Abstract

Optical-resolution photoacoustic microscopy (OR-PAM) combines high spatial resolution and strong absorption-based contrast in tissue, which has enabled structural and spectroscopic imaging of endogenous chromophores, primarily hemoglobin. Conventional piezoelectric ultrasound transducers are typically placed far away from the photoacoustic source due to their opacity, which reduces acoustic sensitivity. Optical ultrasound sensors are an alternative as their transparency allows them to be positioned close to the sample with minimal source-detector distances. In this work, a backward-mode OR-PAM system based on a planar Fabry-Pérot ultrasound sensor and coaxially aligned excitation and interrogation beams was developed. Two 3D imaging modes, using raster-scanning for enhanced image quality and continuous-scanning for fast imaging, were implemented and tested on a leaf skeleton phantom. In fast imaging mode, a scan-rate of 100,000 A-lines/s was achieved. 3D images of a zebrafish embryo were acquired in vivo in raster-scanning mode. The transparency of the FP sensor in the visible and near-infrared wavelength region makes it suitable for combined functional and molecular imaging applications using OR-PAM and multi-photon fluorescence microscopy.

Highlights

  • Optical-resolution photoacoustic microscopy (OR-PAM) provides high-resolution images of biological tissue in vivo from which structural and functional information can be obtained

  • For settings suitable for imaging of functional hemodynamic parameters in the zebrafish embryo, e.g. a field of view (FOV) of (300 × 200) μm2 and a step size of 4 μm, raster-scanning would result in a frame rate of 0.4 Hz, which is below frame rates of >20 Hz required for im­ aging hemodynamic processes

  • A backward-mode OR-PAM system based on a planar FP ultrasound sensor is described

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Summary

Introduction

Optical-resolution photoacoustic microscopy (OR-PAM) provides high-resolution images of biological tissue in vivo from which structural and functional information can be obtained. To generate photoacoustic (PA) waves, the output of a pulsed laser is focussed into superficial re­ gions of the tissue (

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