Published
March 24, 2014

Physics 7, 31 (2014)

DOI:
10.1103/Physics.7.31
Nonlinear freak waves in water can be generated experimentally by exploiting the timereversal symmetry of the equations that govern their propagation.
Breathers are solutions of the nonlinear Schrödinger equation (NLS), which describes the dynamics of a large variety of nonlinear media including water, optical fibers, and clouds of BoseEinstein condensates. As reported in Physical Review Letters, Amin Chabchoub at the Swinburne University of Technology in Melbourne, Australia, and Mathias Fink at the Institut Langevin of the French National Center for Scientific Research (CNRS) have demonstrated the experimental generation of breathers in water [1] based on a particular mathematical property of the NLS: its timereversal symmetry. This property allows the authors, for the first time, to “refocus” breathers: after they are generated, propagated, and are recorded at some distance from the origin, the decayed nonlinear wave profile is timereversed and reemitted in such a way that their energy focuses back, as though a movie of the propagating waves had been played backwards. The effect, which occurs despite the inevitable presence of damping and noise, may be exploited for the generation of breathers in a variety of media or to study the role of nonlinearity in the formation of rogue waves.
Historically, the simplest approach to model freak waves has been the randomplanewave model, in which the linear superposition of waves leads to a statistical (Rayleigh) distribution of wave intensities. Yet, as confirmed by recent research on freak waves in microwave resonators [2], it has been known for many years that this underestimates by orders of magnitude the probability for the occurrence of freak waves. This puzzle remains unsolved even when the model is refined by including multiple wavescattering events. But two other physical effects could be responsible for the unexpectedly high frequency of freak waves observed in the real world: (i) nonlinearity, i.e., the formation of breathers and (ii) caustics, i.e., the focusing of waves to high intensity due to purely linear wave propagation in random media.
Caustics form naturally in random media and act like lenses for waves. They determine, for instance, the changing light patterns that you can see on the bottom of a swimming pool on sunny days. While the contribution of caustics to freak waves has recently been uncovered [3], the role of breathers in the formation of freak waves in the ocean is still foggy. Therefore, a way to experimentally control freak waves formed via breathers would be highly desirable.
Chabchoub and Fink tackle the nonlinear contribution to freak wave dynamics experimentally. They use a
The timereversal symmetry of the NLS would imply that a state at a given time could be backpropagated to yield the initial conditions that generated it. The timereversed signal would then lead to the reformation of a breather after propagating for
It is worth noting that time reversal of breathers as proposed by the authors may provide insight into a broader class of situations beyond freak waves. Moving breathers (more widely known as solitons) manifest themselves in rivers as part of tidal bores, in the form of a wave front followed by a train of solitons [6] (see Fig. 1). This phenomenon is well known among surfers: the tidal bore in the Severn River in the UK can carry surfers several miles upstream. A five star bore—the highest category—attracted surfers and “breather watching” spectators alike in February 2014.
The authors’ results may also have implications in other domains of physics. The NLS describes a variety of physical systems, including BoseEinstein condensates (BECs) confined to cigarshaped traps—a system that can be controlled experimentally with a very high precision. In the presence of an optical lattice potential, the NLS turns into a lattice equation: the discrete NLS. Generating breathers in BECs is appealing, as breathers are stable and localized matter waves that are coherent on long time scales [7], properties that could be used, for instance, in quantum computing. Experiments with BECs may address whether time reversal of decayed breathers is possible. However, quantum effects may pose an obstacle: classically instable motion (including the decay of a breather) leads to decoherence [8], which goes beyond the validity of the NLS.
While the scheme studied by the authors is one dimensional (like solitons in narrow rivers), future research may investigate the simulation of breathers in two dimensions, providing a more realistic approach to understand possible mechanisms for the formation and decay of freak waves on the ocean surface. Furthermore, disentangling nonlinear contributions (i.e., breathers) from linear contributions (i.e., caustics) to freakwave formation remains an outstanding challenge for researchers in a wide range of fields, including microwave chaos, nonlinear optics, and water waves.
References
 Amin Chabchoub and Mathias Fink, “TimeReversal Generation of Rogue Waves,” Phys. Rev. Lett. 112, 124101 (2014).
 H.J. Stöckmann, in Chaos, edited by B. Duplantier, S. Nonnenmacher, and V. Rivasseau Progress in Mathematical Physics, Vol 66 (Birkhäuser, Boston, 2013)[Amazon][WorldCat].
 R. Höhmann, U. Kuhl, H.J. Stöckmann, L. Kaplan, and E. J. Heller, “Freak Waves in the Linear Regime: A Microwave Study,” Phys. Rev. Lett. 104, 093901 (2010).
 A. Chabchoub, N. Hoffmann, M. Onorato, and N. Akhmediev, “Super Rogue Waves: Observation of a HigherOrder Breather in Water Waves,” Phys. Rev. X 2, 011015 (2012).
 A. Przadka, S. Feat, P. Petitjeans, V. Pagneux, A. Maurel, and M. Fink, “Time Reversal of Water Waves,” Phys. Rev. Lett. 109, 064501 (2012).
 M. A. Porter, N. J. Zabusky, B. Hu, and D. K. Campbell, “Fermi, Pasta, Ulam and the Birth of Experimental Mathematics,” American Scientist 97, 214 (2009).
 H. Hennig, D. Witthaut, and D. Campbell, “Global Phase Space of Coherence and Entanglement in a DoubleWell BoseEinstein Condensate,” Phys. Rev. A 86, 051604 (2012).
 Y. Castin and R. Dum, “Instability and Depletion of an Excited BoseEinstein Condensate in a Trap,” Phys. Rev. Lett. 79, 3553 (1997).
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