# DNA melting structures in the generalized Poland-Scheraga model

**Authors:** Quentin Berger, Giambattista Giacomin, Maha Khatib

arXiv: 1703.10343 · 2017-03-31

## TL;DR

This paper analyzes the generalized Poland-Scheraga model for DNA melting, revealing how excess bases lead to distinct structural transitions, including macroscopic loops or unbound single strands, using a bivariate renewal process framework.

## Contribution

It fully characterizes the geometric and configurational transitions in the generalized model, extending previous work with a detailed path property analysis.

## Key findings

- Excess bases cause either macroscopic loop formation or unbound single strand ends.
- The model's phase transitions are explicitly characterized through renewal process analysis.
- The work advances understanding of DNA denaturation structures in complex models.

## Abstract

The Poland-Scheraga model for DNA denaturation, besides playing a central role in applications, has been widely studied in the physical and mathematical literature over the past decades. More recently a natural generalization has been introduced in the biophysics literature to overcome the limits of the original model, namely to allow an excess of bases -- i.e. a different length of the two single stranded DNA chains -- and to allow slippages in the chain pairing. The increased complexity of the model is reflected in the appearance of configurational transitions when the DNA is in double stranded form. In a previous work of two of the authors the generalized Poland-Scheraga model has been analyzed thanks to a representation in terms of a bivariate renewal process. In this work we exploit this representation farther and fully characterize the path properties of the system, making therefore explicit the geometric structures -- and the configurational transitions -- that are observed when the polymer is in the double stranded form. What we prove is that, when the excess of bases is not absorbed in a homogeneous fashion along the double stranded chain, then it either condensates in a single macroscopic loop or it accumulates into an unbound single strand free end.

## Full text

_Full body text omitted from this summary view._ Fetch the complete paper as Markdown: https://tomesphere.com/paper/1703.10343/full.md

## Figures

9 figures with captions in the complete paper: https://tomesphere.com/paper/1703.10343/full.md

## References

19 references — full list in the complete paper: https://tomesphere.com/paper/1703.10343/full.md

---
Source: https://tomesphere.com/paper/1703.10343