Patent Application
20130267820
1. Field of the Invention
The present invention relates to a subject information obtaining apparatus and a subject information obtaining method for obtaining subject information by detecting a photoacoustic wave generated when a subject is irradiated with light.
2. Description of the Related Art
Optical imaging apparatuses which obtain information of an inside of a subject by irradiating the subject with light emitted from a light source, such as a laser, and causing the light to propagate through the subject are intensively studied mainly in the medical field. Photoacoustic imaging (PAI) is one of optical imaging technologies used in such an apparatus. Photoacoustic imaging is a technology for visualizing information regarding an optical characteristic of an inside of a subject (living body) by irradiating the subject with pulsed light emitted from a light source, detecting a photoacoustic wave generated when the light that has propagated and diffused through the subject is absorbed by the subject, and analyzing the detected photoacoustic wave. With this technology, optical characteristic distributions, in particular, an absorption coefficient distribution, an oxygen saturation distribution, etc., in the subject can be obtained.
In photoacoustic imaging, an initial sound pressure P0 of a photoacoustic wave generated from a region of interest of the subject can be expressed as follows:
P
0=Γ·μa·Φ Equation (1)
Here, Γ is a Gruneisen coefficient, which is calculated by dividing the product of a coefficient of cubical expansion β and the square of a sonic speed c by a specific heat at constant pressure CP. It is known that the value of Γ is substantially constant when the subject is determined. In addition, μa is an absorption coefficient of the region of interest, and Φ is a light intensity in the region of interest.
Japanese Patent Laid-Open No. 2010-88627 describes a technology for detecting a variation over time in sound pressure P of a photoacoustic wave that has propagated through a subject with an acoustic wave detector and calculating an initial sound pressure distribution in the subject on the basis of the result of the detection. According to Japanese Patent Laid-Open No. 2010-88627, the product of μa and Φ, that is, an optical energy absorption density, can be obtained by dividing the calculated initial sound pressure by the Gruneisen coefficient Γ. As is clear from Equation (1), it is necessary to divide the optical energy absorption density by the light intensity Φ to obtain the absorption coefficient μa from the initial sound pressure P0.
A subject information obtaining apparatus according to an embodiment of the present invention includes a plurality of acoustic wave detection elements, each of which detects a photoacoustic wave generated when a subject is irradiated with light and outputs a detection signal, an initial-sound-pressure obtaining unit that obtains an initial sound pressure in a region of interest in the subject on the basis of the detection signals, a light-intensity obtaining unit that obtains a corrected light intensity in the region of interest on the basis of weighting coefficients based on sensitivity distributions of the acoustic wave detection elements and a light intensity of the light with which the region of interest is irradiated, and an optical-characteristic-value obtaining unit that obtains an optical characteristic value in the region of interest on the basis of the initial sound pressure and the corrected light intensity.
Further features of the present invention will become apparent from the following description of exemplary embodiments with reference to the attached drawings.
A conversion efficiency with which an acoustic wave detection element converts a photoacoustic wave into a detection signal is dependent on an angle between the normal of a detection surface of the acoustic wave detection element and an incident angle of the acoustic wave. Specifically, the conversion efficiency decreases when the acoustic wave is incident on the detection surface at an angle.
This affects the value of an initial sound pressure obtained through reconstruction based on a detection signal obtained by detecting an acoustic wave with an acoustic wave detector. The thus-obtained initial sound pressure is lower than the actual initial sound pressure.
Accordingly, an optical characteristic value obtained by using the initial sound pressure that is lower than the actual initial sound pressure also differs from the actual value thereof.
Accordingly, an embodiment of the present invention provides a subject information obtaining apparatus and a subject information obtaining method with which an accurate optical characteristic value can be obtained by photoacoustic imaging.
Embodiments of the present invention based on simulations will now be described.
