JP2013103064A - Acoustic wave acquisition device - Google Patents

Abstract

PROBLEM TO BE SOLVED: To provide a technique, in an acoustic wave acquisition device, for reducing a blind region while suppressing the deterioration of image quality.SOLUTION: The acoustic wave acquisition device is used which includes: a holding plate that holds a subject; a sound detecting means that detects an acoustic wave that is transmitted across the holding plate from the subject; a scanning means that scans the sound detecting means on the holding plate; an angle changing means that changes the angle of the direction, in which the sound detecting means detects the acoustic wave, to the holding plate; and a control means that controls the scanning means and the angle changing means according to the position of a measurement site in the subject.

Description

  The present invention relates to an acoustic wave acquisition apparatus.

  In the medical field, apparatuses using ultrasonic waves that can non-invasively image the inside of a living body are widely used. A general ultrasonic diagnostic apparatus can obtain information inside a living body by transmitting ultrasonic waves and receiving ultrasonic waves reflected inside the living body. This makes it possible to find a disease site such as cancer, but in order to further improve the detection efficiency, imaging of physiological information of a living body, that is, functional information, has attracted attention. Photoacoustic Tomography (PAT) that uses light and acoustic waves has been proposed as an imaging means for functional information.

  Photoacoustic tomography uses a photoacoustic effect in which an object is irradiated with pulsed light generated from a light source, and an acoustic wave (typically, an ultrasonic wave) is generated by absorption of light propagated and diffused in the object. This is a technique for imaging the internal tissue that is the source of acoustic waves. When near-infrared light is used for pulsed light, the near-infrared light easily penetrates the water that makes up most of the living body and is easily absorbed by hemoglobin in the blood, so it images blood vessels. be able to. Furthermore, blood oxygen images in blood, which is functional information, can be measured by comparing blood vessel images with pulsed light of different wavelengths and calculating the ratio of oxyhemoglobin and deoxyhemoglobin. Since blood around malignant tumors is considered to have lower oxygen saturation than blood around benign tumors, knowing oxygen saturation makes it possible to distinguish between good and bad tumors.

  Since the ultrasonic diagnostic apparatus and the photoacoustic tomography apparatus use an acoustic wave, it is necessary to consider matching of acoustic wave impedance so that the acoustic wave efficiently propagates from the acoustic wave generation source to the acoustic wave detector. The acoustic wave is reflected at the interface of the object, and the reflectivity depends on the acoustic impedance, which is the product of the density of the substance and the propagation sound velocity. At this time, if the acoustic impedances of the substances on both sides of the interface are close to each other, that is, if matching is achieved, acoustic waves are less likely to be reflected and propagate easily. Conversely, if the acoustic impedance is greatly different, the acoustic wave is reflected and the propagation efficiency is poor.

JP 2004-57823 A

When measuring a wide range of a subject such as a living body, as shown in FIG. 1, the subject 3 is held by a flat subject holding plate 4, and the acoustic detector 5 is parallel to the subject holding plate 4. It is effective to perform scanning while changing the position sequentially.
When a round part such as a breast of a living body is handled as a measurement part of the subject, a gap is created between the subject 3 and the subject holding plate 4 at the peripheral portion, and the acoustic impedance is greatly different from that of the subject 3. Air may enter. Since the acoustic wave does not propagate when there is a gap, the acoustic detector 5 cannot receive the acoustic wave, and a blind region 3c where internal information cannot be obtained is formed. Although it is conceivable to fill the gap with water, gel, or the like whose acoustic impedance is close to that of the subject 3, this places a burden on the subject.
Further, a structure 18 that supports the body and the holding plate is required at the base of the breast. However, in order to maintain the strength of the apparatus, it is difficult to use a material having an acoustic impedance close to that of the subject 3 for the structure 18. Therefore, an acoustic wave cannot propagate and the blind area | region 3a is made.

  In order to reduce the blind area while measuring a wide range of the subject, it is conceivable to use sector scan in addition to linear scan as disclosed in Patent Document 1. However, since the element of the acoustic detector has directivity, sensitivity to an acoustic wave with an angle becomes low. For this reason, there is a limit to the angle of sector scanning, and the S / N ratio (signal-to-noise ratio) is poor even at an acquired angle. Furthermore, the sector scan has a problem that the resolution becomes worse as the measurement site goes to the back side of the subject.

  The present invention has been made on the basis of such problem recognition. An object of the present invention is to provide a technique for reducing blind areas while suppressing deterioration of image quality in an acoustic wave acquisition apparatus.

The present invention employs the following configuration. That is,
A holding plate for holding the subject;
Acoustic detection means for detecting an acoustic wave propagating from the subject across the holding plate;
Scanning means for scanning the acoustic detection means on the holding plate;
An angle changing means for changing an angle with respect to the holding plate in a direction in which the acoustic detecting means detects an acoustic wave;
Control means for controlling the scanning means and the angle changing means in accordance with the position of the measurement site in the subject;
It is an acoustic wave acquisition device characterized by having.

  ADVANTAGE OF THE INVENTION According to this invention, in the acoustic wave acquisition apparatus, the technique for reducing a blind area | region can be provided, suppressing deterioration of an image quality.

