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Nonperturbative corrections to 4D string theory effective actions from SL(2,Z) duality and supersymmetry

High Energy Physics - Theory · Submitted 4 Dec 2006

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The authors' main claim These combine with known perturbative and worldsheet instanton corrections into a single modular invariant function that determines the hypermultiplet low-energy effective acction.

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arXiv IDhep-th/0612027 (version 2)
Pith IDC2AUM7PX, Pith's permanent record of this paper and its review
CitationDaniel Robles-Llana, Frank Saueressig, Martin Rocek, Stefan Vandoren, Ulrich Theis. "Nonperturbative corrections to 4D string theory effective actions from SL(2,Z) duality and supersymmetry." arXiv:hep-th/0612027 (2006). https://pith.science/paper/C2AUM7PX
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We find the D(-1) and D1-brane instanton contributions to the hypermultiplet moduli space of type IIB string compactifications on Calabi-Yau threefolds. These combine with known perturbative and worldsheet instanton corrections into a single modular invariant function that determines the hypermultiplet low-energy effective acction.

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s0 We find the D(-1) and D1-brane instanton contributions to the hypermultiplet moduli space of type IIB string compactifications on Calabi-Yau threefolds. result 0.67 0.95 0.44 asserted 1.00
s1 These combine with known perturbative and worldsheet instanton corrections into a single modular invariant function that determines the hypermultiplet low-energy effective acction. result 0.92 0.69 0.63 asserted 1.00

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Original abstract

We find the D(-1) and D1-brane instanton contributions to the hypermultiplet moduli space of type IIB string compactifications on Calabi-Yau threefolds. These combine with known perturbative and worldsheet instanton corrections into a single modular invariant function that determines the hypermultiplet low-energy effective acction.

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60 arXiv papers cite this in 123 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 96 sentences without a confident label

Contests it 1 paper
Builds on it 2 papers
  • We start by reviewing and extending the results obtained in [ref] for the contribution of D1-D$(-1)$-instantons and A-type D2-brane instantons in Calabi-Yau compactifications of Type IIB and Type IIA strings, respectively.

    D-instantons and twistors · D-instanton corrections in Type II compactifications · 0.98

  • This invariance has been shown in the D1-D(-1) sector [ref] , extending the results of the earlier work [ref] , and our goal is to extend this construction to D3-D1-D(-1)-instantons.

    S-duality in Twistor Space · Twistorial description of $_H$ · 0.83

Uses its method or tool 7 papers
  • In order to obtain these solutions we will simply sum over images of the $α'$ corrections under the duality group following [ref] .

    Non-Perturbative Corrections and Modularity in N=1 Type IIB Compactifications · Introduction · 0.98

  • As explained in [ref] , the invariance under the discrete subgroup $SL(2,)$ can be restored by summing over images, using similar techniques as the ones used for $R^4$ couplings in toroidal compactifications [ref] .

    D-instantons and twistors · S-duality and A-type D-instanton corrections · 0.86

  • To that end, one may consider the initial expression for the corrections given by [ref] and, following [ref] , split it in two terms:

    Instanton Corrections and Emergent Strings · Instantons and Light Strings · 0.96

Compares with it 3 papers
  • Indeed, evaluating the integrals by residues, one can verify that [ref] coincides with the contact potential found in [ref] , while the quantum corrections [ref] reproduce the results in Eq. (5.2) [ref] up to δ_0^inst =∑_q_a ≥0 n_q_a^(0)∑_m,n' mδ_m,n, δσ^inst =-∑_q_a ≥0 n_q_a^(0)∑_m,n' (mτ_1+2n)δ_m,n,

    S-duality in Twistor Space · The quantum mirror map revisited · 0.98

  • In order to do so, it is convenient to notice that the above structures clearly reproduce the type IIB result in [ref] , which we review here for completeness.

    Non-perturbative effects and wall-crossing from topological strings · The type IIB instanton interpretation · 0.90

  • By just looking at the zero mode counting, we do not expect similar corrections to the 1/2-BPS fundamental, $E1$ and $E3$ instanton corrections to the $N=2$ hypermultiplet moduli space as recently discussed for instance in [ref] .

    Power Towers of String Instantons for N=1 Vacua · Remarks · 0.92

Cites it as background 14 papers
  • Although these results have been obtained by following the path presented in Fig. [ref][The first step up towards non-perturbative contributions has been done in [ref] , mirror symmetry has been applied in [ref] , then all D-brane instantons have been included in [ref] , and one-instanton contributions due to NS5-branes have been found in [ref] .], we will not repeat it in detail.

    Twistor Approach to String Compactifications: a Review · Where we are · 0.91

  • In this case the low energy effective action is known to be described by the metric on the vector multiplet (VM) and hypermultiplet (HM) moduli spaces, $$ and $$, and the latter is known to be [ref] and to carry an isometric action of $SL(2,)$ [ref] .

    Modularity, Quaternion-Kahler spaces and Mirror Symmetry · Introduction · 0.84

  • In the case of D2-brane instanton, these effects have been computed via duality in [ref] and are by now well-understood.[In the context of the distance conjecture [ref] , these kind of instantons have been analyzed in the mirror dual Type IIB setup in [ref] , where it was shown that they obstruct certain classical infinite distance limits which otherwise violate the emergent string conjecture [ref] ; see also [ref] for a similar study in M-theory compactifications on Calabi–Yau threefolds.] For our purpose, the relevant corrections originate from the 5-brane instantons, whose computation is more involved.

    Non-perturbative Resolution of Strong Coupling Singularities in 4d N=1 Heterotic/M-theory · Introduction · 0.81

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