In the present embodiment, a subject 30 is secured by being sandwiched between two retaining members 35 and 36. In this state, pulsed light that is emitted from a light source 10 is guided through an optical system 11 and serves as irradiating light 12 with which the subject 30 is irradiated. An acoustic wave detector 20 detects a photoacoustic wave 32 that is generated by a light absorber 31 disposed in the subject 30. The acoustic wave detector 20 includes a first acoustic wave detection element e1, a second acoustic wave detection element e2, and a third acoustic wave detection element e3.
A detection signal obtained by the acoustic wave detector 20 is amplified and converted into a digital signal by a signal collector 47, and is stored in a memory included in a signal processor 40.
The signal processor 40 includes an initial-sound-pressure obtaining module 42, which serves as an initial-sound-pressure obtaining unit and obtains an initial sound pressure in a region of interest 33 of the subject 30 through image reconstruction by using the detection signal.
The signal processor 40 also includes a light-intensity obtaining module 43, which serves as a light-intensity obtaining unit and obtains a light intensity in the region of interest 33.
The signal processor 40 also includes an optical-characteristic-value obtaining module 44, which serves as an optical-characteristic-value obtaining unit and obtains an optical characteristic value in the region of interest 33 by using the initial sound pressure and total light intensity in the region of interest 33.
A display device 50, which serves as a display unit, displays the obtained optical characteristic value.
In the present embodiment, the region of interest refers to a voxel, which is a minimum unit of region that is reconstructed by the initial-sound-pressure obtaining module 42.
The initial-sound-pressure obtaining module 42 is capable of obtaining an initial sound pressure distribution over the entire region of the subject by setting regions of interest over the entire region of the subject 30. Similarly, the light-intensity obtaining module 43 and the optical-characteristic-value obtaining module 44 is capable of respectively obtaining a light intensity distribution and an absorption coefficient distribution over the entire region of the subject by setting regions of interest over the entire region of the subject.
According to the present invention, the light-intensity obtaining module 43 obtains the light intensity on the basis of sensitivity distributions of the acoustic wave detection elements. An accurate absorption coefficient can be obtained by using the light intensity obtained in consideration of the sensitivities of the acoustic wave detection elements.
To explain an aspect of the present invention, a simulation example in which the absorption coefficient is obtained without considering the sensitivities of the acoustic wave detection elements will be explained as a comparative example. The comparative example will be explained with reference to the subject information obtaining apparatus illustrated in
Here, detection signals obtained by the acoustic wave detection elements e1, e2, and e3 illustrated in
The light intensities in the region of interest 33 that correspond to the detection signals Pd1(rT), Pd2(rT), and Pd3(rT) are defined as Φ1(rT), Φ2(rT), and Φ3(rT), respectively.
The distance from each acoustic wave detection element to the region of interest 33 is defined as L, the propagation velocity of the photoacoustic wave in the subject is defined as c, and the time at which the subject 30 is irradiated with the irradiating light 12 is defined as t=0. In this case, the detection signals corresponding to the region of interest are the detection signals obtained by the respective acoustic wave detection elements at the time t=L/c. In addition, the light intensity of the light with which the region of interest 33 is irradiated is the light intensity of the irradiating light 12 in the region of interest 33 at the time t=0.
In the present embodiment, the region of interest 33 is set at a position rT where the light absorber 31 is located.
First, the initial-sound-pressure obtaining module 42 obtains an initial sound pressure P0(rT) in the region of interest 33 by using the detection signals Pd1(rT), Pd2(rT), and Pd3(rT) as expressed in the following Equation (2).
P
0(rT)=Pd1(rT)+Pd2(rT)+Pd3(rT) Equation (2)
The detection signals obtained by the acoustic wave detection elements are determined by simulation as follows:
Pd1(rT)=132 Pa
Pd2(rT)=231 Pa
Pd3(rT)=198 Pa
The initial sound pressure is calculated from Equation (2) by using the above parameters as P0(rT)=561 Pa.
Next, the light-intensity obtaining module 43 obtains the light intensity in the subject from, for example, an average optical coefficient of the subject by using a light propagation Monte Carlo method, a transport equation, a light diffusion equation, or the like.