It is a figure explaining background art. 1 is a schematic diagram illustrating a configuration of an apparatus according to a first embodiment. It is a figure which shows installation of the apparatus which concerns on Embodiment 1. FIG. It is a figure which shows the implementation method of the apparatus which concerns on Embodiment 1. FIG. 3 is a flowchart showing an operation of the apparatus according to the first embodiment. FIG. 6 is a schematic diagram illustrating a configuration of an apparatus according to a second embodiment. 6 is a flowchart showing an operation of the apparatus according to the second embodiment. It is a schematic diagram which shows the structure of the apparatus which concerns on Embodiment 3. FIG. 10 is a flowchart showing the operation of the apparatus according to the third embodiment. FIG. 6 is a schematic diagram illustrating a configuration of an apparatus according to a fourth embodiment. 10 is a flowchart illustrating the operation of the apparatus according to the fourth embodiment. FIG. 10 is a schematic diagram illustrating a configuration of an apparatus according to a fifth embodiment. 10 is a flowchart showing the operation of the apparatus according to the fifth embodiment. 10 is a graph showing acoustic wave detection according to the third embodiment.

  Hereinafter, preferred embodiments of the present invention will be described with reference to the drawings. However, the dimensions, materials, shapes, and relative arrangements of the components described below should be changed as appropriate according to the configuration of the apparatus to which the invention is applied and various conditions. It is not intended to limit the following description.

The acoustic wave acquisition apparatus of the present invention transmits ultrasonic waves to a subject, receives reflected waves (echo waves) reflected within the subject, and acquires characteristic information in the subject as image data. Includes equipment using echo technology. Further, it includes an apparatus using a photoacoustic effect that receives acoustic waves generated in the subject by irradiating the subject with light (electromagnetic waves) and acquires characteristic information as image data.
In the case of an apparatus using the former ultrasonic echo technique, the acquired characteristic information is information reflecting the difference in acoustic impedance of the tissue inside the subject. In the case of an apparatus using the latter photoacoustic effect, the acquired characteristic information is light source distribution of acoustic waves generated by light irradiation, initial sound pressure distribution in the subject, or light derived from the initial sound pressure distribution. Energy absorption density distribution, absorption coefficient distribution, and concentration distribution of substances constituting the tissue are shown. The concentration distribution of the substance is, for example, an oxygen saturation distribution or an oxidized / reduced hemoglobin concentration distribution at a measurement site.

  The acoustic wave referred to in the present invention is typically an ultrasonic wave, and includes an elastic wave called a sound wave, an ultrasonic wave, or an acoustic wave. An acoustic wave generated by the photoacoustic effect is called a photoacoustic wave or an optical ultrasonic wave. The acoustic detector receives an acoustic wave generated or reflected in the subject.

[Embodiment 1]
In Embodiment 1, a basic embodiment of the present invention will be described. FIG. 2 is a block diagram showing components of the apparatus according to this embodiment. In the present embodiment, the invention is applied to a photoacoustic tomography apparatus using a photoacoustic effect. The apparatus includes a light source 1, a light irradiation device 2, an object holding plate 4, an acoustic detector 5, a scanning mechanism 6, an angle changing mechanism 7, an interlock control device 8, an electric signal processing device 9, a data processing device 10, and a display device 11. including. The measurement target of the apparatus is the subject 3.

(light source)
The light source 1 is a device that generates pulsed light. As a light source, a laser is desirable to obtain a large output, but a light emitting diode or the like may be used. In order to generate photoacoustic waves effectively, light must be irradiated in a sufficiently short time according to the thermal characteristics of the subject. When the subject is a living body, the pulse width of the pulsed light generated from the light source 1 is preferably set to several tens of nanoseconds or less. The wavelength of the pulsed light is in the near infrared region called a biological window, and is preferably about 700 nm to 1200 nm. The light in this region can reach relatively deep in the living body, and information on the deep portion can be obtained. If it is limited to the measurement of the surface of the living body, the visible light to near infrared region of about 500 to 700 nm may be used. Further, it is desirable that the wavelength of the pulsed light has a high absorption coefficient with respect to the observation target.

(Light irradiation device)
The light irradiation device 2 is a device that guides the pulsed light generated by the light source 1 to the subject 3. Specifically, it is an optical device such as an optical fiber, a lens, a mirror, or a diffusion plate. Further, when these optical devices guide pulsed light, the shape and optical density of the pulsed light may be changed. The optical apparatus is not limited to those described here, and may be any apparatus as long as it satisfies the required functions.

(Subject)
The subject 3 is a measurement target. As the subject 3, a living body or a phantom (simulated living body) that simulates the acoustic characteristics and optical characteristics of the living body is mainly used. For example, if the purpose is to examine breast cancer, the subject is a living breast. The acoustic characteristics are specifically the propagation speed and attenuation rate of acoustic waves, and the optical characteristics are specifically the light absorption coefficient and scattering coefficient. A light absorber having a large light absorption coefficient needs to be present inside the subject 3 as a measurement site. Specific examples of the light absorber include hemoglobin, water, melanin, collagen, and lipid in the case of a living body. In the case of a phantom, a substance simulating the optical characteristics of the above is enclosed inside as a light absorber.

(Subject holding plate)
The subject holding plate 4 is a flat plate that holds the subject. The material of the subject holding plate 4 is preferably a material having an acoustic impedance close to that of the subject 3. The subject holding plate 4 is placed in close contact with the subject 3. At this time, gel or the like is applied to avoid an air layer between the subject 3 and the subject holding plate 4. However, as described above as a problem, when a living body is used as a subject, the marginal portion does not adhere to the subject and a void is generated.

