“…The consideration of two co-propagating wavepackets in a particular plasma fluid and their mutual interaction, results in a pair of coupled NLS (CNLS) equations, whose coefficients generally depend on the carrier wavenumber(s) of the respective carrier waves. Electron plasma (Langmuir) waves and ion acoustic waves [24,25,26], amidst other studies that focused mostly on electromagnetic modes [27,28,29,30,31,32,33]. Beyond plasma science, general forms of CNLS equations have been investigated in recent years with respect to the existence of vector solitons, breathers, and rogue wave solutions, in contexts including higher-order coupled NLS systems [34,35], coupled mixed-derivative NLS equations [36,37,38], variable coefficients CNLS equations [39], non-autonomous CNLS equations [40,41,42], systems involving four-wave mixing terms [43], coupled cubic-quintic NLS equations [44], space-shifted CNLS equations [45] and non-autonomous partially non-local CNLS equations [46], among others.…”