Abstract

Solving the fluorophore distribution in a tomographic setting has been difficult because of the lack of physically meaningful and computationally applicable propagation models. This study concentrates on the direct modelling of fluorescence signals in optical projection tomography (OPT), and on the corresponding inverse problem. The reconstruction problem is solved using emission projections corresponding to a series of rotational imaging positions of the sample. Similarly to the bright field OPT bearing resemblance with the transmission x-ray computed tomography, the fluorescent mode OPT is analogous to x-ray fluorescence tomography (XFCT). As an improved direct model for the fluorescent OPT, we derive a weighted Radon transform based on the XFCT literature. Moreover, we propose a simple and fast iteration scheme for the slice-wise reconstruction of the sample. The developed methods are applied in both numerical experiments and inversion of fluorescent OPT data from a zebrafish embryo. The results demonstrate the importance of propagation modelling and our analysis provides a flexible modelling framework for fluorescent OPT that can easily be modified to adapt to different imaging setups.

Highlights

  • The classical x-ray computed tomography (CT) has become a standard of tomographic imaging

  • This study focused on direct modelling and iterative inversion in fluorescent optical projection tomography (OPT)

  • As an improved direct model for the fluorescent OPT, we presented a weighted Radon transform

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Summary

Introduction

The classical x-ray computed tomography (CT) has become a standard of tomographic imaging. The high energy x-rays are harmful to biological targets In this and other regards, optical projection tomography (OPT) (Sharpe et al 2002) provides a suitable alternative in the mesoscopic scale with samples of 1–10 mm in diameter (Figueiras et al 2014, Soto et al 2016, Belay et al 2017). Optical imaging provides naturally better contrast with soft tissues and, at lower intensities, light as non-ionizing radiation should have a low, even negligible, impact on living organisms in imaging phase. This allows for long-term monitoring of the samples with OPT if the sample preparation and handling is properly designed

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