For example, the light-intensity obtaining module 43 calculates light intensities Φ1(rT), Φ2(rT), and Φ3(rT) of the light with which the region of interest 33 is irradiated, the light intensities Φ1(rT), Φ2(rT), and Φ3(rT) corresponding to the detection signals Pd1(rT), Pd2(rT), and Pd3(rT), respectively.
Then, the light-intensity obtaining module 43 obtains an accumulated light intensity Φ(rT) in the region of interest 33 by adding up the light intensities of the light with which the region of interest 33 is irradiated, the light intensities corresponding to the respective detection signals, as expressed in the following Equation (3).
Φ(rT)=Φ1(rT)+Φ2(rT)+Φ3(rT) Equation (3)
The light intensities of the light with which the region of interest 33 is irradiated, the light intensities corresponding to the respective detection signals, are determined by simulation as follows:
Φ1(rT)=3750 mJ/m2
Φ2(rT)=3750 mJ/m2
Φ3(rT)=3750 mJ/m2
The accumulated light intensity in the region of interest is calculated from Equation (3) by using these parameters as Φ(rT)=11250 mJ/m2.
Next, the optical-characteristic-value obtaining module 44 obtains an absorption coefficient μa(rT) in the region of interest 33 represented by Equation (4) by using the initial sound pressure P0(rT) in the region of interest 33 represented by Equation (2) and the accumulated light intensity Φ(rT) in the region of interest 33 represented by Equation (3). Here, a Gruneisen coefficient Γ is Γ=1.
The absorption coefficient in the region of interest 33, which is located at the position rT of the light absorber, is calculated from Equation (4) by using the above-mentioned parameters as μa=0.050/mm. On the other hand, the absorption coefficient of the light absorber 31 set in the simulation is μa=0.088/mm.
Thus, the absorption coefficient determined from Equation (4) is smaller than the set value. This is because the absorption coefficient is calculated without considering the sensitivities of the acoustic wave detection elements.
The present inventor has found that an accurate absorption coefficient can be obtained by weighting the light intensities in consideration of the sensitivities of the acoustic wave detection elements.
Example in which Sensitivities of Acoustic Wave Detection Elements are Considered
A simulation example according to the present invention in which the absorption coefficient is obtained by using the light intensities in consideration of the sensitivities of the acoustic wave detection elements will now be described with reference to the flowchart illustrated in
S100: Step of Detecting Photoacoustic Wave Generated when Subject is Irradiated with Light
In this step, the acoustic wave detection elements e1, e2, and e3 detect the photoacoustic wave 32 generated as a result of irradiating the subject 30 with the irradiating light 12.
In this step, the initial-sound-pressure obtaining module 42 obtains the initial sound pressure in the region of interest 33 of the subject 30 by using the detection signals Pd1(rT), Pd2(rT), and Pd3(rT) obtained by the acoustic wave detection elements e1, e2, and e3, respectively, and corresponding to the region of interest 33.
In this step, similar to the method of obtaining the initial sound pressure according to the comparative example, the initial sound pressure is obtained from Equation (2). Therefore, the initial sound pressure obtained by simulation is P0(rT)=561.
In this step, a setting module 41, which is included in the signal processor 40 and serves as a setting unit, sets weighting coefficients on the basis of sensitivity distributions of the acoustic wave detection elements e1, e2, and e3.
In the present embodiment, conversion efficiencies of the acoustic wave detection elements will be explained as the sensitivities of the acoustic wave detection elements.
For example, in the present embodiment, when a photoacoustic wave is incident on an acoustic wave detection element from the front at an angle θ with respect to the normal of the detection surface of the acoustic wave detection element, a conversion efficiency with which the photoacoustic wave is converted into a detection signal is defined as A(θ). Thus, the conversion efficiency is determined by, for example, an angle between a straight line that passes through the region of interest 33 and the detection surface of the acoustic wave detection element and the normal of the detection surface of the acoustic wave detection element, that is, by an incident angle at which the photoacoustic wave generated from the region of interest is incident on the acoustic wave detection element.
