Apparatus for performing medical treatment by using electroacoustic transducer element

Abstract: An acoustic medical treatment apparatus is disclosed, which is designed to perform medial treatment with high efficiency and enhanced safety by using electroacoustic transducer elements (10). The apparatus includes a concave transducer for causing divided partial transducers to generate strong ultrasonic waves on a living body and detecting ultrasonic waves reflected by the living body, pulsers, arranged in correspondence with the partial transducers for driving them, a controller (60) for controlling the pulsers (20) to cause the concave transducer to emit the strong ultrasonic waves or weak ultrasonic waves, a reception system (30) for receiving reflected ultrasonic waves, which propagate in ultrasonic wave propagation paths between the partial transducers and an object to be irradiated in the living body, through the respective partial transducers, when weak ultrasonic waves are emitted from the concave transducer under the control of the controller, and processes the respective reception signals, and a monitor (50) for displaying information of the ultrasonic propagation paths by using each processed signal obtained by the reception system (30).

Description: The present invention relates to an apparatus for performing medical treatment by using the energy of a sound wave such as an ultrasonic wave generated by a piezoelectric element or an electroacoustic transducer element using electromagnetic induction and, more particularly, to an acoustic medical treatment apparatus such as a medical treatment apparatus (stone disintegration apparatus) for generating a shock wave (to be referred to as a strong ultrasonic wave hereinafter) by using, e.g., an electroacoustic transducer element, and disintegrating a stone (calculus) in a body by radiating the strong ultrasonic wave on the stone, or a medical treatment apparatus (hyperthermia apparatus) for radiating a continuous ultrasonic wave from an electroacoustic transducer element onto cancer cells in a body to as to perform thermotherapy of the cancer cells. A conventional acoustic medical treatment apparatus, e.g., a stone disintegration apparatus, is designed to radiate a strong ultrasonic wave from the outside of a body onto a stone, in a body, such as a renal calculus or a gallstone, so as to disintegrate it. In this stone integration apparatus, a concave transducer having a diameter of 30 to 40 cm is arranged in an applicator, and a strong ultrasonic wave is emitted from the convex transducer to a focal point. In this case, the applicator is positioned in relation to the body so as to match the focal position with the stone, and the stone is disintegrated by the energy of the strong ultrasonic wave. This concave transducer is a piezoelectric transducer, i.e. an electroacoustic transducer element, and radiates an ultrasonic narrow pulse wave from its concave surface. In addition, a tomographic imaging ultrasonic probe is to be inserted in a hole formed in the center of the concave transducer. Electronic sector scanning of each transducer of this ultrasonic probe is performed to display a tomographic image on a monitor. The position of the stone can be fixed to a desired position by observing the tomographic image. In this case, a strong ultrasonic wave propagates in the form of a cone. That is, the wave has a relatively large sectional plane near a body surface and is gradually focused on one point toward the stone. Owing to sector scanning, the image obtained by the ultrasonic probe has a sectorial shape. That is, the image is substantially observed as a point near the body surface and gradually spreads toward a given position in the body. For this reason, regions, near the surface of the living body of a patient, other than the above-mentioned point become blind regions. Therefore, even if the lungs or an intestinal tract or a bone is present in the radiation path of a strong ultrasonic wave near the body surface, it is not displayed on a tomographic image. In addition, since the tomographic image represents a sectional plane, regions other than this sectional plane are not displayed and constitute a large blind region. In order to display a stone as clearly as possible, the ultrasonic probe is preferably located as close to the stone as possible. With such an operation, however, the blind region is increased accordingly. For this reason, image display cannot be performed throughout the propagation path of a strong ultrasonic wave. Furthermore, a stone is normally located at a position several centimeters away from a body surface. If a bone, an intestinal gas, a portion of a lung, or the like is present in the propagation path of a strong ultrasonic wave, effective ultrasonic energy cannot be radiated on the stone. Moreover, a bone may be damaged, or an