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We investigate the reduction of generalized K-symmetries and $τ$-symmetries on the multisoliton manifolds of the potential BKP and CKP hierarchies. The n-soliton solution of BKP depends on wave-number parameters kₘ, transverse parameters lₘ, and phase parameters ξₘ₀, defining a $3n$-dimensional manifold. Its restricted K-symmetries project onto an n-dimensional phase-shift subspace, while the restricted $τ$-symmetries engage the full $3n$-dimensional tangent space. This structure naturally yields a row-replacement determinant representation. In contrast, the n-soliton solution of CKP has no independent transverse parameters, reducing the manifold dimension to $2n$. The restricted K-symmetries again form an n-dimensional phase-shift representation, but the $τ$-symmetries now involve only $2n$ tangent directions. For CKP, the natural formulation treats elementary tangent symmetries as unknowns, producing a column-replacement determinant representation via Cramer's rule. The difference between these two determinant structures reflects not a difference in the underlying linear algebra, but rather the distinct parameterizations of the two soliton manifolds. Both formulas express explicitly how infinite-dimensional symmetry hierarchies collapse onto finite-dimensional multisoliton families.
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Hao et al. (2026) studied this question.
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