Abstract

We introduce a new kind of non-relativistic N= 8{\cal N}{=}\,8 supersymmetric mechanics, associated with worldline realizations of the supergroup SU(2∣2)SU(2|2) treated as a deformation of flat N= 8{\cal N}{=}\,8, d=1d{=}1 supersymmetry. Various worldline SU(2∣2)SU(2|2) superspaces are constructed as coset manifolds of this supergroup, and the corresponding superfield techniques are developed. For the off-shell SU(2∣2)SU(2|2) multiplets (3,8,5)({\bf 3,8,5}), (4,8,4)({\bf 4,8,4}) and (5,8,3)({\bf 5,8,3}), we construct and analyze the most general superfield and component actions. Common features are mass oscillator-type terms proportional to the deformation parameter and a trigonometric realization of the superconformal group OSp(4∗∣4)OSp(4^*|4) in the conformal cases. For the simplest (5,8,3)({\bf 5, 8, 3}) model the quantization is performed.

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