2008
DOI: 10.1016/j.physrep.2008.05.002
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Discrete breathers — Advances in theory and applications

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Cited by 941 publications
(879 citation statements)
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References 394 publications
(711 reference statements)
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“…An example is given in [26, Section 2.2 & 2.3, pg. [9][10][11][12][13][14][15][16][17][18], where the minimization of a linear energy functional under a nonlinear constraint verified conditions for the co-existence of breather profiles. For instance, this alternative approach for (2.1) will show the existence of a regime for the hopping parameter α where an upper bound for the power is valid (see Remark II.3).…”
Section: Finite Dimensional Latticesmentioning
confidence: 99%
See 1 more Smart Citation
“…An example is given in [26, Section 2.2 & 2.3, pg. [9][10][11][12][13][14][15][16][17][18], where the minimization of a linear energy functional under a nonlinear constraint verified conditions for the co-existence of breather profiles. For instance, this alternative approach for (2.1) will show the existence of a regime for the hopping parameter α where an upper bound for the power is valid (see Remark II.3).…”
Section: Finite Dimensional Latticesmentioning
confidence: 99%
“…Partly also due to these applications, the DNLS has been a focal point of numerous mathematical/computational investigations in its own right, a number of which has been summarized in [8][9][10][11][12][13] and is related to models used in numerous other settings including micromechanical cantilever arrays [14] and DNA breathing dynamics [15], among others.…”
Section: Introductionmentioning
confidence: 99%
“…Such solutions can be generated from localized initial conditions or may arise from modulational instabilities of periodic waves [12,13,26]. Although such properties are classical in the context of anharmonic Hamiltonian lattices [9], energy localization is particularly strong in the DpS equation. Indeed, it is proved in [3] that the solution of (1) does not disperse for any nonzero initial condition in ℓ2(Z) (i.e.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…The case i = 1 yields the so-called even-parity modes (or site-centered solutions), and the case i = 2 corresponds to odd-parity modes (bond-centered solutions). These solutions were numerically computed in [12,26,13] for p = 5/2 (see also [9,23] and references therein in the case p = 4 with an additional on-site cubic nonlinearity).…”
Section: Theorem 1 the Stationary Dps Equationmentioning
confidence: 99%
“…While ILMs are spatially localized nonlinear excitations that occur in perfect crystals [28][29][30] , in this model a local enhancement of the nonlinearity associated with off-centring Pb atoms 31 instigates the formation of ILMs on cooling [25][26][27] . The ILM frequency then slows below that of the TO phonon into the frequency gap between the TA and TO phonons, and eventually vanishes as PNRs become static [25][26][27] .…”
mentioning
confidence: 97%