JPH08193987A - Ultrasonic probe - Google Patents

Abstract

PURPOSE: To enable a Fresnel lens to be applied to pulse ultrasonic wave. CONSTITUTION: An ultrasonic probe is provided with a refraction and line- focusing type acoustic Fresnel lens 1. The acoustic Fresnel lens 1 is bonded to an ultrasonic vibrator 2, and on both sides of the ultrasonic vibrator 2, a common electrode 3 and zone electrodes 4a, 4b, 4b', 4c, and 4c' divided while corresponding to zones a, b, b', c, and c' of the acoustic Fresnel lens 1, respectively, are disposed. To the zone electrodes 4a, 4b, 4b', 4c, and 4c', pulse signal generating circuits 5a, 5b, 5b', 5c, and 5c' excited by trigger signal, and delay circuits 6a, 6b, 6b', 6c, and 6c' which output to the pulse signal generating circuits 5a, 5b, 5b', 5c, and 5c' which delay a trigger signal by a specified time to correspond are connected. Delay time of each delay circuit 6a, 6b, 6b', 6c, and 6c' is set properly, and transmission time of ultrasonic wave is controlled for each zone 1, b, b', c, and c'.

Description

Detailed Description of the Invention

[0001]

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an ultrasonic probe, and more particularly to a probe having an acoustic lens and used in an ultrasonic diagnostic apparatus or the like.

[0002]

2. Description of the Related Art A device such as an ultrasonic microscope, an ultrasonic flaw detector, an ultrasonic diagnostic device for medical purposes, which obtains image information using ultrasonic waves, uses a plane wave-like ultrasonic wave generated by a flat plate-like ultrasonic vibrator. Acoustic lenses are used to focus the sound waves in a line or point.

However, there is attenuation in the propagation of ultrasonic waves in the acoustic lens, and the attenuation rate increases as the lens thickness increases. In particular, when the focal length is short and the aperture ratio of the lens is large, the maximum thickness of the lens is large. Further, in order to improve the imaging resolution by ultrasonic waves, it is necessary to increase the frequency of ultrasonic waves, but on the other hand, the propagation loss increases as the frequency increases, and the propagation loss increases as the thickness of the lens increases. growing.

Therefore, there is a demand for a thinner lens,
As one of the solutions, it has been proposed to use a refractive Fresnel lens.

In the case of using the refraction type Fresnel lens, in addition to the above advantages, the method for forming the lens has advantages. That is, in order to form the curved surface shape of the lens, generally, conventional machining techniques such as cutting and grinding are used, but when the lens shape is small and the curvature is small, it is difficult to improve the processing accuracy. The problem arises. On the other hand, beam processing using laser, ions, electrons, etc. is advantageous for fine processing, but since the processing speed is slow, particularly when the processing amount is large, the processing takes a lot of time.
Therefore, if a Fresnel lens is used to reduce the thickness of the lens and reduce the maximum unevenness, the amount of processing is reduced, so that beam processing or the like can be applied, and the range of processing technology is expanded.

[0006]

In designing the Fresnel lens, the steps between the individual zones are set so that the phases of the ultrasonic waves emitted from the individual zones forming the Fresnel lens coincide with each other at the focal position. Must be an integral multiple of the wavelength of.

However, the ultrasonic waves used in the above-mentioned devices such as ultrasonic flaw detectors are pulse ultrasonic waves containing a wide range of frequency components, and it is not possible to define a single wavelength to be used. FIG. 4 shows an example of the waveform of the pulsed ultrasonic wave actually used and its spectrum. In such a case,
For example, when the Fresnel lens is designed in accordance with the center frequency, that is, when the step is set, the phase of the other frequency components is deviated at the focal position and the intensity is weakened at the focal position due to the interference. Such a phenomenon is equivalent to that of a Fresnel lens operating as a frequency filter, and the pulse wave at the focal position has a smaller peak intensity and a longer pulse wavelength than the original waveform. The former leads to deterioration of signal strength and signal-to-noise ratio, and the latter leads to deterioration of resolution during distance measurement by the pulse echo method.

Therefore, conventionally, the Fresnel lens could not be applied to the pulsed ultrasonic waves.

An object of the present invention is to make a Fresnel lens applicable to pulse ultrasonic waves by controlling the oscillation timing of pulse ultrasonic waves for each individual zone that constitutes the Fresnel lens.

