TY - JOUR
T1 - Universality of active wetting transitions
AU - Sepúlveda, Néstor
AU - Soto, Rodrigo
N1 - Publisher Copyright:
© 2018 American Physical Society.
PY - 2018/11/27
Y1 - 2018/11/27
N2 - Four on-lattice and six off-lattice models for active matter are studied numerically, showing that in contact with a wall, they display universal wetting transitions between three distinctive phases. The particles, which interact via exclusion volume only, move persistently and, depending on the model, change their direction either via tumble processes or rotational diffusion. When increasing the turning rate νT, the systems transit from total wetting to partial wetting and dewetted phases. In the first phase, a wetting film covers the wall, with increasing heights while decreasing νT. The second phase is characterized by wetting droplets on the wall. And, finally, the wall dries with few particles in contact with it. These phases present two continuous nonequilibrium transitions. For the first transition, from partial to total wetting, the fraction of dry sites vanishes continuously when decreasing νT, with a power law of exponent 1. And, for the second transition, an order parameter proportional to the excess mass in droplets decreases continuously with a power law of exponent 3 when approaching a critical value of νT. The critical exponents are the same for all the models studied.
AB - Four on-lattice and six off-lattice models for active matter are studied numerically, showing that in contact with a wall, they display universal wetting transitions between three distinctive phases. The particles, which interact via exclusion volume only, move persistently and, depending on the model, change their direction either via tumble processes or rotational diffusion. When increasing the turning rate νT, the systems transit from total wetting to partial wetting and dewetted phases. In the first phase, a wetting film covers the wall, with increasing heights while decreasing νT. The second phase is characterized by wetting droplets on the wall. And, finally, the wall dries with few particles in contact with it. These phases present two continuous nonequilibrium transitions. For the first transition, from partial to total wetting, the fraction of dry sites vanishes continuously when decreasing νT, with a power law of exponent 1. And, for the second transition, an order parameter proportional to the excess mass in droplets decreases continuously with a power law of exponent 3 when approaching a critical value of νT. The critical exponents are the same for all the models studied.
UR - http://www.scopus.com/inward/record.url?scp=85057572273&partnerID=8YFLogxK
U2 - 10.1103/PhysRevE.98.052141
DO - 10.1103/PhysRevE.98.052141
M3 - Article
AN - SCOPUS:85057572273
SN - 1539-3755
VL - 98
JO - Physical Review E - Statistical, Nonlinear, and Soft Matter Physics
JF - Physical Review E - Statistical, Nonlinear, and Soft Matter Physics
IS - 5
M1 - 052141
ER -