ultrasonic wave is reflected by a gas, so that the reflected wave scatters around. This may cause the living body to suffer from a pain or may inflict an injury on the living body. DE-A-37 36 733 discloses an acoustic medical treatment apparatus in accordance with the first part of claim 1. There, the applicator is connected to a focal point shifting means comprising a drive means for relocating the shock wave generator. Before starting the shock wave irradiation, obstacles between the calculus to be destroyed and the shock wave generator are detected, and ultrasonic transducer elements directed to such obstacles are kept inactive when transmitting the shock wave. It is an object of the present invention is to provide an acoustic medical treatment apparatus which uses electroacoustic transducer elements and can select a proper radiation path of a sound wave used for medical treatment. It is another purpose of the present invention to provide an acoustic medical treatment apparatus which uses electroacoustic transducer elements and can efficiently perform medical treatment without danger by easily determining the presence/absence of a bone, a gas, or the like by observing the state of a blind region, which cannot be observed on an image obtained by an imaging ultrasonic probe. In order to achieve the above object, there is provided an acoustic medical treatment apparatus in accordance with claim 1. Details of preferred implementations are mentioned in the subclaims. This invention can be more fully understood from the following detailed description when taken in conjunction with the accompanying drawings, in which: Fig. 1 is a block diagram showing only components, of a stone disintegration apparatus, associated with medical treatment, as an embodiment of an acoustic medical treatment using an electroacoustic transducer element according to the present invention; Fig. 2 is a block diagram showing a main part of a hyperthermia apparatus as an embodiment of the acoustic medical treatment apparatus using an electroacoustic transducer element according to the present invention; Fig. 3 is a block diagram showing an overall arrangement of an acoustic medical treatment apparatus, such as a stone integration apparatus or a hyperthermia apparatus, according to the first embodiment of the present invention, which is designed to radiate a sound wave on an upper portion of a living body, and specifically showing a system for independently controlling a section for medical treatment and a section for ultrasonic imaging; Fig. 4 is a block diagram showing an overall arrangement of an acoustic medical treatment apparatus, such as a stone integration apparatus or a hyperthermia apparatus, according to the first embodiment, which is designed to radiate a sound wave on a lower portion of a living body, and specifically showing a system for independently controlling a section for medical treatment and a section for ultrasonic imaging; Fig. 5 is a block diagram showing an overall arrangement of an acoustic medical treatment apparatus, such as a stone disintegration apparatus or a hyperthermia apparatus, according to the first embodiment, which is designed to radiate a sound wave on an upper portion of a living body, and specifically showing a system for collectively controlling a section for medical treatment and a section for ultrasonic imaging; Fig. 6 is a block diagram showing an overall arrangement of an acoustic medical treatment apparatus, such as a stone disintegration apparatus or a hyperthermia apparatus, according to the first embodiment, which is designed to radiate a sound wave on a lower portion of a living body, and specifically showing a system for collectively controlling a section for medical treatment and a section for ultrasonic imaging; Fig. 7 is a schematic plan view showing a concave transducer divided into a plurality of partial transducers mounted in an applicator of the stone disintegration apparatus; Fig. 8 is a schematic sectional view showing a positional relationship between a living body and an applicator in which a concave transducer, an ultrasonic probe, and the like are mounted; Fig. 9 is a view showing part of a display form for displaying the intensities of reception signals in a section for medical treatment; Fig. 10 is a view showing part of a display form for displaying the intensities of reception signals in the section for medical treatment; Fig. 11 is a view showing a display form, in accordance with claim 1, for displaying the intensities of reception signals in the section for medical treatment; and Fig. 12 is a schematic plan view showing another embodiment of an arrangement of concave transducers. Fig. 1 is a block diagram showing only components, of a stone disintegration apparatus, associated with stone disintegration, as an embodiment of an acoustic medical treatment apparatus according