TY - JOUR
T1 - Rogue wave formation scenarios for the focusing nonlinear Schrödinger equation with parabolic-profile initial data on a compact support
AU - Demontis, F.
AU - Ortenzi, Giovanni
AU - Roberti, Giacomo
AU - Sommacal, Matteo
N1 - Funding information: The authors would like to thank the Mathematics of Complex and Nonlinear Phenomena (MCNP) research group members at Northumbria University and, in particular, T. Bonnemien (now at King's College), T. Congy, and G. El for useful remarks. In particular, the authors are indebted to G. El for providing them with a physical copy of . The authors would also like to thank B. Jenkins, S. Lombardo, A. Tovbis, and C. van der Mee for enlightening discussions. G.O. would like to thank B. Suleimanov for bringing to his attention. G.R. and M.S. would like to thank the Isaac Newton Institute for Mathematical Sciences for support and hospitality during the Dispersive Hydrodynamics programme, when work on this paper was undertaken (EPSRC Grant No. EP/R014604/1). G.R.'s work was also supported by the Simon Foundation and by the EPSRC Grant No. EP/W032759/1. G.O.'s work was partly supported by the European Union's Horizon 2020 research and innovation programme under the Marie Skłodowska-Curie Grant No. 778010 IPaDEGAN. The work of G.O. was carried out within the framework of the MMNLP (Mathematical Methods in Non-Linear Physics) project of the INFN (Istituto Nazionale Fisica Nucleare). Finally, the work of F.D., G.O., and M.S. has been carried out under the auspices of the Italian GNFM (Gruppo Nazionale Fisica Matematica), INdAM (Istituto Nazionale di Alta Matematica), which is gratefully acknowledged.
PY - 2023/8/11
Y1 - 2023/8/11
N2 - We study the (1+1) focusing nonlinear Schrödinger equation for an initial condition with compactly supported parabolic profile and phase depending quadratically on the spatial coordinate. In the absence of dispersion, using the natural class of self-similar solutions, we provide a criterion for blowup in finite time, generalizing a result by Talanov et al. In the presence of dispersion, we numerically show that the same criterion determines, even beyond the semiclassical regime, whether the solution relaxes or develops a high-order rogue wave, whose onset time is predicted by the corresponding dispersionless catastrophe time. The sign of the chirp appears to determine the prevailing scenario among two competing mechanisms for rogue wave formation. For negative values, the numerical simulations are suggestive of the dispersive regularization of a gradient catastrophe described by Bertola and Tovbis for a different class of smooth, bell-shaped initial data. As the chirp becomes positive, the rogue wave seems to result from the interaction of counterpropagating dispersive dam break flows, as in the box problem recently studied by El, Khamis, and Tovbis. As the chirp and amplitude of the initial profile are relatively easy to manipulate in optical devices and water tank wave generators, we expect our observation to be relevant for experiments in nonlinear optics and fluid dynamics.
AB - We study the (1+1) focusing nonlinear Schrödinger equation for an initial condition with compactly supported parabolic profile and phase depending quadratically on the spatial coordinate. In the absence of dispersion, using the natural class of self-similar solutions, we provide a criterion for blowup in finite time, generalizing a result by Talanov et al. In the presence of dispersion, we numerically show that the same criterion determines, even beyond the semiclassical regime, whether the solution relaxes or develops a high-order rogue wave, whose onset time is predicted by the corresponding dispersionless catastrophe time. The sign of the chirp appears to determine the prevailing scenario among two competing mechanisms for rogue wave formation. For negative values, the numerical simulations are suggestive of the dispersive regularization of a gradient catastrophe described by Bertola and Tovbis for a different class of smooth, bell-shaped initial data. As the chirp becomes positive, the rogue wave seems to result from the interaction of counterpropagating dispersive dam break flows, as in the box problem recently studied by El, Khamis, and Tovbis. As the chirp and amplitude of the initial profile are relatively easy to manipulate in optical devices and water tank wave generators, we expect our observation to be relevant for experiments in nonlinear optics and fluid dynamics.
UR - http://www.scopus.com/inward/record.url?scp=85167993518&partnerID=8YFLogxK
U2 - 10.1103/PhysRevE.108.024213
DO - 10.1103/PhysRevE.108.024213
M3 - Article
AN - SCOPUS:85167993518
SN - 2470-0045
VL - 108
JO - Physical Review E
JF - Physical Review E
IS - 2
M1 - 024213
ER -