A kissing loop is intramolecular loop that makes interaction with the other strand.
- Roland Krause
Give the energy functions for the new structures for the interaction partition function.
- Roland Krause
Second part given now by Hamid Chitsaz
- Roland Krause
Main interest in the strength and stability of the RNA interaction, which is challenging because all structures must be accounted for exactly once.
- Roland Krause
Make use of a dynamic programming approach using divide and conquer. Compute the partition function for bits of the structure.
- Roland Krause
McCaskill's algorithm (1990) is introduced, describing a participation function for single strands.
- Roland Krause
For two unpaired strands, McCaskill's algorithm can be used directly,
- Roland Krause
98 cases need to be considered, not even in the paper but in the suppl. mat.
- Roland Krause
# sounds like a complicated model, it's not completely presented
- Roland Krause
Explanation for the no-zig zag assumption motivated by less running time, one arch describes them all.
- Roland Krause
Can predict the equilibrium concentaion, the melting temperature and the UV absorption.
- Roland Krause
Presented algorithm (piRNA) outperforms existing ones by an order of magnitude, experimental validation with Tm shows little deviation.
- Roland Krause