to the present invention. A stone disintegration apparatus having a general medical treatment (stone disintegration) function and an imaging function is realized by applying the arrangement shown in Fig. 1 to any one of acoustic medical treatment apparatuses shown in Figs. 3 to 6. Fig. 2 is a block diagram showing only components, of a hyperthermia apparatus, associated with hyperthermia treatment, as an embodiment of the acoustic medical treatment apparatus according to the present invention. A hyperthermia apparatus having a general medical treatment (hyperthermia treatment) function and an imaging function is realized by applying the arrangement shown in Fig. 2 to any one of the acoustic medical treatment apparatuses. Figs. 7 and 12 show concave transducers in these stone disintegration apparatus and hyperthermia apparatus. Fig. 8 shows a positional relationship between a living body and an applicator in the stone disintegration apparatus or the hyperthermia apparatus. In addition, Figs. 9 to 11 respectively show display forms for displaying the intensities of reception signals in the stone disintegration apparatus or the hyperthermia apparatus. An arrangement of a stone disintegration apparatus of this embodiment, which is specified by Figs. 1, 3, 7, and 8, will be described below. The components for stone disintegration shown in Fig. 1 include a concave transducer 10 comprising electroacoustic transducer elements, a driving system 20 including pulsers 22 (22-1 - 22-20), a receiving system including limiters 32 (32-1 - 32-20), preamplifiers 34 (34-1 to 34-20), signal processing circuits 36 (36-1 to 36-20), and a summing processing circuit 38, a digital scan converter DSC 40 including a freeze button 40A, a monitor 50, and a control system 60 (60A) including a rate pulse generator 62 and a controller 64. A stone disintegration apparatus shown in Fig. 3 comprises the components for stone disintegration, which includes the concave transducer 10, the driving system 20, the receiving system 30, the DSC 40, the monitor 50, and the control system 60 (60A) shown in Fig. 1, and a tomographic imaging system for imaging a sector tomographic image (B mode image), which includes an image ultrasonic probe 70, a transmitting system 72, a DSC 76, a monitor 78, and an imaging controller 60B. Each component for stone disintegration will be described below. The concave transducer 10 is constituted by, e.g., a piezoelectric element having a concave surface and is arranged in an applicator 12 shown in Fig. 3 or 8. The concave transducer 10 is driven by the pulsers 22 to emit a strong ultrasonic pulse (shock wave) or a weak ultrasonic pulse. As shown in Fig. 7, the concave transducer 10 consists of two annular members, which are in contact with each other. These annular members are divided into a plurality of different partial transducers. For example, the outside annular member of the concave transducer 10 is divided into 12 equal portions (al, a2, a12), while the inside annular member is divided into 8 equal portions (b1, b2, ... b8). That is, the concave transducer 10 is divided into 20 portions as a whole. These partial transducers (al - a12, b1 - b8) are electrically connected to the pulsers 22 constituting the driving system 20 and to the limiters 32, each serving as an element of the reception system 30. As shown in Fig. 3 or 8, the applicator 12 is equipped with the concave transducer 10, a medium, e.g., water 14, a rubber film 16 for sealing the water 14, the ultrasonic probe 70, a mechanism (not shown) for operating the ultrasonic probe 70, and the like. A strong ultrasonic pulse emitted from the concave transducer 10 propagates to a kidney 82 through the water 14, the rubber film 16, and a body surface 80A of a living body 80. As shown in Fig. 8, the ultrasonic wave propagates in the form of a cone. That is, the sectional plane of the wave is wide near the concave transducer 10 and gradually narrows toward a stone 84. This is because the transducer 10 has a concave sound wave emission surface and is constituted by an annular member. The ultrasonic probe 70 is inserted in a hole in the center of the concave transducer 10 and is sector-scanned by the transmitting system 72 to monitor the position of the stone 84 existing in the kidney 82. When sector scanning of the ultrasonic probe 70 is performed, a tomographic image of a sectorial plane or slice 72 around the stone 84 in the kidney 82 can be obtained on the monitor 78. The sectional plane 72 of sector scanning by the ultrasonic probe 70 gradually broadens downward to constitute a sectorial plane. Referring to Fig. 1, the rate pulse generator 62 generates a rate pulse of several Hz and supplies it to each pulser 22. The pulsers 22 constituting the driving system 20 drive the respective partial transducers (a1 - b8) arranged on the concave transducer 10 in