(Acoustic detector)
The acoustic detector 5 converts an acoustic wave into an analog electric signal. The acoustic detector 5 is installed on the opposite side of the subject 3 with the subject holding plate 4 interposed therebetween. At this time, in order to propagate the acoustic wave satisfactorily, it is necessary to perform acoustic impedance matching between the subject holding plate 4 and the acoustic detector 5, so it is desirable to fill a matching solution between them. Although it is desirable to fill the matching solution in the closed space, the matching solution may always flow between the subject holding plate 4 and the acoustic detector 5 without closing the space.
In photoacoustic tomography, since acoustic waves must be captured at a plurality of locations, the acoustic detector is preferably a 2D type in which a plurality of receiving elements are arranged on a plane. However, a single element type or a 1D type acoustic detector in which receiving elements are arranged in a line may be moved to a plurality of locations by using the scanning mechanism 6. It is desirable that the acoustic detector has high sensitivity and a wide frequency band. Specific examples include an acoustic detector using a PZT, PVDF, cMUT, and Fabry-Perot interferometer. However, the present invention is not limited to those listed here, and any one that satisfies the required function may be used.

(Scanning mechanism)
The scanning mechanism 6 is a mechanism that scans the acoustic detector 5. The scanning is performed in parallel with the subject holding plate 4. The scanning mechanism is preferably an electric stage equipped with a stepping motor or the like, but may be a manual stage. It is desirable that scanning can be performed two-dimensionally. However, the present invention is not limited to those listed here, and any one that satisfies the required function may be used.

(Angle change mechanism)
The angle changing mechanism 7 is a mechanism that changes the angle of the acoustic detector 5 with respect to the subject holding plate 4. By changing the angle, a gap is formed between the acoustic detector 5 and the subject holding plate 4, but acoustic impedance matching can be maintained by filling the gap with an acoustic matching liquid. Although it is desirable that the angle changing mechanism can be changed electrically, it may be manually operated.

(Interlocking control device)
The interlock control device 8 controls the scanning and angle of the acoustic detector in conjunction with each other. Therefore, the interlock control device 8 has a function of controlling the scanning mechanism 6 and the angle changing mechanism 7. The feature of the present invention is to control the scan and the angle in association with each other, and the control method will be described in detail later.

(Electric signal processing device)
The electric signal processing device 9 amplifies the analog electric signal obtained by the acoustic detector 5 and converts it into a digital signal. In order to efficiently acquire data, it is desirable that there are as many analog-digital converters (ADCs) as the number of receiving elements of the acoustic detector, but one ADC may be connected in sequence.

(Data processing device)
The data processor 10 reconstructs image data by processing the digital signal obtained by the electrical signal processor 9. That is, the characteristic information in the subject is generated as image data based on the digital signal. Specific examples of the data processing apparatus include a computer and an electric circuit. The processing method at this time is preferably a universal back projection method in which the differentiated signals are superimposed, but any method can be used as long as it can reconstruct an image. When the acoustic wave propagation speeds of the object holding plate and the object are different, the acoustic wave is refracted according to the angle. Therefore, it is desirable to correct it and perform reconstruction.

(Display device)
The display device 11 displays the image data generated by the data processing device 10. Specifically, a display such as a computer or a television can be mentioned.

  The installation of the subject 3, the subject holding plate 4, the acoustic detector 5, the scanning mechanism 6, and the angle changing mechanism 7 will be described with reference to FIG. FIG. 3 also shows an acoustic wave receiving surface 5 a of the acoustic detector 5, pulse light 16, an effective reception area 17 by the acoustic detector 5, an apparatus structure 18, and a matching solution 19. The subject 3 is divided into an area A (3a) at the base of the breast, an area C (3c) at the tip of the breast, and an intermediate area B (3b).

  The pulsed light 16 generated by the light source 1 and guided by the light irradiation device 2 is irradiated onto the subject 3 from the upper part of FIG. An acoustic detector 5 is installed so as to sandwich the subject holding plate 4 with respect to the subject 3. The space between the subject holding plate 4 and the acoustic detector 5 is filled with a matching solution 19, and the matching solution 19 is held in a closed space including the subject holding plate 4 and a matching solution holding plate (not shown). . The acoustic detector 5 includes an angle changing mechanism 7 and a scanning mechanism 6, and the closed space that holds the matching solution 19 moves in conjunction with the scanning of the acoustic detector 5.

The acoustic detector 5 has an effective reception area 17 that can effectively detect an acoustic wave propagating from the subject. When performing electronic linear scanning, the effective reception area 17 may be an area in front of the acoustic wave receiving surface 5a of the acoustic detector 5. When the electronic sector scan is performed, the effective reception area 17 extends in an oblique direction, but the depth dependency of the resolution becomes higher than that in the linear scan, and the image quality varies depending on the location.
Alternatively, the effective reception area may be determined as an angle within a predetermined range from the direction in which the acoustic wave can be detected with the maximum sensitivity according to the directivity and sensitivity of the receiving element. Further, it may be determined as an angle within a range in which an acoustic wave can be received with a predetermined ratio of intensity compared to the intensity of the acoustic wave received with the maximum sensitivity. When the effective reception area is defined by the sensitivity of the receiving element as described above, an acoustic wave that is detected within a predetermined angle range or an acoustic wave that is detected with a predetermined ratio of intensity is effectively received. It can be called a wave. In the case of an acoustic detector in which receiving elements are arranged on the acoustic wave receiving surface, the normal direction of the acoustic wave receiving surface is usually the direction with the highest sensitivity. In this case, the angle changing mechanism changes the angle of the acoustic detector by changing the direction in which the acoustic wave receiving surface receives the acoustic wave.

