2008
DOI: 10.1140/epjd/e2008-00237-5
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Wave propagation of nonlinear modes and formation of bubble in a two-component helicoidal lattice

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Cited by 26 publications
(32 citation statements)
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“…Of course, the reader should notice that from the beginning we did not include any noise to the model, rather these fluctuations in the breather solution are due to wave collision, i.e., at the point where the two counter-propagating waves mix. However, the features of that solution are expected to change for different values of the helicoidal coupling parameters S. This may be evident as the unwinding of the double helix implies a decrease of S. It was in fact shown that the resonant mode, the one supporting highly localized bubbles, is possible only when the helicoidal effects are weak [12,25]. Therefore, in the rest of the present work, the effect of small helicoidal coupling on the mixed solution is discussed.…”
Section: The Mixed Solutionsmentioning
confidence: 89%
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“…Of course, the reader should notice that from the beginning we did not include any noise to the model, rather these fluctuations in the breather solution are due to wave collision, i.e., at the point where the two counter-propagating waves mix. However, the features of that solution are expected to change for different values of the helicoidal coupling parameters S. This may be evident as the unwinding of the double helix implies a decrease of S. It was in fact shown that the resonant mode, the one supporting highly localized bubbles, is possible only when the helicoidal effects are weak [12,25]. Therefore, in the rest of the present work, the effect of small helicoidal coupling on the mixed solution is discussed.…”
Section: The Mixed Solutionsmentioning
confidence: 89%
“…In both cases, trains of soliton-like structures, with breathing features, are observed. Their importance in collecting the energy necessary for the initiation of the key precesses of replication and transcription has been discussed in many DNA nonlinear models, with suitable biological implications [7,10,12]. Indeed, the breaking of the hydrogen bonds starts with slight oscillations of the bases and then grow progressively in amplitude under the action of RNA-polymerase till the breaking of the hydrogen bond, condition for the genetic information to be collected by the messenger-RNA.…”
Section: Amplitude Equationsmentioning
confidence: 99%
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“…• −1 [51] without any arguments. It was suggested that the corresponding wave length covers an integer number of the periods l [40], i.e.…”
Section: The Helicoidal Peyrard-bishop (Hpb) Modelmentioning
confidence: 99%