Skip to main content
. Author manuscript; available in PMC: 2023 Jan 18.
Published in final edited form as: Phys Rev X. 2022 Jan 18;12(1):011011. doi: 10.1103/physrevx.12.011011

FIG. 7.

FIG. 7.

Phase diagram for the gated RNN. (a) (no biases) In regions 1 and 2, the zero FP is the global attractor of dynamics; however, in region 2, there is a proliferation of unstable FPs without any asymptotic dynamical signatures. In region 3, the (stable) zero FP coexists with chaotic dynamics. Note that the plotted curve separating regions 2 and 3 is computed for αz = 0 and remains valid for sufficiently small values of αz. In region 4, the zero FP is unstable, and dynamics are chaotic. For all parameter values in region 5, a previously unstable or chaotic state can be made marginally stable when αz = ∞. For any given parameter values in region 5, there are infinitely many marginally stable points in the phase space to which the dynamics converge. The red dashed line indicates the critical transition between a stable fixed point (below the line) and chaos (above the line) in the presence of static random input (to the h variable) with standard deviation σh = 0.5. Note that, while chaos is suppressed for small αr along the gh axis, for larger αr there are regions of stable FPs that become chaotic with finite input. This leads to the phenomenon of input-induced chaos.