When the acoustic detector 5 is kept in front of the subject 3 while scanning the left until the acoustic detector 5 hits the structure 18 until it hits the structure 18, the region A (3 a) cannot be scanned any more. It does not enter the effective reception range 17 and becomes a blind area. On the other hand, the area B (3b) can be measured because it enters the effective reception area 17 even when the angle of the acoustic detector 5 is kept in front. The region C (3c) is a blind region in which a gap is generated between the subject holding plate 4 and the subject 3, and measurement cannot be performed while keeping the angle of the acoustic detector 5 in front. In this way, when the angle of the effective reception area 17 of the acoustic detector 5 with respect to the subject 3 remains fixed in a substantially vertical direction from the front of the subject 3, that is, the subject holding plate 4, the acoustic wave is received. There are a wide range of blind areas 3a and 3c that cannot be performed.

  Next, with reference to FIGS. 4 and 5, a control method in which scanning of the acoustic detector 5 and angle change performed by the interlock control device 8, which is a feature of the present invention, are interlocked will be described. For the sake of simplicity, a plan view will be described, but the extension to three dimensions can be realized by increasing the dimension of scanning and angle by one.

  FIG. 4 shows the positional relationship between the subject 3 and the acoustic detector 5 and the angle of the acoustic detector 5 in each step of the flowchart of FIG. Hereinafter, description will be made while associating FIGS. 4A to 4F with the step numbers of FIG. In addition, the determination method of the angles 1-3 used for description here and the positions 1-6 is explained in full detail behind.

First, as shown in FIG. 4A, preparation for acquiring data of the area A (3a) is performed. For this purpose, the angle of the acoustic detector 5 is set to the angle 1 by the angle changing mechanism 7 (step S1). Next, the position of the acoustic detector 5 is set to position 1 by the scanning mechanism 6 (step S2).
As shown in FIG. 4B, the scanning mechanism 6 scans the acoustic detector 5 to the position 2 while keeping the angle 1. During scanning, the operation of irradiating the subject 3 with the pulsed light 16 and acquiring the signal by the acoustic detector 5 is repeated at regular intervals (step S3). At this time, it is desirable to irradiate the pulsed light 16 in a concentrated manner on the region A (3a), but the light may be irradiated to the entire subject in order to diffuse in the living body.

Next, as shown in FIG.4 (c), the preparation which acquires the data of the area | region B (3b) is performed. Therefore, the angle of the acoustic detector 5 is set to the angle 2 (step S4), and the position is set to the position 3 (step S5).
As shown in FIG. 4D, the scanning mechanism 6 scans the acoustic detector 5 to the position 4 while maintaining the angle 2. During scanning, the operation of irradiating the subject 3 with the pulsed light 16 and acquiring the signal by the acoustic detector 5 is repeated at regular intervals (step S6). At this time, it is desirable to irradiate the pulsed light 16 in a concentrated manner on the effective receiving area 17 and move the pulsed light 16 in the same manner as the effective receiving area 17 is scanned. However, the entire subject may be irradiated.

Further, as shown in FIG. 4E, preparation is made for acquiring data of the region C (3c). Therefore, the angle of the acoustic detector 5 is set to the angle 3 (step S7), and the position is set to the position 5 (step S8).
As shown in FIG. 4 (f), the scanning mechanism 6 scans the acoustic detector 5 to the position 6 while maintaining the angle 3. During scanning, the operation of irradiating the subject 3 with the pulsed light 16 and acquiring signals is repeated at regular intervals (step S9). At this time, it is desirable to irradiate the pulsed light 16 in a concentrated manner on the region C (3c), but it may be applied to the entire subject.

  The data processing apparatus 10 performs reconfiguration based on the finally obtained data and displays the result (step S10). When data is acquired with the area A or the area C as a measurement object, the area B is also in the effective reception area, so that a signal is also obtained from the area B. That is, the region B includes a region where a signal has been acquired a plurality of times. It is desirable to reconstruct the location where the signal is obtained a plurality of times by using all the signals of the measurement signal when the region is not the measurement target and the measurement signal when the region is the measurement target. However, each measurement may be reconstructed using only the measurement signal, and a superimposition process such as taking the average value or root mean square of the voxel intensity of the obtained images may be performed.

  As described above, the blind area data can be acquired by controlling the angle and the scanning in conjunction with each other. As a result, since the blind area is linearly scanned at a constant angle, the resolution is the same in all areas, and an easy-to-view image is obtained.

  Angles 1 to 3 and positions 1 to 6 are determined as follows. The angle is defined by the angle formed by the normal of the acoustic wave receiving surface of the acoustic detector and the normal of the subject holding plate. That is, it is defined by the direction of the effective reception area and the direction of the normal line of the subject holding plate. When the acoustic detector is facing the front, that is, the angle 2 is 0 degree. The case where the acoustic detector faces the front indicates a state where the acoustic wave receiving surface of the acoustic detector faces the subject holding plate.