[0010]

According to a first aspect of the present invention, a refraction-type acoustic Fresnel lens, an ultrasonic transducer bonded to the acoustic Fresnel lens, and a common electrode for applying an electric field to the ultrasonic transducer. A zone electrode divided corresponding to each zone constituting the acoustic Fresnel lens, a pulse signal generation circuit provided corresponding to each zone electrode and excited by a trigger signal, and an individual pulse signal A delay circuit, which is provided corresponding to the generating circuit, delays the trigger signal for a predetermined time and outputs the delayed signal to the pulse signal generating circuit, and controls the ultrasonic wave transmission time for each zone. The ultrasonic probe is adopted.

According to a second aspect of the present invention, a refraction type acoustic Fresnel lens made of a conductive material, an ultrasonic transducer bonded to the acoustic Fresnel lens, and divisions corresponding to individual zones forming the acoustic Fresnel lens. Zone electrode,
A pulse signal generation circuit provided for each zone electrode and excited by a trigger signal, and a pulse signal generation circuit provided for each pulse signal generation circuit, delaying the trigger signal for a predetermined time And a delay circuit for outputting the ultrasonic wave, and controlling the transmission time of the ultrasonic wave for each individual zone.

According to a third aspect of the present invention, the ultrasonic transducer is made of a ceramic-based piezoelectric material and is divided corresponding to individual zones. Adopt a child.

According to a fourth aspect of the present invention, the individual zones are formed symmetrically with respect to each other, and a pair of pulse signal generating circuit and delay circuit are commonly provided for the two zones having the symmetrical relationship. The ultrasonic probe according to any one of claims 1 to 3 is adopted.

[0014]

In the ultrasonic probe according to the present invention, each delay circuit excites the corresponding pulse signal generating circuit by delaying the trigger signal for each zone. Here, the delay circuit is preset such that the delay time corresponding to the outer zone is shorter. Therefore, the outer zone is excited earlier than the inner zone. As a result, the ultrasonic pulses emitted from the individual zones reach the focal point at the same time, and the focusing effect similar to the emission from a single cylindrical surface can be obtained.

Further, although a step is formed between each zone, according to the ultrasonic probe of the first aspect, it is possible to obtain the coincidence of the focus positions by setting an appropriate delay time according to the step. Therefore, unlike the conventional acoustic Fresnel lens, it is not necessary to form a step by limiting it to an integral multiple of the wavelength of ultrasonic waves, and an arbitrary step can be set. Therefore,
The most desirable step can be selected from the viewpoint of processing technology.

From the above, according to the ultrasonic probe of the first aspect, it becomes possible to apply the Fresnel lens to the pulsed ultrasonic waves.

According to the ultrasonic probe of the second aspect, since the acoustic Fresnel lens is also used as the common electrode by using the conductive material for the acoustic Fresnel lens, it is necessary to separately provide the common electrode. Disappear.

According to the ultrasonic probe of the third aspect, since the ultrasonic vibrator is made of a ceramic-based piezoelectric material and is divided corresponding to each zone, the independence of vibration for each zone is maintained. can do.

According to the ultrasonic probe of the fourth aspect, by sharing a set of the pulse signal generating circuit and the delay circuit,
The circuit can be simplified.

[0020]

An embodiment of the present invention will be described below with reference to the drawings.

FIG. 1 shows the structure of an ultrasonic probe provided with a refraction type acoustic Fresnel lens, and FIG. 2 shows the appearance of the acoustic Fresnel lens.

In FIG. 1, the acoustic Fresnel lens 1 is
In addition to resins such as acrylic and polyimide, it is formed of quartz, sapphire, aluminum, or the like for high frequencies. The acoustic Fresnel lens 1 is composed of a line focusing type Fresnel lens, and comprises five zones a, b,
It is composed of b ', c, c'. Individual zones a, b,
The surface shape of b ′, c, c ′ is a cylindrical shape (cylindrical surface shape), and the individual zones a, b, b ′, c,
The ultrasonic waves emitted from c ′ are formed with different radii of curvature so that they are focused on the same focal point.

