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The One-Loop Five-Graviton Amplitude and the Effective Action

David M. Richards

TL;DR

This work computes the one-loop five-graviton amplitude in type II string theory within the light-cone GS framework and expands it to reveal the low-energy effective action up to $D^6R^4$ terms. By subtracting contributions from known $D^{2n}R^4$ terms, it shows the absence of $R^5$ and $D^2R^5$ corrections and identifies the precise $D^4R^5$ structure required at this order, with coefficients matching the $D^6R^4$ sector. The analysis also uncovers the role of $\epsilon_{10}$ tensors, showing that $\epsilon_8\epsilon_8$ pieces combine with $t_8t_8$ in a $(t_8t_8\pm\tfrac18\epsilon_{10}\epsilon_{10})$ pattern, and discusses modular-function dependencies (e.g., $Z_{3/2}$ in IIB) and possible universal relations across orders and backgrounds. The results inform the construction of higher-derivative corrections in the string effective action and motivate conjectures about all-orders structures and tree-loop correspondences for five-graviton amplitudes in type II string theory.

Abstract

We consider the one-loop five-graviton amplitude in type II string theory calculated in the light-cone gauge. Although it is not possible to explicitly evaluate the integrals over the positions of the vertex operators, a low-energy expansion can be obtained, which can then be used to infer terms in the low-energy effective action. After subtracting diagrams due to known D^{2n}R^4 terms, we show the absence of one-loop R^5 and D^2R^5 terms and determine the exact structure of the one-loop D^4R^5 terms where, interestingly, the coefficient in front of the D^4R^5 terms is identical to the coefficient in front of the D^6R^4 term. Finally, we show that, up to D^6R^4 ~ D^4R^5, the ε_{10} terms package together with the t_8 terms in the usual combination (t_8t_8\pm{1/8}ε_{10}ε_{10}).

The One-Loop Five-Graviton Amplitude and the Effective Action

TL;DR

This work computes the one-loop five-graviton amplitude in type II string theory within the light-cone GS framework and expands it to reveal the low-energy effective action up to terms. By subtracting contributions from known terms, it shows the absence of and corrections and identifies the precise structure required at this order, with coefficients matching the sector. The analysis also uncovers the role of tensors, showing that pieces combine with in a pattern, and discusses modular-function dependencies (e.g., in IIB) and possible universal relations across orders and backgrounds. The results inform the construction of higher-derivative corrections in the string effective action and motivate conjectures about all-orders structures and tree-loop correspondences for five-graviton amplitudes in type II string theory.

Abstract

We consider the one-loop five-graviton amplitude in type II string theory calculated in the light-cone gauge. Although it is not possible to explicitly evaluate the integrals over the positions of the vertex operators, a low-energy expansion can be obtained, which can then be used to infer terms in the low-energy effective action. After subtracting diagrams due to known D^{2n}R^4 terms, we show the absence of one-loop R^5 and D^2R^5 terms and determine the exact structure of the one-loop D^4R^5 terms where, interestingly, the coefficient in front of the D^4R^5 terms is identical to the coefficient in front of the D^6R^4 term. Finally, we show that, up to D^6R^4 ~ D^4R^5, the ε_{10} terms package together with the t_8 terms in the usual combination (t_8t_8\pm{1/8}ε_{10}ε_{10}).

Paper Structure

This paper contains 38 sections, 165 equations, 3 figures.

Figures (3)

  • Figure 1: One of the fundamental domains of $SL(2,\mathbb{Z})$.
  • Figure 2: The origin of the massless poles in the five-graviton amplitude.
  • Figure 3: The two field theory diagrams contributing to the five-graviton amplitude: (a) a pole diagram and (b) a contact diagram.