The angle 1 and the angle 3 are in the range of 0 degree or more and less than 90 degrees, and the larger the area is (the closer it is parallel to the subject holding plate), the smaller the blind area. Therefore, it is better that the angle is large, but the upper limit of the angle is determined by the following constraint conditions.
One of the constraint conditions is total reflection at each interface of the subject 3, the subject holding plate 4, and the matching solution. When total reflection occurs at any interface, the signal in the subject 3 is not transmitted to the acoustic detector. In order to avoid this, the angle must be made gentle (toward the 0 degree side), and the upper limit of the angle of the acoustic detector is determined by the total reflection condition. The total reflection condition is calculated by using the speed of sound when an acoustic wave propagates through each member and Snell's law. If all the sound speeds of the respective members are the same, there is no total reflection condition, and total reflection does not occur at any angle.

Furthermore, there is another constraint for angle 1 and angle 3 respectively. Comparing this constraint condition with the upper limit of the angle due to total reflection described above, the smaller angle becomes the upper limit.
As for the angle 1, if the angle is too gentle, the effective reception area of the acoustic detector passes through the gap generated between the subject 3 and the subject holding plate 4, and the acoustic wave is not transmitted. Therefore, the angle of the acoustic detector when the effective reception area passes through the upper right end of area A and passes through the lower left end of area C as shown in FIG. 4B is another upper limit.
For the angle 3, if the angle is too gentle, the left upper end of the region C must be scanned further to the left and hit the structure. Therefore, the angle at which the effective reception area passes through the upper left end of the area C when the acoustic detector is closest to the structure as shown in FIG.

  The positions 1 to 6 are determined so that the overlapping of the scanned area of the effective reception area with the area A, the area B, and the area C is maximized when scanning is performed at an angle 1, an angle 2, and an angle 3, respectively.

  According to the above method, almost all blind regions can be imaged, and an image with uniform resolution can be obtained over the entire region.

[Embodiment 2]
When the subject is a living body, there are individual differences in the shape, and it is difficult to maintain with good reproducibility, so the relationship between the angle and the scanning changes with each measurement. In the present embodiment, a method of automatically determining the angle and position of the first embodiment by obtaining the outer shape of the subject with a camera or the like will be described.

  FIG. 6 is a block diagram of the apparatus of this embodiment. The apparatus of the present embodiment is configured by adding a form acquisition device 12 and an angle / position determination device 13 to the configuration of the first embodiment. Specifically, the form acquisition device 12 is a camera, a three-dimensional scanner, or the like, and can obtain form information of an object, that is, an outline. For example, if the shape of the breast margin is acquired, the region of the gap can be determined by combining it with the shape of the subject holding plate. Alternatively, by analyzing an image acquired by the camera, a non-contact portion between the breast and the subject holding plate can be determined. Moreover, the positional relationship between the subject and the structure of the apparatus can be analyzed based on the image, and the range in which the acoustic detector can be scanned can be determined.

The form information is sent to the angle / position determination device 13, and the angle / position determination device 13 automatically determines the angles 1, 3, and positions 1-6. Assume that angle 2 is fixed at 0 degrees. The determined angles 1 and 3 and positions 1 to 6 are sent to the interlock control device 8. The functions of other components are the same as those in the first embodiment.
It is the same.

FIG. 7 is a flowchart of this embodiment. A different part from the flow of Embodiment 1 shown in FIG. 5 is demonstrated.
First, the form information of the subject is acquired by the form acquisition device 12 (step S11). The acquired portable information is transmitted to the angle / position determination device 13.
Subsequently, the angle / position determination device 13 determines the angles 1, 3 and the positions 1 to 6 based on the form information (step S12). Using the angles 1 and 3 and the positions 1 to 6 thus determined, photoacoustic measurement is performed according to steps S1 to S10 in the same manner as in the first embodiment.

  According to the above method, the control method in which the angle and the position of the acoustic detector are linked can be automatically determined, and the blind region can be acquired more easily.

[Embodiment 3]
When the subject holding plate is not transparent, it is difficult to optically measure the contact portion between the subject and the subject holding plate with a camera or the like. Even if the subject holding plate is transparent, it may be difficult to accurately measure the contact site. In this embodiment, a method for acquiring contact information based on an acoustic wave signal will be described.

FIG. 8 is a block diagram showing the configuration of the apparatus of this embodiment. The apparatus of the present embodiment is configured by adding a contact determination device 14 to the apparatus of the second embodiment. In the contact determination device 14, the contact portion is determined using the digital signal obtained by the electrical signal processing device.
Normally, when pulsed light is irradiated onto a living body interface, a large acoustic wave is generated at the interface, and a large photoacoustic signal (electric signal) based on the acoustic wave is generated. However, since an acoustic wave is not propagated in a portion where the subject and the subject holding plate are not in contact, no photoacoustic signal is detected. Since the interface signal propagating from an oblique direction is detected by the acoustic detector, the propagation time is calculated from the sound velocity in the object holding plate, and the signal of the time at which the interface signal in front of the acoustic detector propagates is calculated. By examining, the front contact of the acoustic detector can be determined. At this time, the pulsed light needs to be irradiated near the boundary interface between the subject and the subject holding plate. Further, the angle of the acoustic detector needs to be set at an angle of 2, that is, 0 degree.

FIG. 9 is a flowchart showing this embodiment. First, the operation of irradiating pulsed light and acquiring signals while scanning the entire area at an angle 2 is repeated at regular intervals (step S13). Contact information is acquired from the obtained signal using the above-described method in the contact determination device 14 (step S14).
The contact information is sent to the angle / position determination device 13 and integrated with the information (step S12) obtained from the form acquisition device 14 to determine the angle and position (step S12). Thereafter, similarly to the flow of the second embodiment illustrated in FIG. 7, the processes of steps S11 to S10 are performed.

