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We consider the motion of a harmonically trapped overdamped particle, which is submitted to a self-phoretic force, that is proportional to the gradient of a diffusive field for which the particle itself is the source. In agreement with existing results for free particles or particles in a bounded domain, we find that the system exhibits a transition between an immobile phase, where the particle stays at the center of the trap, and an oscillatory state. We perform an exact analysis giving access to the bifurcation threshold, as well as the frequency of oscillations and their amplitude near the threshold. Our analysis also characterizes the shape of two-dimensional oscillations that take place along a circle or a straight line. Our results are confirmed by numerical simulations.
Jan Steggemann, Konstantin Androsov, Anna Mascellani, Joanna Malgorzata Wanczyk
Mikhail Chapochnikov, Anna Tokareva
Olivier Schneider, Aurelio Bay, Guido Haefeli, Tatsuya Nakada, Frédéric Blanc, Lesya Shchutska, Yasmine Sara Amhis, François Fleuret, Yi Zhang, Mingkui Wang, Ian William Marison, Maxim Karpov, Arnout Lodewijk M Beckers, Chao Wang, Marco Calvi, Liang Sun, Michael Thompson McCann, John Martin Kolinski, Simone Meloni, Valérie Jeanne Thérèse Renaudin-Schouler, Basil Andrew Stansfield Davis, Craig Matthew Smith, Chunmin Zhang, Mercedes Hannelore Rittmann-Frank, Achille Mauri, I-Chun Lin, Xiaoqing Zhou, Marco Guarise, Roland Martin Andersson, Xiaoqiang Wang, Fabiano Colpo, Remy Jean Henry Albrecht, Yang Zou, Huizhen Liu, Chia-Chun Chen, Eliazar Rodriguez Garcia, Tao Zhou