This application is based upon and claims the benefit of priority from prior Japanese Patent Application No. 2007-258899, filed Oct. 2, 2007, the entire contents of which are incorporated herein by reference.
1. Field of the Invention
The present invention relates to an ultrasonic probe and a piezoelectric transducer that generate ultrasonic waves with transmission intensity weighted.
2. Description of the Related Art
There is a ultrasonic probe which has a plurality of piezoelectric transducers arranged in an array direction. In the linear array ultrasonic probe, when a drive signal is applied to the respective piezoelectric transducers, side lobes in acoustic fields in a lens direction cause problems or the acoustic fields in the lens direction are made non-uniform. Therefore, as a technique to reduce side lobes or to make acoustic fields uniform, weighting the ultrasonic waves in the lens direction is conducted to change the intensity distribution of ultrasonic waves transmitted and received to/from a piezoelectric transducer.
As a technique for weighting in this way, there is a method for achieving desired weighting on the ultrasonic wave intensity in the lens direction by disposing the piezoelectric transducers and grooves for dividing the piezoelectric transducers alternately at predetermined intervals (for example, see Jpn. Pat. Appln. KOKAI Publication No. 2003-9288).
As another technique for weighting, there is a method of forming grooves in the lens direction which are arranged on the top surface or bottom surface or both, of piezoelectric transducers at the depth and intervals in accordance with weighting and at the same time which do not divide the piezoelectric transducers (for example, see Jpn. Pat. Appln. KOKAI Publication No. 2005-328507).
However, the technique stipulated in Jpn. Pat. Appln. KOKAI Publication No. 2003-9288 deals with a structure to completely divide the piezoelectric transducer by grooves (so-called composite structure), and therefore, it is difficult to manufacture an ultrasonic probe. In addition, electrodes must be formed on the resin material filled in grooves, but adhesion of electrodes to the resin material is low and the low reliability of an ultrasonic probe results.
In addition, in the technique stipulated in Jpn. Pat. Appln. KOKAI Publication No. 2005-328507, the weighted intensity depends also on the groove depth. That is, in order to obtain still intensified weighting, still deeper grooves are required. When deep grooves are formed, mechanical strength of piezoelectric transducers is lowered. In addition, in this technique, a plurality of piezoelectric transducer pieces are formed by a plurality of grooves. In this kind of structure, it is important to definitely connect an electrode to each one of the piezoelectric transducer pieces. However, it is difficult to connect electrodes to a plurality of piezoelectric transducer pieces with high reliability by pressure-bonding piezoelectric transducer pieces having high rigidity to acoustic matching layers (or flexible PC boards).
It is an object of the present invention to provide an ultrasonic probe and a piezoelectric transducer that can improve the reliability of electrode connections and improve the yield.
An ultrasonic probe according to a first aspect of the present invention comprises: a plurality of piezoelectric elements which vibrate in a first direction and are arranged along a second direction substantially orthogonal to the first direction; a pair of electrodes formed on each of said plurality of piezoelectric elements; and a plurality of non-piezoelectric elements arranged inside each of said plurality of piezoelectric elements along a third direction substantially orthogonal to the first and second directions.
A piezoelectric transducer according to a second aspect of the present invention comprises: a piezoelectric element which vibrates in a first direction; a pair of electrodes formed on the piezoelectric element; and a plurality of non-piezoelectric elements arranged inside the piezoelectric element along a second direction orthogonal to the first direction.
An ultrasonic probe according to a third aspect of the present invention comprises: an ultrasonic probe comprising: a plurality of piezoelectric elements; a first electrode formed on a first surface of each of the piezoelectric elements; a second electrode formed on a second surface of each of the piezoelectric elements, the second surface being opposite to the first surface; and a plurality of predetermined members buried in an area between the first surface and the second surface of each of the piezoelectric elements.
Additional objects and advantages of the invention will be set forth in the description which follows, and in part will be obvious from the description, or may be learned by practice of the invention. The objects and advantages of the invention may be realized and obtained by means of the instrumentalities and combinations particularly pointed out hereinafter.
The accompanying drawings, which are incorporated in and constitute a part of the specification, illustrate embodiments of the invention, and together with the general description given above and the detailed description of the embodiments given below, serve to explain the principles of the invention.