When the acoustic wave detection elements e1, e2, and e3 are at angles of θ1, θ2, and θ3, respectively, with respect to the region of interest 33, the conversion efficiencies of the acoustic wave detection elements e1, e2, and e3 based on directivities thereof can be expressed as A(θ1), A(θ2), and A(θ3), respectively.
The conversion efficiencies set in the simulation are as follows:
A(θ1)=0.4
A(θ2)=0.7
A(θ3)=0.6
In an embodiment of the present invention, the sensitivity of each acoustic wave detection element is not limited as long as the sensitivity is based on information lost in a period from the generation of the photoacoustic wave to the conversion thereof into the detection signal. For example, the sensitivity of each acoustic wave detection element may be determined from an attenuation factor by which the photoacoustic wave is attenuated due to diffusion and scattering while the photoacoustic wave travels from the region of interest to the acoustic wave detection element. The attenuation factor may be determined from, for example, the distance between the region of interest and the acoustic wave detection element.
In this step, sensitivities of the acoustic wave detection elements that have been measured in advance may be used. In such a case, table data including the sensitivities of the acoustic wave detection elements in each region of interest may be stored in a memory included in the signal processor 40.
The setting module 41 sets the conversion efficiencies A(θ1), A(θ2), and A(θ3), which serve as the sensitivities of the acoustic wave detection elements e1, e2, and e3, respectively, as the weighting coefficients. In the present embodiment, the conversion efficiency A(θ1) is set as a first weighting coefficient, the conversion efficiency A(θ2) is set as a second weighting coefficient, and the conversion efficiency A(θ3) is set as a third weighting coefficient. To compensate for the information lost from the generated photoacoustic wave, the sensitivity distribution of each acoustic wave detection element or the product of the sensitivity distribution and a coefficient distribution may instead be used as the weighting coefficient of the acoustic wave detection element.
S400: Step of Obtaining Corrected Light Intensity in Region Of Interest on the Basis of Weighting Coefficients and Light Intensity of Light with which Region of Interest is Irradiated
In this step, the light-intensity obtaining module 43 obtains a corrected light intensity Φ′(rT) in the region of interest 33 on the basis of the weighting coefficients A(θ1), A(θ2), and A(θ3) corresponding to the acoustic wave detection elements e1, e2, and e3, respectively, set in S300 and the light intensities Φ1(rT), Φ2(rT), and Φ3(rT) in the region of interest 33 corresponding to the acoustic wave detection elements e1, e2, and e3, respectively.
For example, first, the light-intensity obtaining module 43 obtains a first corrected light intensity in the region of interest 33 on the basis of the weighting coefficient A(θ1) based on the sensitivity of the acoustic wave detection element e1 and the light intensity Φ1(rT) of the light with which the region of interest 33 is irradiated. Similarly, a second corrected light intensity and a third corrected light intensity are obtained for the acoustic wave detection elements e2 and e3, respectively, on the basis of the corresponding weighting coefficients and light intensities of the light with which the region of interest 33 is irradiated.
Here, the first to third corrected light intensities are obtained by multiplying the weighting coefficients by the light intensities of the light with which the region of interest is irradiated.
Then, the light-intensity obtaining module obtains the corrected light intensity Φ′(rT) in the region of interest 33 by using the first to third corrected light intensities as expressed in the following Equation (5).
Φ1(rT)=A(θ1)·Φ1(rT)+A(θ2)·Φ2(rT)+A(θ3)·Φ3(rT) Equation (5)
As described above, the parameters of Equation (5) are as follows:
Φ1(rT)=3750 mJ/m2
Φ2(rT)=3750 mJ/m2
Φ3(rT)=3750 mJ/m2
A(θ1)=0.4
A(θ2)=0.7
A(θ3)=0.6
The corrected light intensity in the region of interest 33 can be calculated from Equation (5) by using these parameters as Φ′ (rT)=6375 mJ/m2.
