The four-wing attractor is a striking example of a chaotic system whose trajectories unfold into four distinct lobes, or “wings,” in phase space. Unlike classical chaotic attractors such as the Lorenz attractor, which typically exhibit two dominant wings, the four-wing attractor arises from modified nonlinear dynamical equations that introduce additional symmetry and coupling between variables. As the system evolves over time, its state spirals unpredictably between these four regions, never set