An ultrasonic transducer 2 is bonded to the back surface of the acoustic Fresnel lens 1. A common electrode 3 and a plurality of zone electrodes 4a, 4b, 4 are provided on both sides of the ultrasonic transducer 2.
b ', 4c, 4c' are formed. When a conductive material is used for the acoustic Fresnel lens 1, it is not necessary to separately provide the common electrode 3, and the acoustic Fresnel lens 1 can also be used as a common electrode. The individual zone electrodes 4a, 4b, 4b ', 4c, 4c' correspond to the individual zones a, b, b ', c, c'of the acoustic Fresnel lens 1.
It is formed corresponding to the pair 1. The ultrasonic transducer 2 is P
When a ceramic-based piezoelectric material typified by ZT is used, in order to maintain independence of vibration in each zone a, b, b ', c, c', dicing is performed along the boundary between adjacent zones. They are mechanically separated by doing so. The ultrasonic transducer 2 does not need to be separated as described above when a material having a large lateral vibration damping rate such as a polymer piezoelectric material typified by PVDF or a composite piezoelectric material is used. . In addition, as a material of the ultrasonic transducer 2,
In addition to the above piezoelectric material, a magnetostrictive material can also be used. In this case, the common electrode 3 and the zone electrode 4
Instead of a, 4b, 4b ', 4c, 4c', a coil for applying a magnetic field is arranged in each of the zones a, b, b ', c, c'.

Zone electrodes 4a, 4b, 4b ', 4c, 4
In some cases, a vibration damping material 7 is adhered to the back surface of c'for the purpose of reducing the ultrasonic pulse width to be transmitted, that is, improving the distance measurement resolution. As the vibration damping material 7, a rubber material in which a heavy metal such as tungsten is dispersed is used. Particularly, when the ultrasonic vibrator 2 is formed of a material having a small vibration damping rate such as a ceramic-based piezoelectric material, it is effective to connect the vibration damping material 7.

Individual zone electrodes 4a, 4b, 4b ', 4
c and 4c 'respectively include a pair of pulse signal generation circuits 5a, 5b, 5b', 5c, 5c 'and delay circuits 6a, 6c.
b, 6b ', 6c, 6c' are connected.

The pulse signal generation circuits 5a, 5b, 5b ',
5c and 5c 'are excited by the trigger signal, but when all the zones a, b, b', c and c'are excited at the same time, the ultrasonic pulse emitted from the outer zone reaches the focal position. The time is delayed. So, zones a, b,
Delay circuits 6a, 6b, 6b ', 6 for each of b', c, c '
The trigger signal is delayed by c and 6c ′, and the outer zone is excited earlier. As a result, the ultrasonic pulses emitted from the individual zones a, b, b ′, c, c ′ reach the focus position at the same time, and the focusing effect similar to the emission from a single cylindrical surface can be obtained. .

Delay circuits 6a, 6b, 6b ', 6c, 6
For c ′, either an analog delay line or a digital delay line may be used. In either case, the delay time becomes a discrete value, and the error in the delay time caused by this causes deterioration of the ultrasonic pulse waveform. But,
If the minimum unit of the delay time that can be set, that is, the quantization time is about 1/10 to 1/20 of the ultrasonic wave period, it is practically acceptable. As an example, Table 1 below shows delay time patterns given to the individual zones a, b, b ′, c, c ′ of the acoustic Fresnel lens 1. The value of the step in Table 1 is the gap value between the cylindrical surfaces on the axis of symmetry of the acoustic Fresnel lens 1. The delay time shown in Table 1 is given as follows. First, data corresponding to the delay time pattern is stored in the RAM in units of quantization time. Next, this data is sequentially read by the timing circuit. Here, the operating frequency of the timing circuit corresponds to the quantization time.

[0028]

[Table 1]

In the above-mentioned embodiment, the pulse signal generating circuits 5b and 5b 'and the delay circuits 6b and 6b' are provided independently for the left and right symmetrical zones, for example, b and b '. The pair of pulse signal generating circuits 5b and the delay circuit 6b may be shared and the output thereof may be branched and applied to the two zone electrodes 4b and 4b '. In this case, the circuit can be simplified. Note that the individual zones may be left-right asymmetrical as long as the focus positions can be matched.

Further, the zones a, b, and
The step between b ′, c, and c ′ does not need to be limited to an integral multiple of the wavelength of the ultrasonic wave as in the conventional acoustic Fresnel lens 1, and the focus position can be set by setting an appropriate delay time according to the step. Since the coincidence can be obtained, an arbitrary step can be set, and therefore, the step most desirable from the viewpoint of processing technology can be selected.

As described above, according to the above-described embodiment, the ultrasonic pulses emitted from the individual zones reach the focus positions at the same time, and the focusing effect similar to the emission from a single cylindrical surface can be obtained. it can. In addition, since the focus positions can be matched by setting an appropriate delay time according to the step, it is necessary to form the step by limiting it to an integral multiple of the wavelength of the ultrasonic wave as in the conventional acoustic Fresnel lens. However, it is possible to set an arbitrary step, and it is possible to select the most desired step from the viewpoint of processing technology. Therefore, according to the ultrasonic probe according to the above-mentioned embodiment, it becomes possible to apply the Fresnel lens to the pulse ultrasonic wave.

