A simple model of a sequence-reading diffusion: non-self-averaging and self-averaging properties

Motivated by a question about the sensitivity of knots’ diffusive motion to the actual sequence of nucleotides placed on a given DNA, here we study a simple model of a sequence-reading diffusion on a stretched chain with a frozen sequence of ‘letters’ A and B , having different interaction energies....

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Published in:New Journal of Physics
Main Authors: Silvio Kalaj, Enzo Marinari, Gleb Oshanin, Luca Peliti
Format: Article
Language:English
Published: IOP Publishing 2025-01-01
Subjects:
Online Access:https://doi.org/10.1088/1367-2630/adcd94
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author Silvio Kalaj
Enzo Marinari
Gleb Oshanin
Luca Peliti
author_facet Silvio Kalaj
Enzo Marinari
Gleb Oshanin
Luca Peliti
author_sort Silvio Kalaj
collection DOAJ
container_title New Journal of Physics
description Motivated by a question about the sensitivity of knots’ diffusive motion to the actual sequence of nucleotides placed on a given DNA, here we study a simple model of a sequence-reading diffusion on a stretched chain with a frozen sequence of ‘letters’ A and B , having different interaction energies. The chain contains a single distortion—a hernia—which brings two consecutive letters at its bottom together such that they interact. Due to interactions with the solvent, the hernia performs a random hopping motion along the chain with the transition rates dependent on its actual position. Our two focal questions are (a) the dependence of various transport properties on the letters’ interaction energy and (b) whether these properties are self-averaging with respect to different realizations of sequences. We show that the current through a finite interval, the resistance of this interval and the splitting probabilities on this interval lack self-averaging. On the contrary, the mean first-passage time through a finite interval with N sites and the diffusion coefficient in a periodic chain are self-averaging in the limit $N \to \infty$ . Concurrently, two latter properties exhibit strong sample-to-sample fluctuations for finite N , as evidenced by numerical simulations.
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spelling doaj-art-b8a2decd41b04f33954d1f718efa50122025-08-20T03:15:04ZengIOP PublishingNew Journal of Physics1367-26302025-01-0127404302210.1088/1367-2630/adcd94A simple model of a sequence-reading diffusion: non-self-averaging and self-averaging propertiesSilvio Kalaj0Enzo Marinari1Gleb Oshanin2https://orcid.org/0000-0001-8467-3226Luca Peliti3Dipartimento di Fisica, Sapienza Università di Roma , P.le A. Moro 2, I-00185 Roma, Italy; Sorbonne Université , CNRS, Laboratoire de Physique Théorique de la Matière Condensée (UMR 7600), 4 Place Jussieu, 75252 Paris, Cedex 05, FranceDipartimento di Fisica, Sapienza Università di Roma , P.le A. Moro 2, I-00185 Roma, Italy; INFN, Sezione di Roma 1 and Nanotech-CNR , UOS di Roma, P.le A. Moro 2, I-00185 Roma, ItalySorbonne Université , CNRS, Laboratoire de Physique Théorique de la Matière Condensée (UMR 7600), 4 Place Jussieu, 75252 Paris, Cedex 05, France; Asia Pacific Center for Theoretical Physics , Hogil Kim Memorial Building 501 POSTECH, 37673 Pohang, Republic of KoreaSanta Marinella Research Institute , I-00058 Santa Marinella, ItalyMotivated by a question about the sensitivity of knots’ diffusive motion to the actual sequence of nucleotides placed on a given DNA, here we study a simple model of a sequence-reading diffusion on a stretched chain with a frozen sequence of ‘letters’ A and B , having different interaction energies. The chain contains a single distortion—a hernia—which brings two consecutive letters at its bottom together such that they interact. Due to interactions with the solvent, the hernia performs a random hopping motion along the chain with the transition rates dependent on its actual position. Our two focal questions are (a) the dependence of various transport properties on the letters’ interaction energy and (b) whether these properties are self-averaging with respect to different realizations of sequences. We show that the current through a finite interval, the resistance of this interval and the splitting probabilities on this interval lack self-averaging. On the contrary, the mean first-passage time through a finite interval with N sites and the diffusion coefficient in a periodic chain are self-averaging in the limit $N \to \infty$ . Concurrently, two latter properties exhibit strong sample-to-sample fluctuations for finite N , as evidenced by numerical simulations.https://doi.org/10.1088/1367-2630/adcd94diffusion in disordered mediaself-averaging vs non-self-averagingsample-to-sample fluctuations
spellingShingle Silvio Kalaj
Enzo Marinari
Gleb Oshanin
Luca Peliti
A simple model of a sequence-reading diffusion: non-self-averaging and self-averaging properties
diffusion in disordered media
self-averaging vs non-self-averaging
sample-to-sample fluctuations
title A simple model of a sequence-reading diffusion: non-self-averaging and self-averaging properties
title_full A simple model of a sequence-reading diffusion: non-self-averaging and self-averaging properties
title_fullStr A simple model of a sequence-reading diffusion: non-self-averaging and self-averaging properties
title_full_unstemmed A simple model of a sequence-reading diffusion: non-self-averaging and self-averaging properties
title_short A simple model of a sequence-reading diffusion: non-self-averaging and self-averaging properties
title_sort simple model of a sequence reading diffusion non self averaging and self averaging properties
topic diffusion in disordered media
self-averaging vs non-self-averaging
sample-to-sample fluctuations
url https://doi.org/10.1088/1367-2630/adcd94
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