response to the rate pulse supplied from the rate pulse generator 62. The partial transducers (a1 - b8) are respectively driven by the pulsers 22 to emit ultrasonic pulses. The ultrasonic pulses propagate in the living body 80. The controller 64 supplies signals for controlling outputs from the pulsers 22. For example, the controller 64 controls the following modes: a large output pulse mode for generating a strong ultrasonic pulse; a partially large output pulse mode for causing only some of the partial transducers to generate strong ultrasonic pulses; a small output pulse mode for generating weak ultrasonic pulses for monitoring; a selective driving mode for selectively driving the partial transducers; and a stop mode for stopping a pulse output operation. The respective partial transducers al to a8 detect ultrasonic waves reflected by the living body 80 and output electrical signals to the preamplifiers 34 through the limiters 32. Each limiter 32 performs a limiting operation with respect to the echo signal input from a corresponding partial transducer so as to obtain only a desired signal component. Each preamplifier 34 amplifies the desired echo signal component input from a corresponding limiter 32 to a predetermined level. Each signal processing circuit 36 detects the amplified signal input from a corresponding preamplifier 34 by using an envelope detector, performs level adjustment of an obtained signal for a tomographic image, further performs signal processing such as A/D conversion (analog/digital conversion), and supplies the processed signal to the DSC (digital scan converter) 40. The DSC 40 has a frame memory and writes the processed signal, input from each signal processing circuit 36, in the frame memory. More specifically, the DSC 40 writes the respective processed signals in the frame memory by using address signals (not shown) in correspondence with the respective partial transducers, thus forming image patterns shown in Figs. 9 to 11. In addition, the DSC 40 converts the scan format of each processed signal written in the frame memory from the ultrasonic scan format to, e.g., the standard TV scan format, and, at the same time, supplies the image pattern to the monitor 50. An operation of this embodiment having the above-described arrangement will be described below. The controller 64 is set in the stop mode, and a bag 16 of the applicator 12 is brought into contact with the body surface 80A of the living body 80. Subsequently, sector scanning is performed by the ultrasonic probe 70 to display a tomographic image on the monitor 78 shown in Fig. 3. Furthermore, the applicator 12 is moved to superpose an image of the stone 84 on the tomographic image. The position and angle of the applicator 12 are then set to position the focal point of the concave transducer 10 on the stone 84. The controller 64 is set in the small output pulse mode so that the partial transducers al to b8 are respectively driven by the pulsers 22 to emit weak ultrasonic pulses. Ultrasonic waves reflected by the living body 80 and received by the partial transducers al to b8 are added/processed by the addition processing circuit 38. The obtained signal is output to the monitor 50 through the DSC 40. As a result, reflection caused by the stone 84 can be detected through the monitor 50. In this case, since the distance from the concave transducer 10 to the focal position is constant, pulses which fall within a certain range of time required for a pulse emitted from the concave transducer 10 to propagate to the focal position and return to the transducer 10 (about 133 µs per 10 cm) are detected. When the stone 84 and the focal point coincide with each other, a strong reflected pulse is detected. At the same time, reflected wave signals received by the partial transducers al to b8 reflectively pass through the pulsers 22, limiters 32, the preamplifiers 34, and the signal processing circuits 36 and are input to the DSC 40. These signals are then displayed on the monitor 50 by various display schemes. A first display pattern displayed on the monitor 50 will be described later. The intensities of waves reflected by the stone 84 are subjected to luminance modulation in the signal processing circuits 36. The modulated signals are then written in the DSC 40 in correspondence with the positions of the partial transducers al to b8. Reflected wave data is read out from the DSC 40 to be displayed on the monitor 50 in correspondence with the levels of luminance (brightness). If no obstacles, e.g., a gas or bones, are present in propagation paths between the stone 84 and given partial transducers, strong reflected waves such as waves al', ..., a5', a7', and a12' are received in accordance with the given partial transducers, as shown in Fig. 9. As a result, the luminances of portions, of the display pattern displayed on the monitor 