The light-intensity obtaining module 43 may instead obtain the corrected light intensity Φ′(rT) by multiplying the product of a light intensity of the light with which the region of interest is irradiated and the number of acoustic wave detection elements by the sum of the sensitivities of all of the acoustic wave detection elements, as expressed in the following Equation (6).
Φ′(rT)=3Φ1(rT)·{A(θ1)+A(θ2)+A(θ3)} Equation (6)
In this step, the optical-characteristic-value obtaining module 44 obtains an optical characteristic value in the region of interest 33 by using the initial sound pressure P0(rT) in the region of interest 33 obtained in S200 and the corrected light intensity Φ′(rT) in the region of interest 33 obtained in S400.
For example, the optical-characteristic-value obtaining module 44 obtains the absorption coefficient μa(rT) in the region of interest 33 represented by the following Equation (7) as an optical characteristic value.
The absorption coefficient in the region of interest 33 obtained from Equation (7) by using the above-described parameters is μa(rT)=0.088/mm. The absorption coefficient of the light absorber 31 set in the simulation is 0.088/mm. It is clear that the absorption coefficient obtained from Equation (7), which is derived in consideration of the sensitivities of the acoustic wave detection elements, is more accurate than the absorption coefficient obtained from Equation (4), which is derived without considering the sensitivities of the acoustic wave detection elements.
An accurate absorption coefficient of the inside of the subject can be obtained by the above-described steps.
A program including the above-described steps may be executed by the signal processor 40, which serves as a computer.
Although the acoustic wave detector including three acoustic wave detection elements is described in the present embodiment, the present invention may also be applied to a case in which the number of acoustic wave detection elements included in the acoustic wave detector is one, two, or four or more.
A subject information obtaining method according to a second embodiment will now be described with reference to the subject information obtaining apparatus illustrated in
The present embodiment differs from the first embodiment in that the subject is irradiated with multiple lights at different times, and an optical characteristic value is obtained by using photoacoustic waves generated by the respective lights.
First, the optical system 11 guides the pulsed light emitted from the light source 10 so as to irradiate the subject 30 with the irradiating light 12 that serves as first light. A first photoacoustic wave is generated by the light absorber 31 disposed in the subject 30 in response to the irradiation with the first light. The first acoustic wave detection element e1 detects the first photoacoustic wave, so that a first detection signal is obtained.
The subject 30 is also irradiated with the irradiating light 12 that serves as second light at a time different from the time at which the subject 30 is irradiated with the first light. A second photoacoustic wave is generated by the light absorber 31 disposed in the subject 30 in response to the irradiation with the second light. The first acoustic wave detection element e1 detects the second photoacoustic wave, so that a second detection signal is obtained.
Next, the initial-sound-pressure obtaining module 42 obtains the initial sound pressure in the region of interest 33 by using the first detection signal and the second detection signal.
Next, the light-intensity obtaining module 43 obtains the corrected light intensity in the region of interest 33 on the basis of the sensitivity distribution of the first acoustic wave detection element e1, the light intensity of the first light with which the region of interest 33 has been irradiated, and the light intensity of the second light with which the region of interest 33 has been irradiated.
For example, the light-intensity obtaining module 43 obtains a first corrected light intensity in the region of interest on the basis of the sensitivity of the first acoustic wave detection element e1 in the region of interest and the light intensity of the first light with which the region of interest 33 has been irradiated. Similarly, the light-intensity obtaining module 43 obtains a second corrected light intensity in the region of interest on the basis of the sensitivity distribution of the first acoustic wave detection element e1 and the light intensity of the second light with which the region of interest 33 has been irradiated. Then, the light-intensity obtaining module 43 obtains a corrected light intensity in the region of interest 33 by using the first corrected light intensity and the second corrected light intensity.
Next, the optical-characteristic-value obtaining module 44 obtains an optical characteristic value on the basis of the initial sound pressure in the region of interest 33 and the corrected light intensity.
