Soft spectator scattering in the nucleon form factors at large $Q^2$ within the SCET approach

Abstract

The proton form factors at large momentum transfer are dominated by two contributions which are associated with the hard and soft rescattering respectively. Motivated by a very active experimental form factor program at intermediate values of momentum transfers, $Q^2\sim 5-15{\text{GeV}}^2$, where an understanding in terms of only a hard rescattering mechanism cannot yet be expected, we investigate in this work the soft rescattering contribution using soft collinear effective theory (SCET). Within such description, the form factor is characterized, besides the hard scale $Q^2$, by a semi-hard scale $Q\Lambda$, which arises due to presence of soft spectators, with virtuality ${\Lambda }^2$ ($\Lambda \sim 0.5$ GeV), such that $Q^2\gg Q\Lambda \gg {\Lambda }^2$. We show that in this case a two-step factorization can be successfully carried out using the SCET approach. In a first step (SCET${}_I$), we perform the leading order matching of the QCD electromagnetic current onto the relevant SCET${}_I$ operators and perform a resummation of large logarithms using renormalization group equations. We then discuss the further matching onto a SCET${}_{II}$ framework, and propose the complete factorization formula for the Dirac form factor, accounting for both hard and soft contributions. We also present a qualitative discussion of the phenomenological consequences of this new framework.

33 pages, 19 figures; typos corrected, text improved. Version to appear in Phys.Rev.D

References in corpus (7)

• Nucleon Electromagnetic Form Factors
• Recoil Polarization Measurements of the Proton Electromagnetic Form Factor Ratio to Q^2 = 8.5 GeV^2
• Dynamical Threshold Enhancement and Resummation in Drell-Yan Production
• Nucleon electromagnetic form factors
• Nucleon Form Factors in QCD
• Origin of the Large Perturbative Corrections to Higgs Production at Hadron Colliders
• Endpoint behavior of high-energy scattering cross sections

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