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Multiparticle $\mathcal{N}{=}\,8$ mechanics with $F(4)$ superconformal symmetry
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abstract
We present a new multiparticle model of $\mathcal{N}{=}\,8$ mechanics with superconformal $F(4)$ symmetry. The system is constructed in terms of two matrix $\mathcal{N}{=}\,4$ multiplets. One of them is a bosonic matrix $({\bf 1, 4, 3})$ multiplet and another is a fermionic $({\bf 0, 4, 4})$ one. Off-diagonal bosonic components of the $({\bf 1, 4, 3})$ multiplet are chosen to take values in the flag manifold $\mathrm{U}(n)/[\mathrm{U}(1)]^n$ and they carry additional gauge symmetries. The explicit form of the $F(4)$ supersymmetry generators is found. We demonstrate that the $F(4)$ superalgebra constructed contains as subalgebras two different $D(2,1;\alpha\,{=}{-}1/3)$ superalgebras intersecting over the common $sl(2,\mathbb{R})\oplus su(2)$ subalgebra.
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Cited by 2 Pith papers
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Two faces of $N=7,8$ superconformal mechanics
Explicit supercharges and Hamiltonians for OSp(8|2), F(4), and G(3) superconformal mechanics are presented with two distinct R-symmetry realizations and octonionic embeddings of g2 into so(7).
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N=8 superconformal mechanics: direct construction
Explicit supercharges and Hamiltonians are constructed for all N=8 superconformal mechanics variants associated with osp(8|2), F(4), osp(4*|4), and su(1,1|4).
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