50, corresponding to the given transducers, are increased. If obstacles are present in the propagation paths of ultrasonic waves, weak reflected wave outputs (an example is shown in Fig. 10), such as wave outputs a6', a8', a10', and a11', or a9', are detected in accordance with the sizes and qualities of the obstacles. As a result, the luminances of portions, of the display pattern on the monitor 50, corresponding to the transducers which receive the weak reflected waves, are decreased. Since the luminance of a signal is changed depending on the intensity of reflection, the state of an obstacle in a propagation path can be easily obtained by checking this luminance. Instead of the luminance display scheme, a flicker display scheme may be employed, in which the frequency of flicker is increased with a decrease in reflection intensity. In this case, each partial transducer is required to have an area (opening) large enough to ensure a sufficient focusing effect so that ultrasonic waves from the respective partial transducers propagate in their own paths without overlapping much. A second display pattern of the intensities of waves reflected by the stone 84 will be described below with reference to Fig. 10 which, however, does not form part of claim 1. Referring to Fig. 10, the amplitudes of signals received by the partial transducers al to b8 are properly processed by the signal processing circuits 36, and the obtained outputs are plotted along the axis of ordinate of the monitor 50. In addition, time t after the emission of a pulse, i.e., a distance from a partial transducer, is set on the axis of abscissa of the monitor 50. With this setting, the intensity of a reflected wave received by each partial transducer is displayed. In the case shown in Fig. 10, since signals a'' 1 , a'' 2 , and b'' 8 received by the partial transducers a 1 , a 2 , and b 8 exhibit no strong reflected waves in the paths from the partial transducers to the stone (focal point F 0 ), it can be determined that no special large obstacles exist. However, since a strong reflecting object, e.g., an intestinal gas, is present midway along the propagation path between the partial transducer and the stone, strong reflection occurs at the object. As a result, it is detected that the energy of an ultrasonic wave reaching the stone is reduced, and reflection by the stone is weakened. A display pattern of the intensities of reflected waves, in accordance with claim 1, will be described below with reference to Fig. 11. This display pattern includes a pattern of the concave transducer, which is viewed from its upper surface, and a perspective pattern obtained by viewing the propagation paths of ultrasonic waves between the concave transducer and the stone or the focal point F 0 when viewed from the side of the perspective pattern. Referring to Fig. 11, the propagation paths of ultrasonic waves are divided into regions (T 1 - F 0 ), (T 2 - F 0 ), ... (T 6 - F 0 ). The intensities of ultrasonic waves shown in Fig. 9 are luminance-modulated in units of the divided paths and are displayed on the monitor 50. In this case, a substantially perspective image is displayed. For example, therefore, an addition average signal based on the area ratios of signals received by the partial transducers a 2 , a 3 , a 4 , and a 5 , which fall within a region T 1 , is used for the regions (T 1 - F 0 ). In this case, since the area ratios are: a 2 : a 3 : a 4 : a 5 = 0.3 : 0.9 : 0.9 : 0.3 an addition average signal is given by: (a'' 2 × 0.3 + a'' 3 × 0.9 + a'' 4 × 0.9 + a'' 5 × 0.3) + 2.4. For the regions T 2 , ... T 6 , addition average signals are obtained in the same manner as for the region T 1 . The regions T 1 , ... T 6 may be divided into smaller regions. In this embodiment, since a large obstacle exists midway along the path on the left end in relation to an observer (the path of the partial transducer a 9 ), strong reflection is indicated at the corresponding portion, and the reflection is weakened in the subsequent portion of the path, i.e., from the obstacle to the focal point F 0 . As is apparent from strong reflection in the region T 3 , an obstacle is present in the path of the partial transducer a 6 . By simultaneously observing the display pattern in Fig. 9 and the display pattern obtained by viewing the concave transducer from its upper surface in Fig. 11, an operator can easily detect a three-dimensional positional relationship between an obstacle and the concave transducer. If the perspective display pattern in Fig. 11, which is obtained by viewing the propagation paths, is displayed while superposing it on a tomographic image obtained by the ultrasonic probe, a relationship between an organ and the path of a radiated ultrasonic wave can be easily detected. These superposed images can be intermittently frozen by the freeze button 40A shown in Fig. 1 so as to