Figure 5
Comparison of 3D structure reconstruction in cryo-ET subtomogram averaging using the MMSE and MLE rotation estimators. Iterative structure-reconstruction procedures with the MMSE estimator ( ) and MLE estimator ( ) are defined in equations (31) and (32) , respectively. At high SNR levels, a low-resolution structure emerges due to finite grid sampling of the rotation group , effectively acting as a low-pass filter. The 3D reconstruction using the MMSE estimator consistently outperforms the reconstruction using the MLE estimator. For high-SNR conditions (i.e. σ → 0), both estimators yield similar 3D structures, as expected from Proposition 2 . The SNR values used for the panels (from right to left) are 10−2, 2 × 10−3, 7 × 10−4 and 2 × 10−4, with a volume size of 32 × 32 × 32. The boxes highlighted in purple resemble the true input structure (80S ribosome; Wong et al., 2014 ), while the orange-highlighted boxes are more similar to the initial template (β-galactosidase; Bartesaghi et al., 2014 ), illustrating the `Einstein from Noise' phenomenon. Notably, at very low SNRs, the `Einstein from Noise' effect is evident with the MLE estimator but not with the MMSE estimator. |