We develop a nonlinear Schr¨odinger equation with an oceanicinspired structure. Using the de Broglie–Bohm formalism with an adimensional phase, we derive the hydrodynamic equations, obtain Gaussian solutions with time-dependent width, construct an ErmakovLewis-type invariant, and present a Feynman propagator formulation.
Wepropose a nonlinear dissipative Schr¨odinger equation describing deep oceanic wave envelopes with exponential growth, logarithmic dissipation, and Bohmian hydrodynamic structure. The model combines a logarithmic nonlinear interaction with a time-dependent Ermakov–Lewis framework, generating dissipative continuity and Euler equations in the Madelung–Bohm representation. The resulting formalism admits Gaussian envelope solutions, rogue-wave growth regimes, and dissipative soliton-like structures. An associated Ermakov equation governing the temporal width of the oceanic envelope is derived, together with a generalized ErmakovLewis invariant. The theory establishes a connection between nonlinear quantum hydrodynamics and oceanic wave dynamics in deep water environments.
A nonlinear Bohmian Schr¨odinger equation for oceanic wave dynamics is proposed using the Madelung–de Broglie–Bohm hydrodynamic formalism. The probability density is interpreted as the oceanic wave intensity. The model incorporates saturable nonlinear effects, curvature corrections and nonlinear gradient contributions. The associated continuity equation and Euler-type equation are derived. A generalized Ermakov–Lewis invariant is developed together with a Bohmian Feynman propagator. Exact bright soliton solutions are obtained in the weak saturation regime. The model may describe coherent oceanic structures, rogue-wave precursors and nonlinear hydrodynamic wave packets.
We propose a dissipative nonlinear Schr¨odinger equation describing interactions between deep and shallow oceanic waves within the de Broglie–Bohm hydrodynamic formalism. The model incorporates logarithmic, cubic and square-root nonlinearities without the presence of a harmonic oscillator potential. Through a suitable transformation, the dissipative continuity equation and dissipative Euler equation are mapped into conservative forms. The corresponding Ermakov–Lewis invariant is obtained, together with hybrid solitonic solutions and the associated Feynman propagator. The uncertainty relation is analyzed in terms of the competition between logarithmic confinement and nonlinear oceanic interactions.
Anonlinear dissipative Schr¨odinger equation describing deep ocean wave collapse is proposed within the hydrodynamic De Broglie-Bohm framework. The probability density is interpreted as the intensity of deep ocean waves. The model generates simultaneously a dissipative continuity equation and a dissipative Euler equation. A unique exponential variable transformation converts both equations into conservative forms. The associated Bohmian Feynman propagator is constructed through the effective action formalism and path integral approach. The model naturally describes focusing collapse, rogue-wave amplification, nonlinear dissipation, and hydrodynamic quantum trajectories.
Abstract In this work we propose a nonlinear non-dissipative Schr¨odinger equation capable of describing geyser-type oceanic wave structures within the de Broglie–Bohm hydrodynamic formalism. The model is constructed assuming a conservative continuity equation and a conservative Euler equation. The wave intensity is interpreted as an oceanic wave density field. A periodic nonlinear interaction term is introduced in order to generate eruptive and pulsating wave dynamics similar to geyser structures. The corresponding Bohm quantum potential and hydrodynamic equations are derived explicitly.