Referring now to the drawings, ultrasonic probes and piezoelectric transducers according to embodiments of the present invention will be described.
The plurality of piezoelectric transducers 14 are arranged in one line with predetermined intervals provided with respect to the direction Y perpendicular to the paper surface of
Inside the piezoelectric element 17, a plurality of non-piezoelectric elements 23 are arranged at a plurality of varying pitch intervals (center-to-center distance of adjacent non-piezoelectric elements 23) p along a direction substantially orthogonal to the array direction Y and the thickness direction Z (hereinafter called the lens direction). The non-piezoelectric elements 23 have substantially strip shapes and pass through the piezoelectric element 17 in the array direction Y. The pitch intervals p of the non-piezoelectric elements 23 are based on weighting of the ultrasonic wave intensity related to the lens direction. In addition, the length concerning the thickness direction Z of the non-piezoelectric elements 23 is based on the weighting. By weighting, the piezoelectric transducer 14 can transmit uniform ultrasonic waves with respect to the lens direction as compared to the case of equal pitch intervals. The plurality of non-piezoelectric elements 23 do not reach either of both surfaces (both surfaces with electrodes 19 and 21 formed) of the piezoelectric element 17 substantially orthogonal to the thickness direction Z. The non-piezoelectric elements 23 are buried in an area between the both surfaces of the piezoelectric element 17. Although the non-piezoelectric elements 23 are typically formed by hardened adhesives of composite material, etc. of epoxy resin or epoxy resin mixed with fillers, any adhesive can be employed for the non-piezoelectric elements 23 as long as no piezoelectric properties are exhibited. For the material of the piezoelectric element 17, two-component system or three-component system piezoelectric ceramics or piezoelectric monocrystals are used. The detail concerning the structure of the piezoelectric transducer 14 will be discussed later.
Each signal electrode 19 is formed by metal plating by silver, gold, etc. or sputtering. Each signal electrode 19 is electrically connected to each wiring disposed to the FPC 13, one by one. As a result, drive signals are applied individually to the plurality of piezoelectric transducers 14.
The FPC 13 is disposed between the backing material 11 and the piezoelectric transducer 14 as described above. The FPC 13 is composed of a plurality of wirings for supplying electric power to a plurality of signal electrodes 19, flexible substrates, etc. The signal electrodes 19 and wirings are electrically connected. Through this wiring, a predetermined voltage is applied to the signal electrode 19 from an ultrasonic diagnostic apparatus body not shown in the figure.
To the upper surface of the piezoelectric transducers 14, a plurality of acoustic matching layers 25 are disposed. The acoustic matching layers 25 play a role to suppress reflection of ultrasonic waves arising from a difference between acoustic impedance of a patient and acoustic impedance of the piezoelectric transducers 14. The acoustic matching layer 25 is provided with a first acoustic matching layer 27 and a second acoustic matching layer 29. By the first acoustic matching layer 27 and the second acoustic matching layer 29, the acoustic impedance is changed stepwise from the piezoelectric transducer 14 to a patient. The first acoustic matching layer 27 is formed of a conductive material. The lower surface of the first acoustic matching layer 27 is electrically connected to the piezoelectric transducer 14 through the earth electrode 21. The upper surface of the first acoustic matching layer 27 is joined with the second acoustic matching layer 29. The second acoustic matching layer 29 is formed of an insulating material. Note that, the acoustic matching layer 25 is composed of two layers of acoustic matching layers, but it may be composed of one layer or three layers, or more layers of acoustic matching layers.
An acoustic lens 31 is mounted on the upper surface of a plurality of acoustic matching layers 25. The acoustic lens 31 is a lens made of silicone rubber, etc., which has the acoustic impedance close to a living body. The acoustic lens 31 focuses ultrasonic waves in the lens direction and improves resolution.
