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The dose-fractionation theorem for tomographic imaging is a statement that says the total dose required to achieve statistical significance for each voxel of a computed 3D reconstruction is the same as that required to obtain a single 2D image of that isolated voxel at the same level of statistical significance. Hegerl and Hoppe[1] have pointed out that a statistically significant 3D image can be computed from statistically insignificant projections, as long as the total dose that is distributed among these projections is high enough that it would have resulted in a statistically significant projection, if applied to only one image.[2] The original derivations assumed weak-contrast imaging with additive noise, however, the dose-fractionation theorem was demonstrated using a more complete noise model by Yalisove, Sung, et al.[3]
References
edit- ^ R. Hegerl; W. Hoppe (1976). "Influence of Electron Noise on Three-dimensional Image Reconstruction". Zeitschrift für Naturforschung A. 31 (12): 1717–1721. Bibcode:1976ZNatA..31.1717H. doi:10.1515/zna-1976-1241. S2CID 3539651.
- ^ McEwen BF, Downing KH, Glaeser RM (1995). "The relevance of dose-fractionation in tomography of radiation-sensitive specimens". Ultramicroscopy. 60 (3): 357–373. doi:10.1016/0304-3991(95)00082-8. PMID 8525549.
- ^ R. Yalisove; S.H. Sung; P. Ercius; R. Hovden (2021). "Limits of Three-Dimensional Resolution and Dose for Aberration-Corrected Electron Tomography". Physical Review Applied. 15 (1): 014003. arXiv:2006.06585. Bibcode:2021PhRvP..15a4003Y. doi:10.1103/PhysRevApplied.15.014003.
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