Research

Keywords: nonlinear dynamics, random dynamical systems, coupled oscillators, coupled map lattices, chaos, bifurcations, statistical physics

🔷 Topic on bifurcations (or phase transitions) in coupled dissipative systems, with periodic/aperiodic drivings, with or without noise [ongoing]

🔷 Topic on prethermalisation of coupled aperiodically kicked rotor systems: 

Time-dependent drivings may realise novel non-equilibrium phases of matter, however, they generally heat up to infinite temperature due to the absence of energy conservation. A long-lived prethermal state has been discovered in periodically driven systems. 

A natural question is whether prethermalisation can still exist without perfect periodicity. A positive answer is given here by a system of classical coupled rotors subject to a family of random kicks with n-multipolar temporal correlations. The heating, characterised by the averaged kinetic energy (fig.(a)), can be algebraically controlled by the kicking strength K, where the scaling exponent linearly depends on the multipolar order n (fig.(b)). In the limit of n going to infinity (the so-called quasi-periodic Thue-Morse sequence), the prethermal lifetime t* has an abnormal scaling in-between exponential and power law (fig.(c)). 

🔷 Topic on simple random maps

A random dynamical system consists of a setting in which different types of dynamics are generated randomly in time. 

Here, we consider a simplest possible case where an irregular or a regular dynamics is randomly selected at each time step. By varying the sampling probability p, the system exhibits a non-trivial transition from fully chaotic to completely regular dynamics. At the critical point p = 1/2, the anomalous behaviour is characterised by an infinite non-normalisable invariant density, weak ergodicity breaking and power-law correlation decay (see plot to the left).

🔷 Topic on coupled Nth-order Chebyshev maps: 

Chebyshev maps - defined by Chebyshev polynomials - are distinguished in the sense that they have least higher-order correlations among all smooth 1D maps that are conjugated to an N-ary shift (i.e., a Bernoulli shift of N symbols). The eigenspectrum of their Perron-Frobenius operator (or transfer operator) can be analytically derived explicitly via a topological conjugation, given an appropriate functional space. Their coupled map lattices exhibit rich and complex behaviour, for example, a series of plots below shows the probability distribution on the attractor of two coupled 2nd-order Chebyshev maps in varying the coupling strength c

The vanishing spatial and temporal correlations may have profound physical interpretations in stochastically quantised field theories. 

🔷 Topic on coupled oscillators --- for modelling Josephson junction (JJ) arrays or detecting axion-like dark matter in a superconductor (JJ) environment: 

An axion field (the signal) coupled to a Josephson junction (the detector) by means of a capacitive coupling of arbitrary size is described by a system of 2nd-order ODEs. Depending on the system parameters and initial conditions, we find a rich phase space structure of this nonlinear system; the three plots below show a topological transition under variations of the frequency ratio, projected onto a 3D subspace of the 4D phase space, with the fourth dimension shown in colour. 

Other interests: cosmology (dark side of the universe), complex networks (in neural and social sciences), data visualisation, mathematical-related arts