How self-propulsion changes the glass transition of dense active matter · revision history

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Title
How self-propulsion changes the glass transition of dense active matter
Plain
Dense crowds of self-propelled particles, such as packed cell layers or active colloids, become glassy and nearly stop moving, much like a cooling liquid. Whether this active glass follows the same physics as an ordinary glass with an effective temperature, or a different one, is not known.
Precise
For dense active Brownian or active Ornstein-Uhlenbeck particles with active force $f_0$ and persistence time $\tau_p$, determine the dynamical arrest line $\phi_g(f_0, \tau_p)$ and whether fragility, dynamic heterogeneity ($\chi_4$) and the relaxation spectrum map onto those of the passive glass at an effective temperature, given reports that $\tau_{\alpha}$ depends non-monotonically on $\tau_p$ at fixed effective temperature. An answer is the arrest diagram with a quantitative test of the effective-temperature mapping and a theory that predicts where it fails.
Settled by
Simulations over several decades of $\tau_{\alpha}$ and $\tau_{p}$, compared with an active mode-coupling or other theory, and with measurements on dense active colloids or cell monolayers.
Kind
phenomenon
Answer type
classification
References
(empty)
Literature status
open
Status note
Reviewed in 2019 (Janssen, Active glasses, J. Phys.: Condens. Matter, https://doi.org/10.1088/1361-648X/ab3e90); no consensus theory as of 2026.
Posed since
(empty)