Next, the receiving operation will be described. When receiving the reflected signal from the object, each zone a, b,
It is necessary to add the same delay time as that at the time of transmission to the phase of the reflected signal for each of b ', c, c', and then overlap the reflected signal waveforms of the zones a, b, b ', c, c'. As a method of delaying the phase of the reflected signal, a method of delaying the analog signal as it is with an analog delay line, a method of digitizing with an A / D converter and delaying with a digital delay line,
Alternatively, when A / D converting and writing to the buffer memory, a method of delaying the start of A / D conversion with a preset counter and reading at the same timing can be used.

In the above-mentioned embodiment, the ultrasonic probe using the line-focusing type acoustic Fresnel lens 1 is shown. However, in the present invention, the point-focusing type acoustic Fresnel lens 1 as shown in FIG. The cross-sectional shape is the same as that of the line-focusing type acoustic Fresnel lens 1 of FIG. 1, but each zone a, b, c is formed concentrically, and the surface shape of each zone a, b, c is a cylindrical surface. The present invention can be easily applied to an ultrasonic probe using the acoustic Fresnel lens 1 having a spherical surface.

However, the point-focusing type acoustic Fresnel lens 1
In the case of the ultrasonic probe using, the zone electrodes 4a, 4b, 4c (not shown in FIG. 3) are also concentric according to the shapes of the zones a, b, c, so that the ultrasonic transducer is used. When a ceramic-based piezoelectric material is used as the material of 2, the ultrasonic transducer 2 needs to be concentrically divided along the zone electrodes 4a, 4b, 4c. However, curved processing is difficult in the processing method of cutting ceramics using a dicing cutter or the like. Therefore, in the case of an ultrasonic probe using the point-focusing type acoustic Fresnel lens 1, the zone electrodes 4a, 4
It is desirable that the ultrasonic transducer 2 be composed of a polymeric piezoelectric material or a composite piezoelectric material that does not require division of the ultrasonic transducers 2 and 4c.

[Brief description of drawings]

FIG. 1 is a configuration diagram of an ultrasonic probe according to an embodiment.

FIG. 2 is a perspective view of the acoustic Fresnel lens.

FIG. 3 is a perspective view of an acoustic Fresnel lens according to another embodiment.

FIG. 4 is a waveform diagram of pulsed ultrasonic waves and a spectrum diagram thereof.

[Explanation of symbols]

1 acoustic Fresnel lens 2 ultrasonic transducer 3 common electrode a, b, b ', c, c'zone 4a, 4b, 4b', 4c, 4c 'zone electrode 5a, 5b, 5b', 5c, 5c 'pulse signal Generating circuit 6a, 6b, 6b ', 6c, 6c' Delay circuit

Claims (4)

[Claims] 1. A refracting acoustic Fresnel lens, an ultrasonic transducer bonded to the acoustic Fresnel lens, a common electrode for applying an electric field to the ultrasonic transducer, and the acoustic Fresnel lens. Zone electrodes divided corresponding to individual zones, pulse signal generating circuits that are provided corresponding to individual zone electrodes and excited by a trigger signal, and pulse signal generating circuits that are provided corresponding to individual pulse signal generating circuits, An ultrasonic probe comprising: a delay circuit that delays the trigger signal for a predetermined time and outputs the delayed pulse signal to the pulse signal generating circuit, wherein the ultrasonic wave transmission time is controlled for each zone. 2. A refraction-type acoustic Fresnel lens made of a conductive material, an ultrasonic transducer bonded to the acoustic Fresnel lens, and zones divided corresponding to individual zones constituting the acoustic Fresnel lens. Electrode, pulse signal generating circuit provided for each zone electrode and excited by a trigger signal, and pulse signal generating circuit provided for each pulse signal generating circuit, by delaying the trigger signal for a predetermined time An ultrasonic probe comprising: a delay circuit for outputting to a signal generating circuit, and controlling an ultrasonic wave transmission time for each zone. 3. The ultrasonic probe according to claim 1, wherein the ultrasonic transducer is made of a ceramic-based piezoelectric material and is divided corresponding to each zone. 4. The individual zones are formed symmetrically with respect to each other, and a set of a pulse signal generating circuit and a delay circuit are commonly provided for the two zones having the symmetrical relationship. The ultrasonic probe according to any one of claims 1 to 3.