Next discussion will be made on the specific structure of the piezoelectric transducer 14. As shown in
The first piezoelectric element portion 33 includes a plurality of non-piezoelectric elements 23 which are filled, respectively, in a plurality of grooves formed at pitch intervals p based on weighting of ultrasonic intensity along the lens direction X. The plurality of pitch intervals p are increased as they come closer to the center of the lens direction X due to weighting. Each pitch interval p is determined on the basis of sine functions, Gaussian functions, and other functions. On the lower surface of the first piezoelectric element portion 33, the signal electrode 19 is formed by sputtering, etc. Now, let d1 denote the thickness from the bottom end of the non-piezoelectric element 23 concerning the thickness direction Z to the signal electrode 19 and d2 denote the thickness from the upper end to the lower end of the non-piezoelectric element 23. The thickness d2 is determined in accordance with the desired ultrasonic intensity. In this event, assume that the thickness D2 of the non-piezoelectric element 23 is constant. The second piezoelectric element portion 35 is a plate type piezoelectric element. On the upper surface of the second piezoelectric element portion 35, the earth electrode 21 is formed by sputtering, etc.
When drive signals are applied from an ultrasonic diagnostic apparatus body to the signal electrode 19, the first piezoelectric element portion 33 and the second piezoelectric element portion 35 vibrate in an integrated manner. Consequently, the basic resonance characteristics of the piezoelectric transducer 14 are determined on the basis of the thickness d1+d2 combining the overall thickness of the first piezoelectric portion element 33 and the thickness d3 of the second piezoelectric element portion 35 (length from the upper end of the non-piezoelectric element 23 to the earth electrode 21), that is, thickness D (D=d1+d+d3) of the piezoelectric element 17. In addition, the signal electrode 19 and the earth electrode 21 are formed on flat and uniform end surfaces of the first and second piezoelectric element portions 33 and 35, and therefore, as compared to conventional examples (Jpn. Pat. Appln. KOKAI Publication Nos. 2003-9288 and 2005-328507), they have high reliability in electrode connection.
Next description will be made on the sound pressure distribution by the ultrasonic probe 1.
The piezoelectric transducer 100 in the “conventional example” of
As shown in
Next, when the “piezoelectric transducer 14A,” “piezoelectric transducer 14B,” and “piezoelectric transducer 14C” are compared, it is obvious that the weighting effect varies in accordance with the length d2 of the non-piezoelectric element 23. The “conventional example” and the “piezoelectric transducer 14B” have substantially the same weighting effect but when the ratio of the length d2 of the non-piezoelectric element (groove) is compared, the “piezoelectric transducer 14B” is half the “conventional example.”
The foregoing simulation results indicate that stronger weighting effect can be obtained with shorter length d2 of the non-piezoelectric element 23 as compared to the conventional example.
Next, referring to
As shown in
Then, as shown in
As shown in
Next, as shown in
Thereafter, as shown in
Next, as shown in
Incidentally, the piezoelectric transducer 14′ which is manufactured in the manufacturing process S4 (
By the above-mentioned configuration, each piezoelectric element 17 is provided, in its inside, with a plurality of substantially strip-shape non-piezoelectric elements 23 disposed along the lens direction. Consequently, the piezoelectric element 17 can have two flat surfaces which substantially cross at right angles with the thickness direction Z, and which cannot be realized in the conventional example in which weighting is performed to change intensity distribution of ultrasonic waves. Because the electrodes are formed on the two flat surfaces, the electrode adhesion strength of the piezoelectric element 17 can be increased. In addition, the piezoelectric transducer 14 can be weighted as desired by the non-piezoelectric elements (grooves) 23 which are shorter than conventional ones, and therefore, the mechanical strength of the ultrasonic probe 1 and the piezoelectric transducer is improved. Consequently, according to the present embodiment, both the reliability of electrode formation and the yield can be improved.
Incidentally, the grooves 23 may not be filled with anything, though it has been stated that the grooves are filled with adhesives, etc.
In addition, the length d2 and the shape of the non-piezoelectric element 23 are not limited to the above-mentioned embodiments only. For example, as is the case of a piezoelectric transducer 51 shown in
Furthermore, as is the case of a piezoelectric transducer 53 shown in
Additional advantages and modifications will readily occur to those skilled in the art. Therefore, the invention in its broader aspects is not limited to the specific details and representative embodiments shown and described herein. Accordingly, various modifications may be made without departing from the spirit or scope of the general inventive concept as defined by the appended claims and their equivalents.
Number | Date | Country | Kind |
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2007-258899 | Oct 2007 | JP | national |
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Number | Date | Country |
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2003-9288 | Jan 2003 | JP |
2005-328507 | Nov 2005 | JP |
Number | Date | Country | |
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20090088643 A1 | Apr 2009 | US |