Thus, the optical characteristic value is obtained by using the corrected light intensity obtained on the basis of the light intensities in the region of interest of the first light and the second light, with which the subject is irradiated at different times, and a weighting coefficient based on the sensitivity distribution of an acoustic wave detection element. Accordingly, similar to the first embodiment, an accurate optical characteristic value can be obtained.
According to an embodiment of the present invention, the irradiations with the first light and the second light may either be performed under different irradiation conditions or the same irradiation condition as long as they are performed at different times.
Although the photoacoustic waves are detected by a single acoustic wave detection element according to the present embodiment, embodiments of the present invention may also be applied to a case in which the photoacoustic waves generated by lights emitted at different times are detected by a plurality of acoustic wave detection elements.
A program including the above-described steps may be executed by the signal processor 40, which serves as a computer.
An embodiment of the present invention may also be applied to a subject information obtaining apparatus illustrated in
In the subject information obtaining apparatus illustrated in
To provide acoustic impedance matching between the subject 30 and the acoustic wave detector 20, the subject 30 is immersed in water 51 which fills a water tank 52. Since the acoustic wave detector 20 rotates around the subject 30, the water tank 52 according to the present embodiment has a columnar shape. The water tank 52 may be formed of, for example, an acrylic that is transparent to irradiating light 12.
The water tank 52 may have, for example, a hemispherical shape instead of a columnar shape as long as the photoacoustic wave can be detected by the acoustic wave detector while the acoustic wave detector is oriented in various directions. Alternatively, the photoacoustic wave can be detected by a plurality of acoustic wave detectors that are oriented in various directions.
With the above-described structure, portions whose shapes cannot be retained by retaining members or the like can also be measured. In addition, since the detection elements may be arranged in many directions with respect to the subject, data having a large amount of information can be obtained.
In the subject information obtaining apparatus illustrated in
Unlike the other embodiment, in the present embodiment, the operator holds the gripper 71 and manually moves housing 70 instead of mechanically moving the acoustic wave detector 20. Therefore, the positional relationship between the acoustic wave detector 20 and the region of interest 33 at the time when a photoacoustic wave 32 is detected cannot be determined. However, the positional relationship between the acoustic wave detector 20 and the region of interest 33 needs to be determined to obtain a detection signal corresponding to the region of interest from the detection signal obtained by the acoustic wave detector 20. Therefore, in the present embodiment, the housing 70 may include a position detector 72 that detects the position of the housing 70, that is, the positions of the acoustic wave detector 20 and the optical system 11 contained in the housing 70.
Also in the subject information obtaining apparatuses illustrated in
Embodiments of the present invention can also be realized by a computer of a system or apparatus that reads out and executes computer executable instructions recorded on a storage medium (e.g., non-transitory computer-readable storage medium) to perform the functions of one or more of the above-described embodiment(s) of the present invention, and by a method performed by the computer of the system or apparatus by, for example, reading out and executing the computer executable instructions from the storage medium to perform the functions of one or more of the above-described embodiment(s). The computer may comprise one or more of a central processing unit (CPU), micro processing unit (MPU), or other circuitry, and may include a network of separate computers or separate computer processors. The computer executable instructions may be provided to the computer, for example, from a network or the storage medium. The storage medium may include, for example, one or more of a hard disk, a random-access memory (RAM), a read only memory (ROM), a storage of distributed computing systems, an optical disk (such as a compact disc (CD), digital versatile disc (DVD), or Blu-ray Disc (BD)™), a flash memory device, a memory card, and the like.
Structures of Main Components Will Now be Described. Light Source 10
The light source 10 is capable of emitting pulsed light of 5 to 50 nanoseconds. Although a high power laser may be used as the light source, a light emitting diode may be used instead of the laser. Various lasers, such as a solid-state laser, a gas laser, a dye laser, and a semiconductor laser, may be used as the laser. Ideally, a Ti:Sa laser pumped by a Nd:YAG laser or an alexandrite laser, which are a high power laser having a continuously variable wavelength, is used. A plurality of single-wavelength lasers having different wavelengths may also be used.
