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Related papers: One-dimensional sigma-models with N=5,6,7,8 off-sh…

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We construct the non-minimal linear representations of the N=4 Extended Supersymmetry in one-dimension. They act on 8 bosonic and 8 fermionic fields. Inequivalent representations are specified by the mass-dimension of the fields and the…

High Energy Physics - Theory · Physics 2011-07-26 Marcelo Gonzales , Sadi Khodaee , Francesco Toppan

Off-shell $(4,0)$ supermultiplets in 2-dimensions are formulated. These are used to construct sigma models whose target spaces are vector bundles over manifolds that are hyperk\"ahler with torsion. The off-shell supersymmetry implies that…

High Energy Physics - Theory · Physics 2017-09-13 Chris Hull , Ulf Lindström

Using an N=4, d=1 superfield approach, we construct an N=8 supersymmetric action of the self-interacting off-shell N=8 multiplet {\bf (1, 8, 7)}. This action is found to be invariant under the exceptional N=8, d=1 superconformal group F(4)…

High Energy Physics - Theory · Physics 2008-11-26 F. Delduc , E. Ivanov

The complete classification of the irreducible representations of the N-extended one-dimensional supersymmetry algebra linearly realized on a finite number of fields is presented. Off-shell invariant actions of one-dimensional…

High Energy Physics - Theory · Physics 2008-11-26 Francesco Toppan

The ${\cal N}{=}8, 1D$ analytic bi-harmonic superspace is shown to provide a natural setting for ${\cal N}{=}8$ supersymmetric mechanics associated with the off-shell multiplet ${\bf (4, 8, 4)}$ . The latter is described by an analytic…

High Energy Physics - Theory · Physics 2010-11-05 S. Bellucci , E. Ivanov , A. Sutulin

Off-shell $(4,q)$ supermultiplets in 2-dimensions are constructed for $q=1,2,4$. These are used to construct sigma models whose target spaces are hyperk\"ahler with torsion. The off-shell supersymmetry implies the three complex structures…

High Energy Physics - Theory · Physics 2017-04-05 Chris Hull , Ulf Lindström

Proceeding from nonlinear realizations of the most general N=4, d=1 superconformal symmetry associated with the supergroup D(2,1;\alpha), we construct all known and two new off-shell N=4, d=1 supermultiplets as properly constrained N=4…

High Energy Physics - Theory · Physics 2009-11-10 Evgeny Ivanov , Sergey Krivonos , Olaf Lechtenfeld

We define two new indecomposable (not fully reducible) ${\cal N}=8$, $d=1$ off-shell multiplets and consider the corresponding models of ${\cal N}=8$ supersymmetric mechanics with spin variables. Each multiplet is described off shell by a…

High Energy Physics - Theory · Physics 2026-01-22 Evgeny Ivanov , Stepan Sidorov

We construct new models of `curved' SU$(4|1)$ supersymmetric mechanics based on two versions of the off-shell multiplet ${\bf(8,8,0)}$ which are `mirror' to each other. The worldline realizations of the supergroup SU$(4|1)$ are treated as a…

High Energy Physics - Theory · Physics 2018-09-26 Evgeny Ivanov , Olaf Lechtenfeld , Stepan Sidorov

Sigma models describing low energy effective actions on D0-brane probes with N=8 supercharges are studied in detail using a manifestly d=1, N=4 super-space formalism. Two 0+1 dimensional N=4 multiplets together with their general actions…

High Energy Physics - Theory · Physics 2016-08-25 Duiliu-Emanuel Diaconescu , Rami Entin

Exploiting the gauging procedure developed by us in hep-th/0605211, we study the relationships between the models of N=4 mechanics based on the off-shell multiplets (4,4,0) and (1,4,3). We make use of the off-shell N=4, d=1 harmonic…

High Energy Physics - Theory · Physics 2008-11-26 F. Delduc , E. Ivanov

We construct a new off-shell $\mathcal{N}{=}8$, $d{=}1$ nonlinear supermultiplet $(\mathbf{4,8,4})$ proceeding from the nonlinear realization of the $\mathcal{N}{=}8$, $d{=}1$ superconformal group $OSp(4^{\star}|4)$ in its supercoset…

High Energy Physics - Theory · Physics 2008-11-26 S. Bellucci , S. Krivonos , A. Marrani

We construct manifestly ${\cal N}=4$ supersymmetric off-shell superfield actions for the HKT $d=1$ sigma models on the group manifolds U(2) and SU(3), using the harmonic $d=1$ approach. The underlying $({\bf 4, 4, 0})$ and $({\bf 4, 4,…

High Energy Physics - Theory · Physics 2021-01-01 F. Delduc , E. Ivanov

We construct a variety of off-shell $N{=}8, d{=}1$ supermultiplets with finite numbers of component fields as direct sums of properly constrained $N{=}4, d{=}1$ superfields. We also show how these multiplets can be described in $N{=}8,…

High Energy Physics - Theory · Physics 2009-11-10 S. Bellucci , E. Ivanov , S. Krivonos , O. Lechtenfeld

For two families of four-dimensional off-shell N = 2 supersymmetric nonlinear sigma-models constructed originally in projective superspace, we develop their formulation in terms of N = 1 chiral superfields. Specifically, these theories are:…

High Energy Physics - Theory · Physics 2015-05-14 Sergei M. Kuzenko

We develop superspace techniques to construct general off-shell N=1,2,3,4 superconformal sigma-models in three space-time dimensions. The most general N=3 and N=4 superconformal sigma-models are constructed in terms of N=2 chiral…

High Energy Physics - Theory · Physics 2011-02-01 Sergei M. Kuzenko , Jeong-Hyuck Park , Gabriele Tartaglino-Mazzucchelli , Rikard von Unge

We define basics of $(4,4)\;\; 2D$ harmonic superspace with two independent sets of $SU(2)$ harmonic variables and apply it to construct new superfield actions of $(4,4)$ supersymmetric two-dimensional sigma models with torsion and mutually…

High Energy Physics - Theory · Physics 2009-10-28 E. Ivanov , A. Sutulin

We use world-line methods for pseudo-supersymmetry to construct $sl(2|1)$-invariant actions for the $(2,2,0)$ chiral and ($1,2,1)$ real supermultiplets of the twisted $D$-module representations of the $sl(2|1)$ superalgebra. The derived…

High Energy Physics - Theory · Physics 2016-02-16 L. Baulieu , N. L. Holanda , F. Toppan

We present new explicit realizations of the most general N=4, d=1 superconformal symmetry D(2,1;\alpha) in the models of N=4 superconformal mechanics based on the reducible multiplets (1,4,3)\oplus(0,4,4), (3,4,1)\oplus(0,4,4) and…

High Energy Physics - Theory · Physics 2015-10-21 S. Fedoruk , E. Ivanov

We construct new models of N=8 superconformal mechanics associated with the off-shell N=8, d=1 supermultiplets (3,8,5) and (5,8,3). These two multiplets are derived as N=8 Goldstone superfields and correspond to nonlinear realizations of…

High Energy Physics - Theory · Physics 2011-07-28 S. Bellucci , E. Ivanov , S. Krivonos , O. Lechtenfeld
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