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We propose a manifestly U-duality invariant modular form for the D^6 R^4 interaction in the effective action of type IIB string theory compactified on T^2. It receives perturbative contributions upto genus three, as well as non-perturbative…

High Energy Physics - Theory · Physics 2008-11-26 Anirban Basu

The modular invariant coefficient of the D^{2k} {\cal{R}}^4 term in the effective action of type IIB superstring theory is expected to satisfy Poisson equation on the fundamental domain of SL(2,Z). Under certain assumptions, we obtain the…

High Energy Physics - Theory · Physics 2008-11-26 Anirban Basu

Four-graviton couplings in the low energy effective action of type II string vacua compactified on tori are strongly constrained by supersymmetry and U-duality. While the $R^4$ and $D^4 R^4$ couplings are known exactly in terms of…

High Energy Physics - Theory · Physics 2015-06-23 Boris Pioline

The R^4 terms in the effective action for M-theory compactified on a two-torus are motivated by combining one-loop results in type II superstring theories with the Sl(2,Z) duality symmetry. The conjectured expression reproduces precisely…

High Energy Physics - Theory · Physics 2010-11-19 Michael B. Green , Pierre Vanhove

We obtain the exact non-perturbative thresholds of $R^4$ terms in IIB string theory compactified to eight and seven dimensions. These thresholds are given by the perturbative tree-level and one-loop results together with the contribution of…

High Energy Physics - Theory · Physics 2010-04-06 Elias Kiritsis , Boris Pioline

Dualities of M-theory are used to determine the exact dependence on the coupling constant of the D^6R^4 interaction of the IIA and IIB superstring effective action. Upon lifting to eleven dimensions this determines the coefficient of the…

High Energy Physics - Theory · Physics 2009-11-11 Michael B. Green , Pierre Vanhove

We demonstrate how duality invariance of the low energy expansion of the four-graviton amplitude in type II string theory determines the precise coefficients of multiloop logarithmic ultraviolet divergences of maximal supergravity in…

High Energy Physics - Theory · Physics 2013-10-25 Michael B. Green , Jorge G. Russo , Pierre Vanhove

The low-momentum expansion of the two-loop four-graviton scattering amplitude in eleven-dimensional supergravity compactified on a circle and a two-torus is considered up to terms of order S^6R^4 (where S is a Mandelstam invariant and R is…

High Energy Physics - Theory · Physics 2009-11-13 Michael B. Green , Jorge G. Russo , Pierre Vanhove

Scattering of fundamental states of type IIB supergravity and superstring theory is discussed at low orders in perturbation theory in the background of a D-instanton. The integration over fermionic zero modes in both the low energy…

High Energy Physics - Theory · Physics 2009-10-30 Michael B. Green , Michael Gutperle

The two-loop Feynman diagram contribution to the four-graviton amplitude of eleven-dimensional supergravity compactified on a two-torus, T^2, is analyzed in detail. The Schwinger parameter integrations are re-expressed as integration over…

High Energy Physics - Theory · Physics 2008-11-26 Michael B. Green , Hwang-h. Kwon , Pierre Vanhove

In this note we study the U-duality invariant coefficient functions of higher curvature corrections to the four-graviton scattering amplitude in type IIB string theory compactified on a torus. The main focus is on the $D^6R^4$ term that is…

High Energy Physics - Theory · Physics 2018-07-04 Olof Ahlén , Axel Kleinschmidt

We consider the perturbative contributions to the R^4, D^4 R^4 and D^6 R^4 interactions in toroidally compactified type II string theory. These BPS interactions do not receive perturbative contributions beyond genus three. We derive Poisson…

High Energy Physics - Theory · Physics 2016-01-27 Anirban Basu

Invariance of Type IIB superstring theory under SL(2,Z) or S-duality implies dependence on the complex coupling T through real and complex modular forms in T. Their structure may be understood explicitly in an expansion of superstring…

High Energy Physics - Theory · Physics 2022-01-20 Eric D'Hoker , Michael B. Green

We address the issue of T-duality and U-duality symmetries in the toroidally-compactified type IIA string. It is customary to take as a starting point the dimensionally-reduced maximal supergravity theories, with certain field strengths…

High Energy Physics - Theory · Physics 2009-10-07 H. Lu , C. N. Pope

We consider a conformal system of a string and a particle defined in D=10+2 space-time dimensions. The extra time-like dimension is a gauge artifact and can be eliminated by choosing a gauge in which the SO(10,1) Lorentz symmetry is…

High Energy Physics - Theory · Physics 2007-05-23 Costas Kounnas

Four-graviton, eight-derivative couplings in the low energy effective action of toroidal type II string compactifications are tightly constrained by U-duality invariance and by supersymmetry. In this note, we revisit earlier proposals for…

High Energy Physics - Theory · Physics 2014-06-23 Boris Pioline

It has been shown recently that the toroidally compactified type IIB string effective action possesses an SL(2, R) invariance as a consequence of the corresponding symmetry in ten dimensions when the self-dual five-form field strength is…

High Energy Physics - Theory · Physics 2010-11-19 Shibaji Roy

Based on the structure of the on-shell linearized superspace of type IIB supergravity, we argue that there is a non--BPS 16 derivative interaction in the effective action of type IIB string theory of the form (t_8 t_8 R^4)^2, which we call…

High Energy Physics - Theory · Physics 2015-06-16 Anirban Basu

The effective action for type II string theory compactified on a six torus is $N=8$ supergravity, which is known to have an $E_{7}$ duality symmetry. We show that this is broken by quantum effects to a discrete subgroup, $E_7(\Z)$, which…

High Energy Physics - Theory · Physics 2009-07-09 C. M. Hull , P. K. Townsend

The $D^4\mathcal{R}^4$ and $D^6\mathcal{R}^4$ coefficient functions in the effective action of type II string theory compactified on $T^d$ contain terms of the form $\mathcal{E}_1 {\rm ln}g_d$ and $\mathcal{E}_2 ({\rm ln}g_d)^2$ in specific…

High Energy Physics - Theory · Physics 2016-07-06 Anirban Basu
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