Odd Response-Induced Phase Separation of Active Spinners
Yu Ding,
Boyi Wang,
Qing Yang,
Zhiyuan Zhao,
Shigeyuki Komura,
Ryohei Seto,
Mingcheng Yang,
Fangfu Ye
Affiliations
Yu Ding
Beijing National Laboratory for Condensed Matter Physics and Laboratory of Soft Matter Physics, Institute of Physics,
Chinese Academy of Sciences, Beijing 100190, China.
Boyi Wang
Beijing National Laboratory for Condensed Matter Physics and Laboratory of Soft Matter Physics, Institute of Physics,
Chinese Academy of Sciences, Beijing 100190, China.
Qing Yang
Beijing National Laboratory for Condensed Matter Physics and Laboratory of Soft Matter Physics, Institute of Physics,
Chinese Academy of Sciences, Beijing 100190, China.
Zhiyuan Zhao
Wenzhou Institute,
University of Chinese Academy of Sciences, Wenzhou, Zhejiang 325001, China.
Shigeyuki Komura
Wenzhou Institute,
University of Chinese Academy of Sciences, Wenzhou, Zhejiang 325001, China.
Ryohei Seto
Wenzhou Institute,
University of Chinese Academy of Sciences, Wenzhou, Zhejiang 325001, China.
Mingcheng Yang
Beijing National Laboratory for Condensed Matter Physics and Laboratory of Soft Matter Physics, Institute of Physics,
Chinese Academy of Sciences, Beijing 100190, China.
Fangfu Ye
Beijing National Laboratory for Condensed Matter Physics and Laboratory of Soft Matter Physics, Institute of Physics,
Chinese Academy of Sciences, Beijing 100190, China.
Due to the breaking of time-reversal and parity symmetries and the presence of non-conservative microscopic interactions, active spinner fluids and solids respectively exhibit nondissipative odd viscosity and nonstorage odd elasticity, engendering phenomena unattainable in traditional passive or active systems. Here, we study the effects of odd viscosity and elasticity on phase behaviors of active spinner systems. We find the spinner fluid under a simple shear experiences an anisotropic gas–liquid phase separation driven by the odd-viscosity stress. This phase separation exhibits equilibrium-like behavior, with both binodal-like and spinodal curves and critical point. However, the formed dense liquid phase is unstable, since the odd elasticity instantly takes over the odd viscosity to condense the liquid into a solid-like phase. The unusual phase behavior essentially arises from the competition between thermal fluctuations and the odd response-induced effective attraction. Our results demonstrate that the cooperation of odd viscosity and elasticity can lead to exotic phase behavior, revealing their fundamental roles in phase transition.