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

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.

Authors

Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-05-30
DOI
https://doi.org/10.5281/zenodo.20477416
Primary Topic
Chaos control and synchronization
Type
preprint
Controls
|||
ALL TIME
JAN
FEB
MAR
APR
MAY
JUN
JUL
AUG
SEP
OCT
preprint

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

Rishabh Mehta
Zenodo (CERN European Organization for Nuclear Research)
Chaos control and synchronization
preprint

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

Rishabh Mehta
preprint en

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.

Zenodo (CERN European Organization for Nuclear Research)
Chaos control and synchronization
AI Navigator

Ask Laika to Summarize, Analyze, and Connect papers live on the map.

Summarize Papers & Methodologies

Extract key findings, datasets, and comparative methods across publications.

Benchmark Rankings & Visual Analytics

Rank top research institutions, authors, funders, topics, and journals by Field-Weighted Citation Impact (FWCI) and paper volume with instant charts.

Connect Distant Disciplines

Bridge topological clusters on the map to find hidden collaborative intersections.