  According to the above method, the contact portion can be calculated more accurately, the automatic setting of the wrong angle and position can be reduced, and the measurement can be performed more efficiently.

[Embodiment 4]
As described in the first embodiment, when the incident angle of the acoustic wave with respect to the interface is increased, that is, when the acoustic wave is angled, total reflection of the acoustic wave occurs. Even if the total reflection is not reached, the transmittance through the subject holding plate is lowered due to the angle. In the present embodiment, a method for correcting the influence due to the angle is described.

  FIG. 10 is a block diagram showing the configuration of the apparatus according to this embodiment. The components of the apparatus are the same as those in the first embodiment, but angle information is sent from the interlock control apparatus 8 to the data processing apparatus 10.

  FIG. 11 shows a processing flow performed in this embodiment. Since the content of the reconstruction process is different from that in the first embodiment, step S10 is described in detail. Steps S1 to S9 are performed in the same manner as in the first embodiment.

  In the present embodiment, in the three-dimensional space, the obtained signal is converted in the axis in consideration of the propagation speed (step S10-1), and back-projected from the acoustic detector position (step S10-3). The obtained image data is displayed (step S10-4). Here, the backprojection specifically refers to drawing a reverse signal in a concentric sphere centered on the position of the acoustic detector. In the present embodiment, processing for correcting the transmittance and the refractive index according to the angle from the acoustic detector is performed on the signal to be backprojected. Therefore, in the data processing device 10, the transmittance is calculated by calculating the transmittance for each angle based on the angle information obtained from the interlock control device 8, and dividing the signal projected to the angle by the transmittance. The influence of the decrease in the correction is corrected (step S10-2). Note that steps S10-1 and S10-2 may be interchanged. Then, processing is performed in the order of back projection (step S10-3) and image display (step S10-4).

  According to the above method, since the difference in transmission of the acoustic wave according to the angle of the acoustic detector can be corrected, an image having the same contrast in all regions can be obtained.

[Embodiment 5]
An embodiment in which the present invention is applied to an ultrasonic apparatus such as an ultrasonic diagnostic apparatus will be described. In photoacoustic tomography, the subject is irradiated with light, but in the ultrasonic apparatus, ultrasonic waves are transmitted to the subject. Further, in the photoacoustic tomography, the light absorber is imaged as a measurement site, but in the ultrasonic apparatus, a portion having a different acoustic impedance is imaged as a measurement site.

  FIG. 12 is a block diagram showing the configuration of the apparatus of this embodiment. Compared with the first embodiment, the light source 1 and the light irradiation device 2 are eliminated, and an acoustic transceiver 15 is provided instead of the acoustic detector 5. The acoustic transmitter / receiver 15 is a device that transmits an acoustic wave, receives an acoustic wave reflected in the subject, and converts it into an electrical signal, and includes a scanning mechanism 6 and an angle changing mechanism 7.

FIG. 13 is a flowchart showing the flow of processing of this embodiment.
In order to measure the area A, the acoustic wave transmitting / receiving apparatus is set to an angle 1 and a position 1 (steps S1 and S2). While scanning up to position 2, the acoustic transceiver 15 transmits and receives ultrasonic waves. The received signal is processed and imaged by the electrical signal processing device 9 (step S15).
Similarly, in order to measure the region B, the sound detector is set at the angle 2 and the position 3 (steps S4 and S5). While scanning up to position 4, ultrasonic waves are transmitted and received and imaged (step S16).
Further, in order to measure the region C, the sound detector is set at an angle 3 and a position 5 (steps S4 and S5). While scanning up to position 6, ultrasonic waves are transmitted and received and imaged (step S17).
The finally obtained images are connected to display an image (step S18).

  According to the above method, even in the ultrasonic apparatus, most of the blind area can be imaged, and an image with uniform resolution over the entire area can be obtained.

[Embodiment 6]
In the present embodiment, a method for acquiring data from more blind areas will be described. The components of the apparatus and the flow of processing are basically the same as those in the first embodiment.

The photoacoustic wave generated in the light absorber inside the subject 3 isotropically spreads, and the side surface of the subject 3 toward the surface opposite to the subject holding plate 4 when viewed from the light absorber. Also propagate. Here, the outside of the subject 3 is normal air, and the acoustic impedance differs greatly between the subject and air. For this reason, the photoacoustic wave propagated to the opposite side of the subject holding plate 4 as viewed from the light absorber is reflected at the interface between the subject and air and propagates toward the subject holding plate 4. As a result of the reflected acoustic wave being received by the acoustic detector, a reflected wave is obtained with a delay from the direct wave from the source of the photoacoustic wave.

  As described in the first embodiment, the angle of the acoustic detector is limited by the total reflection of the acoustic wave at the interface between the subject and the subject holding plate, the gap between the subject and the subject holding plate, and the arrangement of the structures. For this reason, in the direct wave, there is a region where no signal is obtained in the vicinity of the subject holding plate in the blind region. However, if a reflected wave is used, a signal can be obtained from such a region.

