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. Author manuscript; available in PMC: 2021 Jul 19.
Published in final edited form as: Clin Cancer Res. 2019 Sep 24;25(24):7436–7447. doi: 10.1158/1078-0432.CCR-19-0360

Figure 1. Fabry-Perot-based photoacoustic scanner and example image of a subcutaneous tumor xenograft.

Figure 1

(a) scanner architecture. Excitation laser pulses are transmitted through the FP sensor head and absorbed in the tissue generating photoacoustic signals which are then detected by the Fabry-Perot polymer film ultrasound sensor. Inset: an expanded view of the sensor which comprises a polymer spacer sandwiched between a pair of dichroic mirrors that are transparent to the excitation laser wavelength but highly reflective to the sensor interrogation beam wavelength. The sensor operates by raster scanning a focused continuous wave interrogation laser beam across it and measuring the change in the power of the reflected beam produced by acoustically-induced changes in the polymer spacer thickness. (b) Photoacoustic image of SW1222 tumor xenograft acquired using the scanner and displayed (clockwise) as x-y, x-z and y-z maximum intensity projections (MIPs). An animated volume rendered representation of this data can be viewed online (Video 1. The yellow arrows on the x-y MIP indicate the tumor. The x-z and y-z MIPs show that the entire tumor can be visualised with high resolution to a depth of approximately 8mm.