2001
DOI: 10.1016/s0375-9601(01)00013-5
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Darboux integration of

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Cited by 19 publications
(35 citation statements)
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“…All these equations were of the form iρ = [H, f (ρ)] where [f (ρ), ρ] = 0. Their physically nontrivial solutions were found in [73] for f (ρ) = ρ 2 and recently generalized to other f 's in [74]. A link of such general f 's with nonextensive statistical mechanics was described in [75].…”
mentioning
confidence: 89%
“…All these equations were of the form iρ = [H, f (ρ)] where [f (ρ), ρ] = 0. Their physically nontrivial solutions were found in [73] for f (ρ) = ρ 2 and recently generalized to other f 's in [74]. A link of such general f 's with nonextensive statistical mechanics was described in [75].…”
mentioning
confidence: 89%
“…Another important property of the dynamics is that (6) is integrable in the sense of soliton theory for any f . A soliton technique of solving (6), based on Darboux transformations, was introduced in [14], and further developed in [32,33,34]. Therefore, as opposed to standard kinetic equations that typically have to be solved numerically, we can work with exact analytic solutions.…”
Section: Soliton Kinetic Equationsmentioning
confidence: 99%
“…There exists a class of solutions of (4) which exhibits a kind of a three-regime switching effect [23][24][25]: For times −∞ < t ≪ t 1 the dynamics looks as if there was not feedback, then in the switching regime t 1 < t < t 2 a 'sudden' transition occurs which drives the system into a new state which for times t 2 ≪ t < ∞ evolves again as if there was no feedback. Of course, the feedback is present for all times, but is 'visible' only during the switching period.…”
Section: Soliton Morphogenesismentioning
confidence: 99%