Results 111 to 120 of about 3,150,705 (223)

Goldstino superfields in N = 2 $$ \mathcal{N}=2 $$ supergravity

open access: yesJournal of High Energy Physics, 2017
We present off-shell N = 2 $$ \mathcal{N}=2 $$ supergravity actions, which exhibit spontaneously broken local supersymmetry and allow for de Sitter vacua for certain values of the parameters. They are obtained by coupling the standard N = 2 $$ \mathcal{N}
Sergei M. Kuzenko   +2 more
doaj   +1 more source

Constraints from extended supersymmetry in quantum mechanics

open access: yesNuclear Physics B, 1998
22 pages ...
Mark Stern, Sonia Paban, Savdeep Sethi
openaire   +3 more sources

On quantum compatibility of counterterm deformations and duality symmetries in N≥5 $$ \mathcal{N}\ge 5 $$ supergravities

open access: yesJournal of High Energy Physics, 2018
In N=5 $$ \mathcal{N}=5 $$, 6, 8 supergravities there are hidden symmetries of equations of motion, described by duality groups SU(1, 5), SO*(12), E 7(7) respectively.
Renata Kallosh   +3 more
doaj   +1 more source

The action with manifest E7 type symmetry

open access: yesJournal of High Energy Physics, 2019
We generalize Cremmer-Julia 1st order action of N = 8 $$ \mathcal{N}=8 $$ supergravity with manifest E 7(7) symmetry to cases of N = 6 $$ \mathcal{N}=6 $$ with manifest SO∗(12) and N = 5 $$ \mathcal{N}=5 $$ with manifest SU(1, 5) duality symmetries ...
Renata Kallosh
doaj   +1 more source

New Fayet-Iliopoulos terms in N = 2 $$ \mathcal{N}=2 $$ supergravity

open access: yesJournal of High Energy Physics, 2019
We present a new type of Fayet-Iliopoulos (FI) terms in N = 2 $$ \mathcal{N}=2 $$ supergravity that do not require the gauging of the R-symmetry. We elaborate on the impact of such terms on the vacuum structure of the N = 2 $$ \mathcal{N}=2 $$ theory and
Ignatios Antoniadis   +3 more
doaj   +1 more source

Reflection groups and 3d N $$ \mathcal{N} $$ > 6 SCFTs

open access: yesJournal of High Energy Physics, 2019
We point out that the moduli spaces of all known 3d N $$ \mathcal{N} $$ = 8 and N $$ \mathcal{N} $$ = 6 SCFTs, after suitable gaugings of finite symmetry groups, have the form ℂ 4r /Γ where Γ is a real or complex reflection group depending on whether the
Yuji Tachikawa, Gabi Zafrir
doaj   +1 more source

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