not necessary to use a standoff material.

【0029】図2に示した例は、生体表面当接型であっ
たが、もちろん血管当接型、あるいは体腔内挿入型の超
音波探触子にも本実施例の超音波探触子を適用できる。
体腔内挿入型のドプラ診断用超音波探触子においては、
挿入管の側面に本実施例のSAW素子を配置すればよ
い。
The example shown in FIG. 2 is of a living body surface contact type, but of course, the ultrasonic probe of this embodiment can be applied to a blood vessel contact type or a body cavity insertion type ultrasonic probe. Applicable.
In the ultrasonic probe for Doppler diagnosis of the body cavity insertion type,
The SAW element of this embodiment may be arranged on the side surface of the insertion tube.

【0030】[0030]

【発明の効果】以上説明したように、本発明によれば、
超音波を発生させる超音波振動子を斜めに配置すること
なくドプラ計測を行うことが可能となる。従って、従来
において必要とされていたスタンドオフ材等を排除でき
るという効果がある。
As described above, according to the present invention,
It is possible to perform Doppler measurement without arranging ultrasonic transducers that generate ultrasonic waves at an angle. Therefore, there is an effect that the stand-off material or the like which has been conventionally required can be eliminated.

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

【図1】本発明に係るドプラ診断用超音波探触子の要部
構成を示す上面図及び側断面図である。
1A and 1B are a top view and a side cross-sectional view showing a configuration of a main part of an ultrasonic probe for Doppler diagnosis according to the present invention.

【図2】本発明に係るSAW素子を利用してドプラ計測
を行う場合の概念を示す説明図である。
FIG. 2 is an explanatory diagram showing the concept of Doppler measurement using the SAW element according to the present invention.

【図3】一般的なSAW素子の上面図である。FIG. 3 is a top view of a general SAW element.

【図4】図3に示すSAW素子を生体表面106に当接
して弾性表面波を発生させた場合における斜め方向の弾
性表面波を示す説明図である。
FIG. 4 is an explanatory diagram showing a surface acoustic wave in an oblique direction when the surface acoustic wave is generated by contacting the SAW element shown in FIG.

【図5】SAW素子からの斜め方向の2つの弾性表面波
の放射角度を示す説明図である。
FIG. 5 is an explanatory diagram showing radiation angles of two surface acoustic waves in an oblique direction from the SAW element.

【図6】従来の体表当接型の超音波探触子を示す説明図
である。
FIG. 6 is an explanatory view showing a conventional body surface contact type ultrasonic probe.

【図7】従来の血管当接型の超音波探触子を示す説明図
である。
FIG. 7 is an explanatory view showing a conventional blood vessel contact type ultrasonic probe.

【図8】従来の体腔内挿入型超音波探触子を示す説明図
である。
FIG. 8 is an explanatory view showing a conventional ultrasonic probe inserted into a body cavity.

【図9】従来の体腔内挿入型超音波探触子を示す説明図
である。
FIG. 9 is an explanatory diagram showing a conventional ultrasonic probe inserted into a body cavity.

【符号の説明】[Explanation of symbols]

30 圧電材料 32 電極部 33 導波部 34 電極 30 Piezoelectric material 32 Electrode part 33 Waveguide part 34 Electrode

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 圧電素子の上面に電極が形成され前記圧
電素子上面にて弾性表面波が発生される弾性表面波素子
を超音波探触子に配設し、 前記弾性表面波素子を音響伝搬媒体に当接させ、前記圧
電素子上面にて発生する弾性表面波を斜めに放射させて
ドプラ計測を行うことを特徴とするドプラ診断用超音波
探触子。
1. A surface acoustic wave element having electrodes formed on the upper surface of the piezoelectric element and generating surface acoustic waves on the upper surface of the piezoelectric element is disposed in an ultrasonic probe, and the surface acoustic wave element propagates acoustically. An ultrasonic probe for Doppler diagnosis, which is brought into contact with a medium and obliquely emits a surface acoustic wave generated on the upper surface of the piezoelectric element to perform Doppler measurement.
【請求項2】 弾性表面波素子を有するドプラ診断用超
音波探触子であって、 前記弾性表面波素子は、上面が電極領域と導波領域とに
区分された圧電材料と、前記電極領域上に形成された電
極部と、で構成され、 前記電極部は、一方の櫛型電極と、それに噛み合う他方
の櫛形電極と、それらの両電極を覆う吸収カバーと、で
構成され、 音響媒体が当接される前記導波領域から1つの斜め方向
に弾性表面波が放射されることを特徴とするドプラ診断
用超音波探触子。
2. A Doppler diagnostic ultrasonic probe having a surface acoustic wave element, wherein the surface acoustic wave element has a piezoelectric material whose upper surface is divided into an electrode region and a waveguide region, and the electrode region. And an electrode cover formed on the electrode part formed above, and the electrode part is composed of one comb-shaped electrode, the other comb-shaped electrode that meshes with the comb-shaped electrode, and an absorbing cover that covers both of the electrodes. An ultrasonic probe for Doppler diagnosis, characterized in that surface acoustic waves are radiated in one oblique direction from the abutting waveguide region.
JP5000492A 1993-01-06 1993-01-06 Doppler diagnostic ultrasound probe Expired - Fee Related JP2975493B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5000492A JP2975493B2 (en) 1993-01-06 1993-01-06 Doppler diagnostic ultrasound probe

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5000492A JP2975493B2 (en) 1993-01-06 1993-01-06 Doppler diagnostic ultrasound probe

Publications (2)

Publication Number Publication Date
JPH06197894A true JPH06197894A (en) 1994-07-19
JP2975493B2 JP2975493B2 (en) 1999-11-10

Family

ID=11475261

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5000492A Expired - Fee Related JP2975493B2 (en) 1993-01-06 1993-01-06 Doppler diagnostic ultrasound probe

Country Status (1)

Country Link
JP (1) JP2975493B2 (en)

Also Published As

Publication number Publication date
JP2975493B2 (en) 1999-11-10

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