2018 52nd Annual Conference on Information Sciences and Systems (CISS) 2018
DOI: 10.1109/ciss.2018.8362313
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Heterogeneous multireference alignment: A single pass approach

Abstract: Multireference alignment (MRA) is the problem of estimating a signal from many noisy and cyclically shifted copies of itself. In this paper, we consider an extension called heterogeneous MRA, where K signals must be estimated, and each observation comes from one of those signals, unknown to us. This is a simplified model for the heterogeneity problem notably arising in cryo-electron microscopy. We propose an algorithm which estimates the K signals without estimating either the shifts or the classes of the obse… Show more

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Cited by 47 publications
(59 citation statements)
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References 37 publications
(49 reference statements)
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“…On the other hand, autocorrelation analysis requires shorter computation time by summarizing the data as autocorrelation statistics with one pass over the data. We note that the distinct computational speeds for autocorrelation analysis and the EM algorithm is also observed in the related problem of multi-reference alignment [8], [14]. The difference in run time and the similar reconstruction quality of the two methods at low SNR make autocorrelation analysis the preferred approach for large datasets.…”
Section: Numerical Experimentsmentioning
confidence: 76%
“…On the other hand, autocorrelation analysis requires shorter computation time by summarizing the data as autocorrelation statistics with one pass over the data. We note that the distinct computational speeds for autocorrelation analysis and the EM algorithm is also observed in the related problem of multi-reference alignment [8], [14]. The difference in run time and the similar reconstruction quality of the two methods at low SNR make autocorrelation analysis the preferred approach for large datasets.…”
Section: Numerical Experimentsmentioning
confidence: 76%
“…where W ≥ L is the length of the sought signal and the weights are set to w 1 = 1/2, w 2 = 1/2n 2 , w 3 = 1/2n 3 , where n 2 , n 3 are the number of moments used: n 2 = L − 1, n 3 = (L−1)(L−2) 2 (weights could also be set in accordance with variance estimates as in [9]).…”
Section: Discussionmentioning
confidence: 99%
“…Recall that S 3 ( x 1 , x 2 ) is a discrete version of s 3 ( x 1 , x 2 ), which only depends on the three parameters: | x 1 |, | x 2 | and θ( x 1 , x 2 ). Let S * 3 be the estimate of S 3 from the noisy measurement M via (6), that is, the de-biased and normalized autocorrelation of the measurement A 3 (4), andŜ * 3 denote the DFT of S * 3 . Since the noise is assumed to be i.i.d.…”
Section: Leveraging Symmetriesmentioning
confidence: 99%