Wave fields corresponding to different steady-state dynamics at droplet impact. The droplet is denoted by a blue circle for in-phase impacts and a red circle when in flight for antiphase dynamics. Walking droplets for (a) δx = 0.065 with Γ /Γ F = 0.9 and (b) δx = 0.08 with Γ /Γ F = 0.96. Two anticlockwise orbiting droplets with Γ /Γ F = 0.91 for (c) in-phase and (d) antiphase impacts. A single droplet orbiting anticlockwise under a central force for Γ /Γ F = 0.975 with orbit radius (e) R d = 0.45 and ( f ) R d = 0.95.

Wave fields corresponding to different steady-state dynamics at droplet impact. The droplet is denoted by a blue circle for in-phase impacts and a red circle when in flight for antiphase dynamics. Walking droplets for (a) δx = 0.065 with Γ /Γ F = 0.9 and (b) δx = 0.08 with Γ /Γ F = 0.96. Two anticlockwise orbiting droplets with Γ /Γ F = 0.91 for (c) in-phase and (d) antiphase impacts. A single droplet orbiting anticlockwise under a central force for Γ /Γ F = 0.975 with orbit radius (e) R d = 0.45 and ( f ) R d = 0.95.

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A droplet may ‘walk’ across the surface of a vertically vibrating bath of the same fluid, due to the propulsive interaction with its wave field. This hydrodynamic pilot-wave system exhibits many dynamics previously believed to exist only in the quantum realm. Starting from first principles, we derive a discrete-time fluid model, whereby the bath–dr...

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Context 1
... is formulated as many 4 × 4 linear systems subject to (6.6), akin to finding the walking states. An example in-phase wave field is given in figure 4(c). ...
Context 2
... wave amplitude maps (6.4), but with t n+1 → t n+1/2 and δθ → π + δθ /2. An example wave field is shown in figure 4(d). The stability analysis requires a two-stage transition map to account for the antiphase impacts. ...
Context 3
... µ ± ∈ C, we use Euler's formula to ensure a real solution, whose stability is analysed analogously to § 6.1. Example wave fields are given in figure 4(e,f ). We characterise this system with Λ(Γ ) ≡ δx(Γ )/ √ ˜ κ, where δx(Γ ) is the steady walking speed for˜κfor˜ for˜κ = 0. ...

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... All of these features are reminiscent of kink-antikink collisions and scattering [40,39,35], and Appendices A.1 and A.2 provide further conceptual links between the timecontinuous version of the proposed model (4) and the collective coordinate description of solitary wave interactions. In future work, it would also be of interest to determine whether more refined models of walkers, such as those in [41,42], also lead to single and multi-bounce behavior, bound states, and bounce windows with fractal structure. We expect that they would. ...
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