2009
DOI: 10.1209/0295-5075/85/38001
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Dynamics of a bubble formed in double-stranded DNA

Abstract: We study the fluctuational dynamics of a tagged base-pair in double stranded DNA. We calculate the drift force which acts on the tagged base-pair using a potential model that describes interactions at base pairs level and use it to construct a Fokker-Planck equation.The calculated displacement autocorrelation function is found to be in very good agreement with the experimental result of Altan-Bonnet et. al. Phys. Rev. Lett. 90, 138101 (2003) over the entire time range of measurement. We calculate the most pro… Show more

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Cited by 15 publications
(10 citation statements)
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“…Simple models, e.g, Poland Scheraga (PS) model [9] or Peyrard-Bishop-Dauxious (PBD) model [10][11][12] have described some of the essential macroscopic features of the meting profile of dsDNA quite effectively and predicted that the force-induced melting transition is a first order transition [14][15][16]. However, semimicroscopic information about the opening such as whether a dsDNA opens from the end or interior of the chain, distribution of partially opened regions in the form of bubbles in the chain [12,13,[17][18][19][20], are some of the intriguing issues in these studies. Moreover, in all SMFS experiments, the experimental setup puts an extra constraint on the ends of the chain, which makes force-induced melting different from the thermal melting.…”
Section: Introductionmentioning
confidence: 99%
“…Simple models, e.g, Poland Scheraga (PS) model [9] or Peyrard-Bishop-Dauxious (PBD) model [10][11][12] have described some of the essential macroscopic features of the meting profile of dsDNA quite effectively and predicted that the force-induced melting transition is a first order transition [14][15][16]. However, semimicroscopic information about the opening such as whether a dsDNA opens from the end or interior of the chain, distribution of partially opened regions in the form of bubbles in the chain [12,13,[17][18][19][20], are some of the intriguing issues in these studies. Moreover, in all SMFS experiments, the experimental setup puts an extra constraint on the ends of the chain, which makes force-induced melting different from the thermal melting.…”
Section: Introductionmentioning
confidence: 99%
“…But strand dynamics is expected to be dominant at least for long DNAs and large bubbles, since for a flexible chain of length N the Rouse diffusion time scales like N 2 . (iii) Other models fit well the experimental autocorrelation function [9,16,17], but with the relaxation time as a fitting parameter, which does not shed light on the origin of such large times.…”
Section: Introductionmentioning
confidence: 87%
“…It has recently regained interest with the development of new experimental tools that allow for the direct observation of the dynamics of a single DNA molecule [7,8]. On the theoretical side, various methods have been used to study different aspects of the breathing process [9,10], and to investigate the interaction of the DNA with binding proteins: the master equation approach [11,12], a stochastic Gillespie scheme [13], the Fokker-Planck equation approach based on the Poland-Scheraga free energy function [5,[14][15][16], and stochastic dynamic simulations based on the Dauxios-Peyrard-Bishop model [17,18]. Specifically, the thermally-induced denaturation problem has been recently studied by mapping it onto a quantum Coulomb problem [19,20].…”
Section: Introductionmentioning
confidence: 99%
“…Using the BFP method, we derive and solve differential equations for the Laplace transforms of various Brownian functionals. This is in contrast to the standard Fokker-Planck treatment, which yields the distribution function to obtain a bubble of a given size at a given time [14][15][16]18]. Utilizing the PD approach, we can calculate the distribution functions of interest by splitting a representative path of the dynamics into parts, and then considering the weight of each part separately.…”
Section: Introductionmentioning
confidence: 99%