  When reconstruction is performed including a signal from a reflected wave, a mirror image by reflection appears on the opposite side of the subject from the reflection interface. Therefore, a process for folding the reconstructed image at the reflection interface is performed, and a superimposition process for taking the average or the root mean square of the images overlapped by the folding is performed. Here, the description has been made on the assumption that the periphery of the subject is air. However, when the acoustic impedance is close to that of a living body such as water, it is necessary to provide a reflector. In addition, it is desirable to install a reflector and shape the reflection interface into a flat surface so that the object is close to regular reflection even when the subject is air.

  According to the above method, the blind area can be further reduced and completely eliminated depending on conditions such as an angle.

[Example 1]
Examples in which the effects of the present invention have been confirmed through experiments will be described. The subject is a simulated living body and has a breast shape and a light absorber inside. The subject holding plate is polymethylpentene having a thickness of 6.8 mm. The acoustic detector was installed so that the distance between the acoustic detector surface and the surface of the subject holding plate was 15 mm, and the distance from the acoustic detector surface to the rotation axis of the angle changing mechanism was 5 mm. The space between the acoustic detector and the subject holding plate was filled with water.
At this time, the thickness of the subject (perpendicular to the subject holding plate) is 50 mm, and the width (parallel to the subject holding plate) is 115 mm. Of the subject, the width of the blind region due to the structure supporting the subject holding plate is 20 mm, and the width of the blind region due to the subject being separated from the subject holding plate due to roundness is 35 mm.

  The acoustic detector is a 2D array acoustic detector having a frequency band of 1 MHz ± 40%, and the elements of the array are 2 mm wide, 2 mm pitch, 10 × 10 in a row. The light source is an Nd: YAG laser, and irradiates the subject from the opposite side of the subject holding plate with nanosecond-order pulse light having a wavelength of 1064 nm. In the present embodiment, the angle and position of the acoustic detector are set based on the form information obtained from the camera.

The settings of the angles 1 to 3 and the positions 1 to 6 (see FIG. 4) of the acoustic detector are as follows. The position is defined at the center of the acoustic detector, and the origin is position 3.
Angle 1:35 degrees, angle 2: 0 degrees, angle 3:35 degrees.
Position 1: 15 mm, Position 2: 35 mm, Position 3: 0 mm, Position 4: 40 mm, Position 5: 5 mm, Position 6: 20 mm.

  While changing the angle and scanning the acoustic detector using the above settings, pulsed light irradiation, acoustic wave reception, electrical signal amplification, and digital-analog conversion were performed at regular intervals to obtain a digital signal. The ADC used at this time has a sampling frequency of 20 MHz and a resolution of 12 bits. The light absorbers were imaged by averaging the digital signals of the respective elements and performing image reconstruction processing in consideration of refraction and reflection.

  As a result, when the measurement was performed only with the linear scan that is the conventional method, only the region B could be measured. By implementing this method, the image quality of 90% of the region A and 65% of the region C was deteriorated. Was able to get without.

[Example 2]
In this example, the result of contact determination using the method described in Embodiment 3 from a signal acquired by measurement will be described. The apparatus was set up in the same manner as in Example 1. Then, the entire area of the subject is scanned with the angle of the acoustic detector being 0 degree, and pulsed light irradiation, acoustic wave reception, electric signal amplification, and digital / analog conversion are performed at regular intervals to obtain a digital signal. It was. Since the acoustic wave propagation velocity in polymethylpentene is 2200 m / s and the acoustic wave propagation velocity in water is 1500 m / s, the signal after 13.1 μs after pulse light irradiation represents the interface between the subject and the subject holding plate. ing.

FIG. 14A shows an example of a signal obtained when the acoustic detector is placed in front of a position where the simulated living body and the subject holding plate are not in contact with each other. On the other hand, FIG. 14B shows a case where the acoustic detector is placed in front of the position where the simulated living body and the subject holding plate are in contact.
As shown in FIG. 14B, when the simulated living body is in contact with the subject holding plate, the signal level of 13.1 μs is lowered to the baseline level because light does not wrap around. On the other hand, as shown in FIG. 14A, when the simulated living body and the subject holding plate are not in contact with each other, a signal is observed at the time of 13.1 μs due to the light wrapping around.

FIG. 14C shows the signal level of the obtained digital signal after 13.1 μs from the irradiation of the pulsed light for each position. The signal obtained after the position 42 mm (65 or more on the horizontal axis in the figure) was higher than the baseline. Therefore, it was found that 42 mm is an accurate boundary between the region B and the region C.
Therefore, the angles 1 to 3 and the positions 1 to 6 were set as follows. Angle 1:35 degrees, angle 2: 0 degrees, angle 3:35 degrees, position 1:15 mm, position 2:35 mm, position 3: 0 mm, position 4:42 mm, position 5: 5 mm, position 6:22 mm. Thereafter, signals were acquired and image reconstruction processing was performed in the same manner as in Example 1 to image the light absorber.

  As described above, the boundary between the region B and the region C can be obtained with high accuracy by performing the contact determination based on the signal as in the present embodiment. By using this result, it is possible to appropriately determine the position and angle of the acoustic detector, and it is possible to obtain a good image.

[Example 3]
An embodiment in which the entire blind area is imaged using a reflector will be described. In addition to the setup of Example 1, a reflector was installed so that the simulated living body was sandwiched between the subject holding plate and the reflector. The material of the reflector is glass and the acoustic impedance is 16.0 [MRayl]. Since the acoustic impedance of the simulated living body is 1.5 [MRayl], 83% of the photoacoustic wave generated from the simulated living body and propagating toward the reflecting plate is reflected at the interface with the glass and is reflected on the acoustic detector. Propagate toward. Since the pulsed light is almost transmitted through the glass, the irradiation with the pulsed light can be performed in the same manner as in the first embodiment.

