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.
Therefore, virtual monopoles within the topological vector potential of vector DHBS can admit charges of ±1/2,±3/2, and±5/2, though not all necessarily simul- taneously
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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.