We solve the Gardner deformation problem for the N =2 supersymmetric a=4 Korteweg-de Vries equation (P. Mathieu, 1988). We show that a known zerocurvature representation for this superequation yields the system of new nonlocal variables such that their derivatives contain the Gardner deformation for the classical KdV equation.
Introduction. The classical problem of construction of the Gardner deformation [1]for an infinite-dimensional completely integrable system of evolutionary partial differential equations essentially amounts to finding a recurrence relation between the integrals of motion. For the N=2 supersymmetric generalizations of the Korteweg-de Vries equation [2,3], the deformation problem was posed when the integrable triplet of such super-systems was discovered. Various attempts to solve it were undertaken since then (e.g., see [2]) but the progress was limited. The first solution for the N=2, a=4 SKdV in the triplet a ∈ {−2, 1, 4} was achieved in [4]; in that paper, we stated the 'no-go' theorem about the impossibility to deform this super-equation in terms of the superfield (but not the impossibility to deform it by treating the components of the super-field separately, see below), c.f. [2]. We then presented the two-step solution of the deformation problem: We obtained the Gardner deformation for the Kaup-Boussinesq equation, which is the bosonic limit of the super-equation that precedes the N=2, a=4 super-KdV in its hierarchy. We thus derived the recurrence relation between the Hamiltonians of the bosonic limit hierarchy and then we showed how each conserved density is extended to the super-density for the N=2 super-system. In other words, we deformed the bosonic subsystem of the super-equation at hand within the frames of the classical scheme [1], whence we recovered the full N=2 supersymmetry-invariance.In this paper we re-address, from a principally different viewpoint, the Gardner deformation problem for a vast class of (not necessarily supersymmetric) KdV-like systems. Namely, in [4] we emphasized the geometric likeness of the Gardner deformations and zero-curvature representations, each of them manifesting the integrability of nonlinear systems. Indeed, both constructions generate infinite sequences of nontrivial integrals