prevent wasteful emission of ultrasonic waves. By monitoring this state, the applicator 12 can be set at an optimal position, in relation to the living body, at which only a few obstacles are present. In this case, the focal point is matched with the stone, and the display patterns in Figs. 9 to 11 are displayed. An optimal applicator position where the focal point always coincides with the stone can be easily set by rotating a support mechanism (not shown) of the applicator 12 about the focal position. After the optimal position is determined in this manner, the controller 64 is set in the large output pulse mode to emit strong ultrasonic waves. If an obstacle in a propagation path cannot be avoided, the controller 64 is set in the partial large output pulse mode to stop emission of strong ultrasonic waves from partial transducers corresponding to the path in which the obstacle is present and to cause other partial transducers to emit strong ultrasonic waves. This operation may be manually performed. However, driving of the corresponding partial transducers can be automatically stopped on a condition that the intensities of waves reflected by the stone, which are shown in, e.g., Fig. 9 or 10, are equal to or lower than a predetermined value. In addition, an indication which is controlling flickeringly active (on-driving) electroacoustic transducer elements and a representation of echo waves as shown Fig. 9 to Fig. 11 are superimposed on each other and displayed. Therefor, an operator can clearly understand which transducers are off-driven or on-driven. In this method, therefore, radiation of unnecessary strong ultrasonic waves into a living body can be prevented. This increases the safety of a living body and relieves a pain. The shapes and number of partial transducers are not limited to those shown in Fig. 1. For example, circular partial transducers may be used, as shown in Fig. 12. In addition, each partial transducer may be constituted by a combination of a plurality of transducers. If one partial transducer is constituted by a combination of smaller transducers, the degree of freedom in combination is greatly increased to allow finer control. The above-described embodiment is associated with the method of independently receiving reception signals in units of partial transducers. However, since the directivity of transmission is the same as that of reception, the same effect as described above can be obtained by independently transmitting signals from the respective partial transducers. More specifically, the partial transducers a 1 , a 2 , ... are sequentially driven by the controller 64 in the small output pulse mode. A reflected wave may be received by a corresponding partial transducer at each driving operation, or may be received by all the transducers, and the received waves are used as signals respectively corresponding to the paths of the partial transducers. In the above embodiment, stone disintegration is exemplified. However, the present invention is not limited to stone disintegration and can be equally applied to, e.g., an ultrasonic hyperthermia treatment and a treatment for cancer by strong ultrasonic waves. In this case, a strong ultrasonic wave may be a pulse wave or a continuous wave. This will be described later. In the above embodiment, a piezoelectric transducer is exemplified as a means for generating a strong ultrasonic wave. However, an element based on electromagnetic induction may be used. Such an element is designed such that a metal plate is placed on a spiral coil. When a large current is instantaneously supplied to the coil, a shock wave is generated from a surface of the metal plate. Therefore, the same arrangement as that of the concave transducer shown in Fig. 1 can be realized by using a plurality of such elements as partial transducers. In this case, in order to increase the sensitivity of a reception signal, reception signals received by a plurality of electromagnetic induction partial transducers may be used. Alternatively, piezoelectric elements may be arranged between the partial transducers, and a combination thereof may be used. Furthermore, in the above embodiment, the intensities of reflected waves are displayed in correspondence with luminance modulation. However, the intensities of reflected waves may be displayed by, e.g., a color display scheme. The stone disintegration apparatus specified by Figs. 1 and 3 has been described above. As shown in Fig. 3, this stone disintegration apparatus is designed to radiate a shock wave on an upper portion of a living body and, more specifically, represents a system for independently controlling a section for stone disintegration and a section for ultrasonic imaging. An applicator 12 is arranged in a living body 80. The system includes a convex electroacoustic transducer element controller 60A and an imaging controller 