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Two-photon exchange corrections to $γ^*NΔ$ form factors for $Q^2\leq 4 $ (Gev/$c$)$^2$

Published 12 Apr 2017 in nucl-th, hep-ph, and nucl-ex | (1704.03605v4)

Abstract: We evaluate the corrections of the two-photon exchange (TPE) process on the $\gamma* N\Delta$ transition form factors. The contributions of the TPE process to the $eN\rightarrow e\Delta(1232)\rightarrow eN\pi$ are calculated in a hadronic model with the inclusion of only the elastic nucleon intermediate states, to estimate its effects on the multipoles $M{(3/2)}_{1+}, E{(3/2)}_{1+}, S{(3/2)}_{1+}$ at the $\Delta$ peak. We find that TPE effects on $G*_M$ is very small. $G*_E,$ and $ G*_C$ are also little affected at small $Q2 $. For $G*_E$, the TPE effects reach about $3 - 8\%$ near $Q2\sim 4$ GeV$2$, depending on the model, MAID or SAID, used to emulate the data. For $G*_C$, the TPE effects decrease rapidly with increasing $\epsilon$ while growing with increasing $Q2$ to reach $\sim 6 - 15\%$ with $Q2 \sim 4$ GeV$2$ at $\epsilon = 0.2$. Sizeable TPE corrections to $G*_E$ and $G*_C$ found here points to the need of including TPE effects in the multipole analysis in the region of high $Q2$ and small $\epsilon$. The TPE corrections to $R_{EM}$ and $R_{SM}$ obtained in our hadronic calculation are compared with those obtained in a partonic calculation for moderate momentum transfer of $2<Q2<4$ GeV$2$.

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