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Contact interactions in D-brane models

I. Antoniadis, K. Benakli, A. Laugier

TL;DR

This work analyzes tree-level four-fermion amplitudes in Type I D-brane models where matter resides at brane intersections (notably D3/D7 setups), showing that massless exchanges mix KK modes, winding states, and string oscillator excitations to generate dimension-six contact operators. Compared to the DD-string case, ND configurations produce dominant dimension-six contributions, with oscillator exchanges providing the leading coefficients (approximately 0.59) and volume/Wilson-line effects producing exponential suppressions and phase factors. By subtracting massless exchanges, the authors derive effective four-fermion operators and quantify their dependence on internal radii, brane separations, and the number of brane sets, yielding model-independent bounds on the string scale $M_s$ from LEP and low-energy data (roughly 2–3 TeV, depending on the setup). The study highlights the distinct phenomenology of brane intersections, including enhanced sensitivity to geometric data (radii, separations) and a framework for translating stringy contact interactions into experimental limits relevant for TeV-scale string scenarios.

Abstract

We compute the tree-level four-point scattering amplitudes in string models where matter fields live on D-brane intersections. Extracting the contribution of massless modes, we are left with dimension-six four-fermion operators which in general receive contributions from three different sources: exchange of massive Kaluza--Klein excitations, winding modes and string oscillator states. We compute their coefficients and extract new bounds on the string scale in the brane-world scenario. This is contrasted with the situation where matter fields arise from open strings with both ends confined on the same collection of D-branes, in which case the exchange of massive string modes leads to dimension-eight operators that have been studied in the past. When matter fields live on brane intersections, the presence of dimension-six operators increases the lower bound on the string scale to 2--3 TeV, independently of the number of large extra dimensions.

Contact interactions in D-brane models

TL;DR

This work analyzes tree-level four-fermion amplitudes in Type I D-brane models where matter resides at brane intersections (notably D3/D7 setups), showing that massless exchanges mix KK modes, winding states, and string oscillator excitations to generate dimension-six contact operators. Compared to the DD-string case, ND configurations produce dominant dimension-six contributions, with oscillator exchanges providing the leading coefficients (approximately 0.59) and volume/Wilson-line effects producing exponential suppressions and phase factors. By subtracting massless exchanges, the authors derive effective four-fermion operators and quantify their dependence on internal radii, brane separations, and the number of brane sets, yielding model-independent bounds on the string scale from LEP and low-energy data (roughly 2–3 TeV, depending on the setup). The study highlights the distinct phenomenology of brane intersections, including enhanced sensitivity to geometric data (radii, separations) and a framework for translating stringy contact interactions into experimental limits relevant for TeV-scale string scenarios.

Abstract

We compute the tree-level four-point scattering amplitudes in string models where matter fields live on D-brane intersections. Extracting the contribution of massless modes, we are left with dimension-six four-fermion operators which in general receive contributions from three different sources: exchange of massive Kaluza--Klein excitations, winding modes and string oscillator states. We compute their coefficients and extract new bounds on the string scale in the brane-world scenario. This is contrasted with the situation where matter fields arise from open strings with both ends confined on the same collection of D-branes, in which case the exchange of massive string modes leads to dimension-eight operators that have been studied in the past. When matter fields live on brane intersections, the presence of dimension-six operators increases the lower bound on the string scale to 2--3 TeV, independently of the number of large extra dimensions.

Paper Structure

This paper contains 14 sections, 55 equations, 1 figure, 1 table.

Figures (1)

  • Figure 1: Radius dependence of the four-fermion contact terms for two (solid line) and three (dashed line) sets of branes.