“…[6][7][8][9][10] These systems have wide applications in physics, in areas as diverse as fluids, quantum mechanics, superconductivity, plasma physics, optical systems, astrophysics, and high-energy accelerators. 3,[11][12][13][14][15] Motivated by this more recent trend in research, and in line with previous work searching for simple systems of a given form that exhibit chaotic behavior, [16][17][18][19][20] this work began with a search for simple driven chaotic oscillators with a complex variable z, of the form ż + f͑z͒ = e i⍀t . This form is equivalent, with z = x + iy and f͑z͒ = u͑x , y͒ + iv͑x , y͒, where u and v are real functions, to the driven two-dimensional system, ẋ = − u͑x,y͒ + cos ⍀t, ͑1͒ ẏ = − v͑x,y͒ + sin ⍀t, which can be recast as the autonomous three-dimensional system, ẋ = − u͑x,y͒ + cos ⍀t, ẏ = − v͑x,y͒ + sin ⍀t, ͑2͒ ṫ = 1.…”