Talk:Photoacoustic imaging in biomedicine

From Wikipedia, the free encyclopedia

WikiProject Medicine This article is within the scope of WikiProject Medicine. Please visit the project page for details or ask questions at the doctor's mess.
B This page has been rated as B-Class on the quality assessment scale
Low This article has been rated as Low-importance on the importance assessment scale

[edit] PI

Photoacoustic Imaging (originally called Optoacoustic Imaging) is a method of image acquisition and reconstruction based on time-resolved detection of acoustic pressure profiles induced in tissue through absorption of optical pulses under irradiation conditions of temporal pressure confinement during optical energy deposition [A.A. Oraevsky, A.A. Karabutov: “Optoacoustic Tomography ”, in Biomedical Photonics Handbook, ed. By T. Vo-Dinh, CRC Press, 2003, Vol. PM125, Chapter 34, pp. 34/1-34/34]. The term “irradiation conditions of temporal pressure confinement” means that optical energy (or other heat-generating energy) must be delivered to tissue faster than resulting acoustic wave can propagate the distance in tissue equal to the desirable spatial resolution. For example, having desirable resolution of optoacoustic images of 15 µm, and the speed of sound propagation in tissue of 1.5 mm per µs, one needs optical pulses shorter than 0.01 µs. Thus, utilization of short (nanosecond) optical pulses represents necessary (but not sufficient) condition to achieve desirable spatial (axial) resolution of OAT. The sufficient condition to obtain desirable spatial resolution is to employ detectors of acoustic waves with temporal response-function of not worse than the optical pulse duration. Satisfaction of irradiation conditions of temporal pressure confinement is also required for the optoacoustic signals to accurately resemble profiles of absorbed optical energy in tissue. Distribution of absorbed optical energy can be used to visualize and characterize quantitatively various tissue structures and their physiological functions based on variations in tissue optical properties. In order to relate tissue structure to optoacoustic images, the acoustic detectors must be capable of resolving not only rapid changes in optoacoustic signals associated with sharp edges and boundaries in tissues, but also reproduce slow changes associated with smooth variation in optical properties within one type of tissue. In other words, acoustic detectors have to detect both high and low ultrasonic frequencies of acoustic pressure at once. These types of acoustic detectors are called ultrawide-band acoustic transducers. These transducers have relatively equal detection sensitivity over the entire ultrasonic range from 20 kHz to 20 MHz (and in some cases even higher up to 100 MHz). The ultrasonic detection bandwidth of acoustic transducers defines the limits of axial (radial) resolution. The lateral resolution of an optoacoustic image, on the other hand, is defined by dimensions of each acoustic transducer, dimensions and geometry of the acoustic transducers in array. The array of transducers can be simulated by scanning a single transducer along tissue surface. Thermoacoustic tomography is a modification of the optoacoustic tomography in which pulses of electromagnetic radiation other than light (such as microwaves or radiowaves) induce thermoelastic expansion of tissue and generation of ultrasound signals.