Dynamic of a pest management system with hibernation of pests and impulsive nonlinear release of natural enemies. [PDF]
Sun H, Jiao J, Dai X, Wu L.
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Bifurcation analysis and analytical traveling wave solutions of a sasa-satsuma equation involving beta, M-truncated and conformable derivatives using the EGREM method. [PDF]
Munir F +5 more
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Harmonic trophic potentials and memory effects in ecological dynamics in resource-limited ecosystems through the Generalized Lotka-Volterra model with biomass constraints. [PDF]
Marinho JAO, da Rocha HO, Reis FPP.
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Topological phase locking in stochastic oscillators. [PDF]
Chatzittofi M +2 more
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A lightweight multi round confusion-diffusion cryptosystem for securing images using a modified 5D chaotic system. [PDF]
Anujaa T +6 more
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Secure Signal Encryption in IoT and 5G/6G Networks via Bio-Inspired Optimization of Sprott Chaotic Oscillator Synchronization. [PDF]
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Music Analysis with Phase Portraits
2021Many complications in music theory are derived from the line system for writing musical notes: The intervals of lines are not equal, although the physical intervals of two adjacent lines are equal. Different from such a line system we introduce a method to interpret musical pieces by the dynamical approach of the phase plot.
Kinko Tsuji, Stefan C. Müller
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Global Phase Portraits of Memristor Oscillators
International Journal of Bifurcation and Chaos, 2014In this paper, the global dynamics of memristor oscillators are investigated. For the sake of analysis, we first reformulate the original system into a simple form, which has only three parameters, and analyze its dynamics according to the variation of the parameters.
Chen, Hebai, Li, Xuefang
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Phase Portraits of Quantum Systems
Few-Body Systems, 2013We formulate a general approach to construct phase portraits of a quantum system in the Fock–Bargmann space. This approach is applied to simple model problems and two-cluster nuclei as well.
Yu. A. Lashko +3 more
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Consider a dynamical system of two coupled ordinary differential equations (ODEs) of the general structure $$ \dot{x} \equiv \frac{{dx}}{{dt}} = P(x,y),\dot{y} \equiv \frac{{dy}}{{dt}} = Q(x,y) $$ (5.1) where P and Q are known functions of the dependent variables x and y and the independent variable has been taken to be the time t.
Richard H. Enns, George C. McGuire
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