We discuss the existence of knot solitons (Hopfions) in a Skryme-Faddeev-Niemi-type model on the target space , which can be viewed as an effective theory of both the Yang-Mills theory and the anti-ferromagnetic Heisenberg model. We derive the knot solitons with two different types of ansatz: the first is a trivial embedding configuration of into , and the second is a non-embedding configuration that can be generated through the B"{a}cklund transformation. The resulting Euler-Lagrange equations for both ansatz reduce exactly to those of the Skyrme-Faddeev-Niemi model. We also examine some quantum aspects of the solutions using the collective coordinate zero-mode quantization method.

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