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Supersymmetric Duality Rotations
High Energy Physics - Theory · Submitted 11 Jan 2000
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We derive N = 1, 2 superfield equations as the conditions for a (nonlinear) theory of one abelian N = 1 or N = 2 vector multiplet to be duality invariant.
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The abstract, sentence by sentence
We derive N = 1, 2 superfield equations as the conditions for a (nonlinear) theory of one abelian N = 1 or N = 2 vector multiplet to be duality invariant. The N = 1 super Born-Infeld action is a particular solution of the corresponding equation. A family of duality invariant nonlinear N = 1 supersymmetric theories is described. We present the solution of the N = 2 duality equation which reduces to the N = 1 Born-Infeld action when the (0,1/2) part of N = 2 vector multiplet is switched off. We also propose a constructive perturbative scheme to compute duality invariant N = 2 superconformal actions.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We derive N = 1, 2 superfield equations as the conditions for a (nonlinear) theory of one abelian N = 1 or N = 2 vector multiplet to be duality invariant. | contribution 0.85 | 0.96 | 0.61 | asserted 1.00 |
| s1 | The N = 1 super Born-Infeld action is a particular solution of the corresponding equation. | result 0.95 | 0.70 | 0.15 | asserted 1.00 |
| s2 | A family of duality invariant nonlinear N = 1 supersymmetric theories is described. | contribution 0.56 | 0.91 | 0.28 | asserted 1.00 |
| s3 | We present the solution of the N = 2 duality equation which reduces to the N = 1 Born-Infeld action when the (0,1/2) part of N = 2 vector multiplet is switched off. | result 0.87 | 0.93 | 0.20 | asserted 1.00 |
| s4 | We also propose a constructive perturbative scheme to compute duality invariant N = 2 superconformal actions. | contribution 0.49 | 0.89 | 0.13 | asserted 0.51 |
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The paper
Original abstract
We derive N = 1, 2 superfield equations as the conditions for a (nonlinear) theory of one abelian N = 1 or N = 2 vector multiplet to be duality invariant. The N = 1 super Born-Infeld action is a particular solution of the corresponding equation. A family of duality invariant nonlinear N = 1 supersymmetric theories is described. We present the solution of the N = 2 duality equation which reduces to the N = 1 Born-Infeld action when the (0,1/2) part of N = 2 vector multiplet is switched off. We also propose a constructive perturbative scheme to compute duality invariant N = 2 superconformal actions.
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References
How the literature uses it
44 arXiv papers cite this in 148 sentences
Papers citing it · 104 sentences without a confident label
Builds on it 7 papers
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Finally, we give a new realization for the duality-invariant $=2$ supersymmetric theories presented in [ref] .
Duality rotations in supersymmetric nonlinear electrodynamics revisited · Duality rotations in $=2$ supersymmetric nonlinear electrodynamics · 0.93
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Here we consider a generalization of the $N=0$ and $N=1$ actions assuming—as in [ref] —dependence on the $=2$ superfields $^2$ and $^2$.
N=2 Supersymmetry and U(1)-Duality · $N=2$ SUSY, $U(1)$ duality, and derivative requirements · 0.93
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These $(1)$ duality invariant theories are curved-superspace extensions of the globally supersymmetric systems introduced in [ref] .
Superconformal vector multiplet self-couplings and generalised Fayet-Iliopoulos terms · Introduction · 0.98
Uses its method or tool 2 papers
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To study duality symmetries one has to use the Noether-Gaillard-Zumino type construction [ref] , which provides the conserved current for such symmetries and guaranties that the equations of motion are duality invariant.[The bona fide Noether current of the Lorentz non-covariant version of the theory developed in [ref] and the Hamiltonian approach in [ref] may be used for an alternative analysis of the UV properties of $N=8$ supergravity. ] In application to $N=8$ supergravity, the current of the classical theory was constructed explicitly in [ref] by embedding $E_7(7)$ into $Sp(2n,ℝ)$.
E{7(7)} Symmetry and Finiteness of N=8 Supergravity · Introduction · 0.93
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To verify duality invariance of the BI-like generalization of ModMax, it is convenient to use, following [ref] , the flat superspace counterparts of the variables [ref]: u:= 𝒟^2 W^2=-8(𝕊-ℙ) , u̅ := 𝒟̅^2 W̅^2=-8(𝕊+ℙ) .
ModMax meets Susy · Duality invariance · 0.99
Compares with it 6 papers
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In spite of this, the functional form of their self-duality equations, see [ref] for the vector multiplet and [ref] for the gravitino multiplet, agrees with that of [ref].[There have been a number of publications devoted to solutions of the self-duality equation for the $=2$ vector multiplet [ref] .] This leads us to believe that the latter is somewhat universal.
Self-duality for $\cal N$-extended superconformal gauge multiplets · Concluding comments · 0.82
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This agrees with the perturbative solution derived in [ref] .
Superconformal duality-invariant models and $\mathcal{N} = 4$ SYM effective action · Superconformal duality-invariant models in flat space · 0.97
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This equation is formally identical to the condition on the bosonic Lagrangian density required for duality invariance of its EL equations [ref] .
ModMax meets Susy · Duality invariance · 0.90
Cites it as background 18 papers
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Last but not least, an approach was developed in [ref] .
On the road to N=2 supersymmetric Born-Infeld action · Introduction · 0.95
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Within the GZGR approach or its supersymmetric extensions, a consistent nonlinear deformation of a given $(1)$ duality-invariant theory (say, Maxwell's theory) is typically derived in perturbation theory and requires an infinite number of terms for the deformed action to satisfy the self-duality equation [ref] or its supersymmetric extensions [ref] .
Higher-derivative deformations of the ModMax theory · Introduction · 0.89
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General duality-invariant supersymmetric theories with at most two derivatives at the component level were constructed in [ref] .
Superconformal duality-invariant models and $\mathcal{N} = 4$ SYM effective action · Formulation without auxiliary chiral variables · 0.89
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