Exact solution for anisotropic mobility in trapped self-propelled particles yields non-monotonic negative excess kurtosis and a strictly sub-Gaussian steady-state distribution that displaces the particle into high-potential regions.
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Passive particle fraction drives continuous or discontinuous order-disorder transitions in self-aligning active matter depending on mobility anisotropy, captured by a mean-field equation from microscopic dynamics.
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Mobility Anisotropy Reshapes Self-Propelled Motion
Exact solution for anisotropic mobility in trapped self-propelled particles yields non-monotonic negative excess kurtosis and a strictly sub-Gaussian steady-state distribution that displaces the particle into high-potential regions.
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Passivity-Driven Order-Disorder Transitions in Self-Aligning Active Matter
Passive particle fraction drives continuous or discontinuous order-disorder transitions in self-aligning active matter depending on mobility anisotropy, captured by a mean-field equation from microscopic dynamics.