2008
DOI: 10.1088/1126-6708/2008/09/081
|View full text |Cite
|
Sign up to set email alerts
|

Recursion relations from space-time supersymmetry

Abstract: We describe a method for obtaining relations between higher derivative interactions in supersymmetric effective actions. The method extends to all orders in the momentum expansion. As an application, we consider the string coupling dependence of theĜ 2k λ 16 interaction in type IIB string theory. Using supersymmetry, we show that each of these interactions satisfies a Poisson equation on the moduli space with sources determined by lower momentum interactions. We argue that these protected couplings are only re… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

2
111
0

Year Published

2010
2010
2020
2020

Publication Types

Select...
7

Relationship

2
5

Authors

Journals

citations
Cited by 33 publications
(113 citation statements)
references
References 44 publications
2
111
0
Order By: Relevance
“…Next, we use the fact that upon acting on functions depending only on the GL(2)/U (1) factor parametrised by U = U 1 + iU 2 ∈ H 1 and y d , the Laplacian on E d+1 reduces to to [1, (4.65)] 11 The normalisation of the character is defined such that the action of the Cartan torus element on the lowest weight representation Λ k is normalised to y k . In other words, we write the torus element as exp(− i log(yi)hi), where the hi are the canonical Chevalley generators that need to be evaluated in the lowest weight representation.…”
Section: Laplace Identitiesmentioning
confidence: 99%
“…Next, we use the fact that upon acting on functions depending only on the GL(2)/U (1) factor parametrised by U = U 1 + iU 2 ∈ H 1 and y d , the Laplacian on E d+1 reduces to to [1, (4.65)] 11 The normalisation of the character is defined such that the action of the Cartan torus element on the lowest weight representation Λ k is normalised to y k . In other words, we write the torus element as exp(− i log(yi)hi), where the hi are the canonical Chevalley generators that need to be evaluated in the lowest weight representation.…”
Section: Laplace Identitiesmentioning
confidence: 99%
“…The general form of self-dual field strength is 11) and that of anti-self-dual field strength is 12) where h AB and h AB are symmetric tensors in A and B. Although H sf and H asf is not manifestly antisymmetric in the pairs of indices {A i }, {B i }, {C i }, one can show the explicitly antisymmetric property by the identities 13) and 14) where the notation of antisymmetrization in indicies is defined as where we have specified the SU(4) R-symmetry indices.…”
Section: Jhep09(2015)098mentioning
confidence: 99%
“…Furthermore, for N = 4 quantum mechanics, one can show that the coefficient of six-derivative terms are completely determined by that of four derivatives [5]. Supersymmetry has also been extensively used to study higher derivative terms in the effective actions of maximal supersymmetric gravity theories with many interesting exact results have been obtained [6][7][8][9][10][11][12].…”
Section: Introduction and Motivationsmentioning
confidence: 99%
“…This leads to Poisson equations on moduli space, where the source terms are given by couplings at lower orders in the α ′ expansion. These source terms that arise from the supervariation of the form δ (p) S (q) are at least quadratic in the couplings, where one factor arises from the coupling in S (q) while the other factor arises from the coupling in the corrected supersymmetry transformation δ (p) whose form is dictated by the closure of the supersymmetry algebra [7] 8 and involves an appropriate coupling in S (p) . For the D 6 R 4 interaction, this leads to the perturbative contributions [20]…”
Section: Supersymmetry and S-duality Constraints On Transcendentalitymentioning
confidence: 99%