Abstract
Photoacoustic tomography (PAT) refers to imaging that is based on the photoacoustic effect. Although the photoacoustic effect as a physical phenomenon was first reported on by Alexander Graham Bell in 1880 [1], PAT as an imaging technology was developed only after the advent of ultrasonic transducers, computers, and lasers [2–31]. A review on biomedical photoacoustics is available [32]. The motivation for PAT is to combine optical-absorption contrast with ultrasonic spatial resolution for deep imaging in the optical quasi-diffusive or diffusive regime. In PAT, the tissue is irradiated by usually a short-pulsed laser beam to achieve a thermal and acoustic impulse response (Fig. 19.1). Locally absorbed light is converted into heat, which is further converted to a pressure rise via thermo-elastic expansion. The initial pressure rise – determined by the local optical absorption coefficient (μ â ), fluence (ψ) and other thermal and mechanical properties – propagates as an ultrasonic wave, which is referred to as a photoacoustic wave.
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Acknowledgment
The author thanks H. Zhang and K. Maslov for providing unpublished Fig. 19.4. This work was sponsored by National Institutes of Health grants R01 EB000712 and R01 NS46214.
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Wang, L.V. (2010). Photoacoustic Tomography. In: Welch, A., van Gemert, M. (eds) Optical-Thermal Response of Laser-Irradiated Tissue. Springer, Dordrecht. https://doi.org/10.1007/978-90-481-8831-4_19
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