The movies show the absolute values of the colliding compactons observed from the top (unless mentioned otherwise). Collision time in the manuscript is shifted, if initially the compactons were located too far apart.
Energy (E) and charge (Q) frequency (ω) relation. Insert: sublinear E(Q) relation -- below the reference (Ref.) line
Fig. 4 -- ><: δ=1/3, a=b=1, σ=0, λ1=λ2=0.4, ω1γ1=ω2γ2=2 (corresponding to II in 3D)
><: δ=1/3, a=1, b=1, σ=0, λ1=0.5, ω1=2, λ2=0.75, ω2=3
/\: δ=1/3, a=1, b=1, σ=0, λ1=0.5, ω1=2, λ2=0.75, ω2=3
><: δ=1/3, a=1, b=1, σ=0, λ1=0.94, ω1=4, λ2=0.97, ω2=4.4
Fig. 6 -- ><: δ=1/3, a=b=1, σ=0, λ1=0.97, ω1γ1=10, λ2=0.94, ω2γ2=8 (corresponding to I in 3D)
+><+: δ=0, a=1, b=1, σ=1.6, λ1=λ2=0.4, ω1γ1=ω2γ2=2 (flatons)
+><-: δ=0, a=1, b=1, σ=1.6, λ1=λ2=0.4, ω1γ1=-ω2γ2=2 (flatons)
Fig. 5 (right) -- +><+: δ=1/3, a=1, b=1, σ=1.6, λ1=λ2=0.4, ω1γ1=ω2γ2=2 (flatons)
Fig. 5 (left) -- +><-: δ=1/3, a=1, b=1, σ=1.6, λ1=λ2=0.4, ω1γ1=-ω2γ2=2
+><+: δ=1/3, a=1, b=1, σ=1, λ1=λ2=0.94, ω1γ1=ω2γ2=2 (flatons)
+><+: δ=5/7, a=1, b=1, σ=1.6, λ1=λ2=0.4, ω1γ1=ω2γ2=2 (flatons)
Fig. 7 -- ><: δ=1/3, a=b=1, σ=0, n1=3, λ1=0.94, ω1γ1=10, n2=1, λ2=0.91, ω2γ2=7
><: δ=1/3, a=b=1, σ=0, n1=3, λ1=0.94, ω1γ1=10, n2=3, λ2=0.91, ω2γ2=8