  Angles 1 to 3 and positions 1 to 6 were set in the same manner as in Example 1. While scanning, pulsed light irradiation, electrical signal amplification, and digital / analog conversion were performed at regular intervals to obtain a digital signal. . At this time, the digital signal was acquired until 100 μs after pulse light irradiation.

When image reconstruction processing is performed using this signal, light absorption including the real image by the photoacoustic wave directly propagating to the acoustic detector and the mirror image by the photoacoustic wave propagating to the acoustic detector via the reflector. A body image was obtained. In the obtained image, when the acoustic detector is in front and the reflection plate is in the back, the region deeper than 50 mm from the boundary surface with the subject holding plate is a mirror image region composed only of mirror images. . The mirror image area is folded back so as to be line-symmetric with a line of 50 mm from the boundary surface with the subject holding plate, and an average value is obtained with each voxel in the real image area 50 mm before the boundary surface with the subject holding plate to absorb light I got a picture of my body.

  By this method, the entire area could be imaged and the blind area could be eliminated.

  4: subject holding plate, 5: acoustic detector, 6: scanning mechanism, 7: angle changing mechanism, 8: interlocking control device

Claims (15)

A holding plate for holding the subject;
Acoustic detection means for detecting acoustic waves propagating from the subject through the holding plate;
Scanning means for scanning the acoustic detection means on the holding plate;
An angle changing means for changing an angle with respect to the holding plate in a direction in which the acoustic detecting means detects an acoustic wave;
Control means for controlling the scanning means and the angle changing means in accordance with the position of the measurement site in the subject;
An acoustic wave acquisition apparatus comprising: The acoustic detection means has an effective reception area that is an area in which acoustic waves can be effectively detected in the direction of detecting acoustic waves,
2. The sound according to claim 1, wherein the angle changing unit changes an angle of the acoustic detection unit in a direction in which an acoustic wave is detected with respect to the holding plate by changing a direction of the effective reception area. Wave acquisition device. The acoustic detection means has a plurality of receiving elements arranged on an acoustic wave receiving surface,
The acoustic wave acquisition apparatus according to claim 2, wherein the effective reception area is an area in front of the acoustic wave reception surface. The acoustic wave acquisition apparatus according to claim 2, wherein the effective reception area is a range in which a reception element included in the acoustic detection unit can receive an acoustic wave with a predetermined sensitivity. The acoustic detection unit detects an acoustic wave propagating from the measurement site when the direction of the effective reception area of the acoustic detection unit is a normal direction of the holding plate among the measurement sites in the subject. If the measurement area that cannot be measured is a blind area,
The control means controls the angle changing means and the scanning means so that the effective reception area covers the blind area when the measurement site is included in the blind area. The acoustic wave acquisition apparatus of any one of these. In the blind region, there is a structure at a position where the acoustic wave propagated from the measurement site in the direction of the normal line of the holding plate passes through the holding plate, so that the scanning unit scans the acoustic detection unit. The acoustic wave acquisition apparatus according to claim 5, wherein the acoustic wave acquisition apparatus is an area where it cannot be performed. The blind region is a region in which an acoustic wave from a measurement site does not propagate in a normal direction of the holding plate due to a gap between the subject and the holding plate. The acoustic wave acquisition device described in 1. When the measurement site is included in the blind area, the control means controls the scanning means so that the acoustic detection means is not included in the area facing the blind area, and the direction of the effective reception area is the blind area. The acoustic wave acquisition apparatus according to any one of claims 5 to 7, wherein the angle changing means is controlled so as to be in a certain direction of the region. It further has a form acquisition means for acquiring the form of the subject,
The acoustic wave acquisition according to any one of claims 1 to 8, wherein the control unit controls the scanning unit and the angle changing unit based on the configuration information acquired by the configuration acquisition unit. apparatus. The control means acquires contact information between the subject and the holding plate from an acoustic wave detected by the acoustic detection means, and controls the scanning means and the angle changing means based on the contact information. The acoustic wave acquisition apparatus according to any one of claims 1 to 9. 11. The acoustic wave acquisition apparatus according to claim 1, further comprising a data processing unit that generates characteristic information in the subject based on an acoustic wave detected by the acoustic detection unit. The data processing means acquires angle information with respect to the holding plate for each acoustic wave detected by the acoustic detection means, and corrects a decrease in transmittance of the acoustic wave by the holding plate using the angle information. The acoustic wave acquisition apparatus according to claim 11. A reflection plate installed on the opposite side of the holding plate across the subject;
The acoustic detection means detects an acoustic wave generated at a measurement site in the subject and reflected by the reflecting plate,
13. The acoustic wave acquisition apparatus according to claim 11, wherein the data processing unit generates characteristic information using an acoustic wave reflected by the reflecting plate. 14. The acoustic according to claim 1, wherein the acoustic wave propagating from the subject is a photoacoustic wave generated from a light absorber in the subject irradiated with light. Wave acquisition device. 14. The acoustic wave propagating from the subject is an acoustic wave that is reflected from the acoustic wave transmitted from the acoustic detection means within the subject. 14. Acoustic wave acquisition device.

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