60B. As shown in Fig. 4, a stone disintegration apparatus specified by Figs. 1 and 4 is designed to radiate a shock wave on a lower portion of a living body and, more specifically, represents a system for independently controlling a section for stone disintegration and a section for ultrasonic imaging. An applicator 12 is arranged under a living body 80. The system includes a concave electroacoustic transducer element controller 60A and an imaging controller 60B. As shown in Fig. 5, a stone disintegration apparatus specified by Figs. 1 and 5 is designed to radiate a shock wave on an upper portion of a living body and, more specifically, represents a system for collectively controlling a section for stone disintegration and a section for ultrasonic imaging. An applicator 12 is arranged on a living body 80. The system includes a collective control system 60'. As shown in Fig. 6, a stone disintegration apparatus specified by Figs. 1 and 6 is designed to radiate a shock wave on a lower portion of a living body and, more specifically, represents a system for collectively controlling a section for stone disintegration and a section for ultrasonic imaging. An applicator 12 is arranged under a living body. The system includes a main control system 60'. Fig. 2 is a block diagram showing only components, of a hyperthermia apparatus, associated with a hyperthermia treatment, as an embodiment of the acoustic medical treatment apparatus according to the present invention. In the arrangement shown in Fig. 2, the pulsers 22 constituting the driving system 20 in Fig. 1 are replaced by continuous wave generation drivers 24, thus constituting a section for a hyperthermia treatment. Figs. 2 and 3 show an overall arrangement of the hyperthermia apparatus. As shown in Fig. 3, this hyperthermia apparatus is designed to radiate a continuous wave or a burst wave on an upper portion of a living body and, more specifically, represents a system for independently controlling a section for a hyperthermia treatment and a section for ultrasonic imaging. An applicator 12 is arranged on a living body 80. The system incudes a concave electroacoustic transducer element controller 60A and an imaging controller 60B. As shown in Fig. 4, a hyperthermia apparatus specified by Figs. 2 and 4 is designed to radiate a continuous wave or a burst wave on a lower portion of a living body and, more specifically, represents a system for independently controlling a section for a hyperthermia treatment and a section for ultrasonic imaging. An applicator 12 is arranged under a living body 80. The system includes a concave electroacoustic transducer element controller 60A and an imaging controller 60B. As shown in Fig. 5, a hyperthermia apparatus specified by Figs. 2 and 5 is designed to radiate a continuous wave on an upper portion of a living body and, more specifically, represents a system for collectively controlling a section for a hyperthermia treatment and a section for ultrasonic imaging. An applicator 12 is arranged on a living body 80. The system includes a main control system 60'. As shown in Fig. 6, a hyperthermia apparatus specified by Figs. 2 and 6 is designed to radiate a continuous wave on a lower portion of a living body and, more specifically, represents a system for collectively controlling a section for a hyperthermia treatment and a section for ultrasonic imaging. An applicator 12 is arranged under a living body 80. The system includes a main control system 60'. Each of the hyperthermia apparatuses respectively specified by Figs. 2 and 3, Figs. 2 and 4, Figs. 2 and 5, and Figs. 2 and 6 may use the concave transducer shown in Fig. 7 or 12. In addition, Fig. 8 shows a positional relationship between a living body and the applicator in each of the hyperthermia apparatuses. Furthermore, the display forms shown in Figs. 9 to 11 can be used as display forms for displaying the intensities of reception signals in these hyperthermia apparatuses. According to the present invention, a transducer is divided into a plurality of partial transducers. Weak ultrasonic waves are respectively emitted from these partial transducers, and the reflected waves are respectively detected by the partial transducers to be displayed. Therefore, the state of a propagation path connecting each partial transducer to a focal point can be easily detected, thus eliminating blind regions. With this operation, a shock wave or a continuous wave for medical treatment can be emitted after an optimal propagation path is easily selected and confirmed, thereby providing an acoustic medical treatment apparatus using an electroacoustic transducer element, which can greatly reduce the adverse effects, of unnecessary reflection of waves by a bone, a lung, or an intestinal gas, on a patient, and a pain in a living body, can enhance the safety, and allows efficient medical treatment.

