Circuit topology

This article is about the topology of polymers. For the topology of electrical circuits, see Circuit topology (electrical).
Circuit topology relations in a chain with two binary contacts.
Circuit topology relations in a chain with two binary contacts.

The circuit topology of a folded linear polymer refers to the arrangement of its intra-molecular contacts. Examples of linear polymers with intra-molecular contacts are nucleic acids and proteins. Proteins fold via the formation of contacts of various natures, including hydrogen bonds, disulfide bonds, and beta-beta interactions.[1] RNA molecules fold by forming hydrogen bonds between nucleotides, forming nested or non-nested structures. Contacts in the genome are established via protein bridges including CTCF and cohesins and are measured by technologies including Hi-C.[2] Circuit topology categorises the topological arrangement of these physical contacts, that are referred to as hard contacts (or h-contacts). Furthermore, chains can fold via knotting (or the formation of "soft" contacts (s-contacts)). Circuit topology uses a similar language to categorise both "soft" and "hard" contacts, and provides a full description of a folded linear chain. In this framework, a "circuit" refers to a segment of the chain where each contact site within the segment forms connections with other contact sites within the same segment, and thus is not left unpaired. A folded chain can thus be studied based on its constituting circuits.

A simple example of a folded chain is a chain with two hard contacts. For a chain with two binary contacts, three arrangements are available: parallel (P), series (S), and crossed (X). For a chain with n contacts, the topology can be described by an n by n matrix in which each element illustrates the relation between a pair of contacts and may take one of the three states, P, S and X. Multivalent contacts can also be categorised in full or via decomposition into several binary contacts. Similarly, circuit topology allows for the classification of the pairwise arrangements of chain crossings and tangles, thus providing a complete 3D description of folded chains. Furthermore, one can apply circuit topology operations to soft and hard contacts to generate complex folds, using a bottom-up engineering approach.

Both knot theory and circuit topology aim to describe chain entanglement, making it important to understand their relationship. Knot theory considers any entangled chain as a connected sum of prime knots, which are themselves undecomposable. Circuit topology splits any entangled chains (including prime knots) into basic structural units called soft contacts, and lists simple rules on how soft contacts can be put together.[3][4] An advantage of circuit topology is that it can be applied to open linear chains with intra-chain interactions, so-called hard contacts.[5] This enabled topological analysis of proteins and genomes, which are often described as "unknot" in knot theory. [6][7] Finally, circuit topology enables studying interactions between hard contacts and entanglements and can identify slip knots, while knot theory typically overlooks hard contacts and split knots. Thus, circuit topology serves as a complementary approach to knot theory.

Circuit topology has implications for folding kinetics and molecular evolution and has been applied to engineer polymers including molecular origami.[8] Circuit topology along with contact order and size are determinants of the folding rate of linear polymers.[9] The approach can also be used for medical applications including the prediction of pathogenicity of mutations.

  1. ^ Mashaghi, Alireza; van Wijk, Roeland J.; Tans, Sander J. (2014). "Circuit Topology of Proteins and Nucleic Acids". Structure. 22 (9): 1227–1237. doi:10.1016/j.str.2014.06.015. PMID 25126961.
  2. ^ Scalvini, Barbara; Schiessel, Helmut; Golovnev, Anatoly; Mashaghi, Alireza (March 2022). "Circuit topology analysis of cellular genome reveals signature motifs, conformational heterogeneity, and scaling". iScience. 25 (3): 103866. Bibcode:2022iSci...25j3866S. doi:10.1016/j.isci.2022.103866. PMC 8861635. PMID 35243229.
  3. ^ Golovnev, Anatoly; Mashaghi, Alireza (7 December 2021). "Circuit Topology for Bottom-Up Engineering of Molecular Knots". Symmetry. 13 (12): 2353. arXiv:2106.03925. Bibcode:2021Symm...13.2353G. doi:10.3390/sym13122353.
  4. ^ Flapan, Erica; Mashaghi, Alireza; Wong, Helen (1 June 2023). "A tile model of circuit topology for self-entangled biopolymers". Scientific Reports. 13 (1): 8889. Bibcode:2023NatSR..13.8889F. doi:10.1038/s41598-023-35771-8. PMC 10235088. PMID 37264056. S2CID 259022790.
  5. ^ Golovnev, Anatoly; Mashaghi, Alireza (September 2020). "Generalized Circuit Topology of Folded Linear Chains". iScience. 23 (9): 101492. Bibcode:2020iSci...23j1492G. doi:10.1016/j.isci.2020.101492. PMC 7481252. PMID 32896769.
  6. ^ Yasuyuki Tezuka, Tetsuo Deguchi, Topological Polymer Chemistry: Concepts and Practices (2022) ISBN 978-981-16-6807-4
  7. ^ "Leiden scientists develop topological barcodes for folded molecules" (Press release). Leiden University. 25 August 2020.
  8. ^ Yasuyuki Tezuka and Tetsuo Deguchi, Topological Polymer Chemistry: Concepts and Practices (2022) ISBN 978-981-16-6806-7
  9. ^ Mugler, Andrew; Tans, Sander J.; Mashaghi, Alireza (2014). "Circuit topology of self-interacting chains: implications for folding and unfolding dynamics". Phys. Chem. Chem. Phys. 16 (41): 22537–22544. Bibcode:2014PCCP...1622537M. doi:10.1039/C4CP03402C. PMID 25228051.