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June 2, 20260 citationsOpen Access

The Tatvamasi attractor: a new chaotic attractor in a modified Rössler system with cubic dissipation

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RMRishabh Mehta

Key Points

  • This research aims to introduce a novel chaotic attractor within a modified Rössler system.
  • Introduced a three-dimensional autonomous system with cubic damping and cross-coupling nonlinearity.
  • Employed numerical integration to analyze system dynamics and stability.
  • Conducted equilibrium analysis and bifurcation diagram generation.
  • Identified a chaotic attractor with the largest Lyapunov exponent λ1 ≈ 0.0159.
  • Revealed two saddle-focus fixed points and a period-doubling route to chaos.
  • Established a Kaplan–Yorke dimension DKY ≈ 2.0003, indicating system novelty.

Abstract

We introduce a new three-dimensional autonomous system obtained by adding acubic damping term and a cross-coupling nonlinearity to the classical R¨ossler equations.The system is motivated by a simple physical model of a damped driven oscillator withnonlinear feedback. Through numerical integration we find a chaotic attractor forparameters a = 0.10, b = 0.2, c = 5.7, d = 0.20, e = 0.01. The largest Lyapunovexponent is λ1 ≈ 0.0159, confirming chaos, and the power spectrum is broadband.Equilibrium analysis reveals two saddle-focus fixed points. A bifurcation diagram asa function of d shows a period-doubling route to chaos, and a parameter-space heatmap in the (d, e) plane identifies the chaotic region. The full Lyapunov spectrum is(λ1, λ2, λ3) = (0.0159,−0.00957,−18.98), yielding a Kaplan–Yorke dimension DKY ≈2.0003. Searches in major databases yielded no identical system, indicating novelty.We propose to name this new chaotic attractor the Tatvamasi attractor.

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Cite This Study

Rishabh Mehta (2026) studied this question.

synapsesocial.com/papers/6a1e72ad30b38c64201b5dbahttps://doi.org/10.5281/zenodo.20477416
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