“…where ϕpξq " ξ 1`ξ 2 , D x " 1 i B x and ϕpD x q is the Fourier multiplier operator defined by p w p,q s pMq " $ ' ' ' ' & ' ' ' ' % F L q s pMq (Fourier-Lebesgue spaces) if p " q M 2,q s pMq (modulation spaces) if p " 2 M 2,2 s pMq " W 2,2 s pMq " H s pMq (Sobolev spaces) if p " q " 2 F L q s pMq " M p,q s pMq " W p,q s pMq if M " T d . These time-frequency spaces are proven to be very fruitful in handling various problems in analysis and have gained prominence in nonlinear dispersive PDEs, e.g., [7][8][9][10][11][12][13][14][15]. We now state our main theorem.…”