Claims: An acoustic medical treatment apparatus, using electroacoustic transducer elements, for causing said electroacoustic transducer elements to radiate a sound wave on a morbid portion in a living body so as to perform medical treatment with energy of the sound wave radiated on the morbid portion, comprising: sound wave generating means (10), having a plurality of said electroacoustic transducer elements arranged to form a concave surface for forming a focal point, for causing said respective electroacoustic transducer elements to generate sound waves upon application of voltages to said electroacoustic transducer elements; driving control means (20) for driving/controlling said plurality of electroacoustic transducer elements to selectively generate sound waves for medical treatment and sound waves for non-treatment; reception means (30) for receiving electrical signals coming from said electroacoustic transducer elements which receive reflected sound waves when said sound wave generating means (10) has been driven by said driving control means (20) to generate sound waves for non-treatment; and generating/display means (40, 50, 60) for generating information associated with sound wave propagation paths between said plurality of electroacoustic transducer elements and the focal point on the basis of the electrical signals received by said reception means (30); characterized in that the generating/display means (40, 50, 60) display the generated information in a display pattern including a first pattern of the arrangement of said electroacoustic transducer elements and a second, perspective pattern obtained by viewing the propagation paths of the sound waves between said electroacoustic transducer elements and the focal point (F 0 ), said second pattern including an indication of detected obstacles. An apparatus according to claim 1, characterized in that said sound wave generating means (10) is arranged in an applicator (12) having a bag (16) in which an ultrasonic propagation medium is stored, said bag (16) being arranged to be brought into contact with a body surface of a living body. An apparatus according to claim 1, characterized in that said sound wave generating means (10) includes a plurality of electroacoustic transducer elements arranged to form an annular shape. An apparatus according to claim 1, characterized in that said sound wave generating means (10) includes a plurality of electroacoustic transducer elements arranged as dots. An apparatus according to any of claims 1 to 4, characterized in that said driving control means (20) drives/controls said plurality of electroacoustic transducer elements to selectively generate strong ultrasonic waves as shock waves for disintegrating a stone and ultrasonic waves for detecting propagation paths of the strong ultrasonic waves. An apparatus according to any of claims 1 to 4, characterized in that said driving control means (20) drives/controls said plurality of electroacoustic transducer elements to selectively generate strong ultrasonic waves as shock waves for a hyperthermia treatment and ultrasonic waves for detecting propagation paths of the strong ultrasonic waves. An apparatus according to any of claims 1 to 6, characterized in that the apparatus further comprises an imaging ultrasonic probe (70) inserted in a substantially central portion of said concave surface of said sound wave generating means (10) along an axial direction toward the focal point, said probe (70) including a large number of small ultrasonic transducers; and tomographic imaging means (60B, 72, 74, 76, 78) for scanning/driving each of said ultrasonic transducers of said ultrasonic probe (70) to generate a tomographic image, and for displaying the tomographic image. An apparatus according to claim 7, characterized in that the display pattern generated by said detecting means (40, 50, 60) and the tomographic image obtained by said tomographic imaging means (70, 72, 74, 76, 78, 60B) are displayed in correspondence with each other. An apparatus according to claim 7 or 8, characterized in that said driving control means (20) also controls transmission/reception operations of said tomographic imaging means (60B, 72, 74, 76, 78). An apparatus according to claim 7, 8 or 9, wherein said tomographic imaging means (60B, 72, 74, 74, 76, 78) generates a sector tomographic image, and displays the sector tomographic image.

Inventors: IINUMA KAZUHIRO, IINUMA, KAZUHIRO, IINUMA, KAZUHIRO, C/O INTELLECTUAL PROPERTY DIV.
Applicants: TOSHIBA KK, KABUSHIKI KAISHA TOSHIBA
Application year: 1991
Main classification: A61B17
IPC codes: A61B18, A61B8, A61B17