The disclosed technology relates to photoacoustic imaging systems and to photoacoustic transducers in particular.
Photoacoustic sensing and imaging is a mechanism where properties of tissue can be examined based on the response of the tissue to excitation light pulses. As will be understood by those skilled in the art, short pulses of laser excitation light that are directed onto tissue cause the tissue to rapidly heat and expand. This rapid expansion creates an ultrasonic signal that can be detected, analyzed and converted into an image. Because different types of tissue will heat and expand differently when exposed to the excitation light pulses, the ultrasound signals produced have different signal characteristic and images can be produced where the different types of tissue can be seen.
While the theory of photoacoustic imaging system is well understood, there are significant hurdles associated with being able to produce good images with the technology. One factor that can produce variations in the ultrasound signals received is the variations in the power of the excitation light pulses produced the light source. It is not uncommon for variations in the pulses to vary by more than +/−5% for a well tuned laser system and by +/−10% for less regulated excitation light systems. The variations in laser light power are directly proportional to the strength of the ultrasound signals created. Therefore, in order to compensate the images produced for the variations in the laser light power used to produce the ultrasound signals, it is desirable to know how much light was applied to the tissue.
Prior solutions such as those described in PCT/US2011/034640 measure the power of light reflected from the tissue in order to gauge how much light power was applied to the tissue. While this approach can work, improvements can be made. Given this problem, there is a need for an improved system that can measure the light energy that is applied to tissue in a photoacoustic imaging system.
As will be discussed in further detail below, the disclosed technology relates to photoacoustic imaging systems and in particular to photoacoustic imaging transducers that can measure the power of laser light that is delivered to a region of interest. In one embodiment, a transducer receives laser excitation light on a bundle of optical fibers. The fibers are randomized to produce a uniform light distribution. One portion of the fibers is coupled to a light bar that runs along one side of an acoustic stack that includes an ultrasound transducer. Another portion of the fibers is coupled to a second light bar that runs along the other side of the acoustic stack. A small percentage of the fibers in the bundle are coupled to an optical sensor that is located in a transducer handle.
In one embodiment, the optical sensor is a Pyro-Electric crystal based sensor that is positioned proximal to the acoustic stack in the transducer handle. The optical fibers are coupled to the sensor with an SMA optical coupler. Signals from the optical sensor are digitized and analyzed by a programmed processor to adjust the gain of images produced in response to ultrasound signals detected by the transducer. In one embodiment, the optical fibers coupled to the optical sensor are arranged in the transducer handle such that they have the same length as the optical fibers that are coupled to the light bars.
One embodiment of the disclosed technology is illustrated in
A bundle of optical fibers 18 delivers optical excitation light to the transducer 10. The optical fibers in the bundle are preferably randomized so that the supplied optical energy at one end bundle will be uniformly distributed without any hot spots at the other end of the bundle. Within the transducer 10, the bundle of fibers 18 is split into three or more groups. A first group of fibers 22 is optically coupled at a distal end to a laser light bar 24 or other lens system that is located along one edge of the front face of the acoustic stack 14. A second group of fibers 26 is optically coupled at a distal end to a laser light bar (not shown) or other lens system that is located along a second edge of the front face of the acoustic stack 14. In one embodiment, the light bars on either side of the acoustic stack 14 focus the light in the fibers within a region of interest from which the ultrasound transducer elements in the acoustic stack 14 receive ultrasound signals.
In accordance with one embodiment of the disclosed technology, a small percentage (e.g. 3-5%) of the optical fibers in the bundle 18 is split into a third bundle 30 that is coupled at a distal end to a light sensor 34. The optical fibers in the bundle 30 preferably have the same length as those optical fibers that are coupled to the light bars on either side of the acoustic stack. To keep the length of the fibers in the bundle 30 the same as those fibers that are coupled to the light bars, there may need to be some bending or routing of the bundle optical fibers in the transducer housing. In one embodiment, the optical fibers in the bundle 30 are coupled to the light sensor 34 with an SMA optical connector. The optical sensor 34 produces signals that are reflective of the power of the optical signals that are delivered to the tissue (or other object to which the transducer is engaged). As discussed above, the power of the light pulses may vary due to variations in the laser power. In addition, the power may vary due to the effect of filters such as an optical parameter oscillator that are place in the light path.
As can be seen in
Light from the laser 64 is delivered to the transducer 10 through the bundle of optical fibers 18. Signals from the ultrasound transducer are carried from the transducer 10 to an ultrasound imaging system 70 on a number of wires or other signal carriers 72.
As discussed above, the ultrasound system preferably includes a programmed processor that operates to receive the ultrasound signals produced by the transducer as well as the signals produced by the optical sensor 34. The optical sensor 34 produces signals that are proportional to the strength or power of the light pulses that exit the optical fibers within the transducer. Depending on the strength of the light pulses, the gain of the ultrasound signals may be increased or decreased during the creation of images from the ultrasound signals.
From the foregoing, it will be appreciated that specific embodiments of the invention have been described herein for purposes of illustration, but that various modifications may be made without deviating from the scope of the invention. In another embodiment, the optical sensor 34 need not be completely contained within the transducer housing but may be only partially contained within the transducer housing.
Accordingly, the invention is not limited except as by the appended claims.
This application claims benefit of and priority to U.S. Provisional Patent Application Ser. No. 61/827,520, filed on May 24, 2013, and entitled “PHOTOACOUSTIC TRANSDUCER WITH OPTICAL FEEDBACK,” which is hereby incorporated herein in its entirety by reference.
Number | Date | Country | |
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61827520 | May 2013 | US |