2021
DOI: 10.1103/physreve.103.022601
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Active particles with polar alignment in ring-shaped confinement

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Cited by 16 publications
(8 citation statements)
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“…33 Further, chiral active particles with polar (i.e., ferromagnetic Heisenberg-like) interactions exhibit rotating macrodroplets, 34,35 chimera states, [36][37][38] chiral selfrecognition, 39 dynamical frustration, 40 or a surface-population reversal effect in ring-shaped confinement. 41 Additional effects can arise in the presence of a rotating magnetic field, where disk-shaped chiral active particles without anisotropic interactions can display chiral separation and polar ordering. 42 In the present study, we go one step further and consider chiral active particles with dipole-dipole interactions.…”
Section: Introductionmentioning
confidence: 99%
“…33 Further, chiral active particles with polar (i.e., ferromagnetic Heisenberg-like) interactions exhibit rotating macrodroplets, 34,35 chimera states, [36][37][38] chiral selfrecognition, 39 dynamical frustration, 40 or a surface-population reversal effect in ring-shaped confinement. 41 Additional effects can arise in the presence of a rotating magnetic field, where disk-shaped chiral active particles without anisotropic interactions can display chiral separation and polar ordering. 42 In the present study, we go one step further and consider chiral active particles with dipole-dipole interactions.…”
Section: Introductionmentioning
confidence: 99%
“… 26 , 29 , 30 , 53 , 54 and references therein). Although these phenomena are enabled and sustained by particle activity, they can arise only in the presence of interparticle and particle-wall interactions, including Vicsek 26 , 29 , 55 and Vicsek-like 56 – 59 alignment interactions and hydrodynamic interactions 57 , 60 . Most of the aforementioned phenomena can emerge in active systems with only short-ranged steric interactions between the constituent particles, signifying their generic nature.…”
Section: Introductionmentioning
confidence: 99%
“…Active bath-mediated interactions between suspended inclusions can substantially be affected also by the presence of any confining boundaries 51 , 77 , shape, mobility and concentrations 48 , 51 , 52 , 68 , 75 , 78 and, if present, dissimilarity 49 , 69 and permeability 52 , 79 of the inclusions. On the other hand, the shape of active particles itself plays a crucial role in determining their bulk properties 37 , 80 – 83 , near-wall accumulations at rigid 40 43 , 56 , 84 and deformable 85 87 boundaries and, hence, the active (or ‘swim’) pressure they exert on these boundaries 56 , 64 , 79 , 88 , 89 , and the effective interactions they mediate between external objects 47 , 66 , 68 , 69 . For instance, the nonequilibrium wall accumulation of self-propelled rods turns out to be weaker than that of self-propelled disks 41 , 42 .…”
Section: Introductionmentioning
confidence: 99%
“…33 Further, chiral active particles with polar (i.e., ferromagnetic Heisenberg-like) interactions exhibit rotating macrodroplets, 34,35 chimera states, [36][37][38] chiral selfrecognition, 39 dynamical frustration, 40 or a surface-population reversal effect in ring-shaped confinement. 41 Additional effects can arise in the presence of a rotating magnetic field, where diskshaped chiral active particles without anisotropic interactions can display chiral separation and polar ordering. 42 In the present study, we go one step further and consider chiral active particles with dipole-dipole interactions.…”
Section: Introductionmentioning
confidence: 99%