The pulsed light emitted from the light source 10 is typically guided to the subject while being shaped into a desired optical distribution by optical components, such as a lens and a mirror. However, the pulsed light may instead be propagated through an optical waveguide such as an optical fiber or the like.
The optical system 11 includes, for example, a mirror that reflects light, a lens that collects, magnifies, or changes the shape of light, and a diffusing plate that diffuses light. These optical components are not limited as long as the pulsed light emitted from the light source can be formed into a desired shape before the subject is irradiated therewith. The light can be spread over a certain area instead of being collected by a lens. In such a case, the safety of the subject and the diagnostic region can be increased.
An optical-system moving mechanism for moving the optical system 11 may be provided so that the subject can be scanned with the irradiating light. The optical system may include a plurality of light emitting units so that the irradiating light can be emitted from a plurality of positions.
The acoustic wave detector 20 is a detector for detecting a photoacoustic wave generated at a surface and an inside of a subject when the subject is irradiated with light. The acoustic wave detector 20 detects the acoustic wave and converts the acoustic wave into an analog electric signal. The acoustic wave detector 20 may hereinafter be referred to simply as a probe or a transducer. Any type of acoustic wave detector, such as a transducer using a piezoelectric phenomenon, a transducer using optical resonance, or a transducer using a change in capacitance, may be used as long as acoustic wave signals can be detected.
The acoustic wave detector 20 may include a plurality of acoustic wave detection elements that are one-dimensionally or two-dimensionally arranged in an array. When the acoustic wave detection elements that are multi-dimensionally arranged are used, the acoustic wave can be detected simultaneously at a plurality of positions. Therefore, the detection time and the influence of, for example, vibration of the subject can be reduced.
The acoustic wave detector 20 may be configured to be mechanically movable by a detector moving mechanism.
The acoustic wave detector 20 may include a gripper so that an operator can hold the gripper and manually move the acoustic wave detector 20.
The signal collector 47 may be provided which amplifies the electric signal obtained by the acoustic wave detector 20 and converts the electric signal, which is an analog signal, into a digital signal. The signal collector 47 typically includes an amplifier, an A/D converter, and a field programmable gate array (FPGA) chip. In the case where a plurality of detection signals are obtained by the acoustic wave detector, the signal collector 47 may be configured to simultaneously process the plurality of detection signals. In such a case, the time required to form an image can be reduced. In this specification, the concept of “detection signal” includes both the analog signal output from the acoustic wave detector 20 and the digital signal into which the analog signal is converted by the signal collector 47.
The signal processor 40 obtains the optical characteristic value of the inside of the subject by performing, for example, image reconstruction. The signal processor 40 typically includes a workstation, and an image reconstruction process, for example, is performed by software that is programmed in advance. The software used in the workstation includes, for example, the setting module 41, the initial-sound-pressure obtaining module 42, the light-intensity obtaining module 43, and the optical-characteristic-value obtaining module 44.
The modules included in the signal processor 40 may instead be provided as individual devices.
In the case where the modules are formed as hardware, each module may be, for example, an FPGA or an ASIC. Alternatively, each module may be formed as a program for causing the computer to execute the corresponding process.
The signal collector 47 and the signal processor 40 may be integrated with each other. In this case, an optical characteristic value of the subject may be generated by a hardware process instead of a software process performed by a workstation.
While the present invention has been described with reference to exemplary embodiments, it is to be understood that the invention is not limited to the disclosed exemplary embodiments. The scope of the following claims is to be accorded the broadest interpretation so as to encompass all such modifications and equivalent structures and functions.
This application claims the benefit of Japanese Patent Application No. 2012-085728 filed Apr. 4, 2012, which is hereby incorporated by reference herein in its entirety.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2012-085728 | Apr 2012 | JP | national |
