Abstract

Algorithms for prediction of RNA secondary structure— the set of base pairs that form when an RNA molecule folds— are valuable to biologists who aim to understand RNA structure and function. Improving the accuracy and efficiency of prediction methods is an ongoing challenge, particularly for pseudoknotted secondary structures, in which base pairs overlap. This challenge is biologically important, since pseudoknotted structures play essential roles in functions of many RNA molecules, such as splicing and ribosomal frameshifting. State-ofthe-art methods, which are based on free energy minimization, have high runtime complexity (typically Θ(n) or worse), and can handle (minimize over) only limited types of pseudoknotted structures. We analyze a new approach for prediction of pseudoknotted structures, motivated by the hypothesis that RNA structures fold hierarchically, with pseudoknot free (non-overlapping) base pairs forming first, and pseudoknots forming later so as to minimize energy relative to the folded pseudoknot free structure. Our HFold algorithm, based on work of S. Zhao, uses two-phase energy minimization to predict hierarchically-formed secondary structures in O(n) time, matching the complexity of the best algorithms for pseudoknot free secondary structure prediction via energy minimization. Our algorithm can handle a wide range of biological structures, including kissing hairpins and nested kissing hairpins, which have previously required Θ(n) time. We also report on the experimental evaluations of HFold and present thorough analyses of the results. We show that if the input structure to the algorithm is correct, running the algorithm results in 16% accuracy improvement on average over the accuracy of the true pseudoknot free structures. However if the input structure is not correct, the accuracy improvement is not significant. If the first 10 suboptimal foldings are given as input to our algorithm instead of just the minimum free energy structure (MFE), the prediction accuracy improves significantly over the accuracy of the MFE structures. This improvement is even more when the number of suboptimal foldings as input to our algorithm increases. The comparison of the energy of the structures predicted by HFold on the true pseudoknot free structures with the energy of the true structures calculated using a different method with the same energy model shows that the energy model may be the cause for the cases for which HFold predicts structures far from the true structures. Our experimental result provides some ways in which the hierarchical folding hypothesis might need to be refined.

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