Poles of the density function in nonlinear waves form virtual Dirac monopoles with quantized charges ±3/2 and ±5/2, in contrast to the ±1/2 charges previously associated with simple zeros.
Two mergers result in a time interval during which the phase shift ∆ϕ= 2π
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Dirac monopole potentials with high charges underlying nonlinear waves
Poles of the density function in nonlinear waves form virtual Dirac monopoles with quantized charges ±3/2 and ±5/2, in contrast to the ±1/2 charges previously associated with simple zeros.