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May 19 – 23, 2025
Jefferson Lab
US/Eastern timezone

All-Order Factorization for Virtual Compton Scattering at next-to-leading Power

May 19, 2025, 2:30 PM
30m
CEBAF Center, Auditoriium (Jefferson Lab)

CEBAF Center, Auditoriium

Jefferson Lab

12000 Jefferson Ave Newport News, VA 23606

Speaker

Jakob Schoenleber (Brookhaven National Laboratory)

Description

We discuss all-order factorization for the virtual Compton process at next-to-leading power (NLP) in the $\Lambda_{\rm QCD}/Q$ and $\sqrt{-t}/Q$ expansion (twist-3), both in the double-deeply-virtual case and the single-deeply-virtual case. We use the soft-collinear effective theory (SCET) as the main theoretical tool. We conclude that collinear factorization holds in the double-deeply virtual case, where both photons are far off-shell.
The agreement is found with the known results for the hard matching coefficients at leading order $\alpha_s^0$, and we can therefore connect the traditional approach with SCET. In the single-deeply-virtual case, commonly called deeply virtual Compton scattering (DVCS), the contribution of non-target collinear regions complicates the factorization. These include momentum modes collinear to the real photon and (ultra)soft interactions between the photon-collinear and target-collinear modes. However, such contributions appear only for the transversely polarized virtual photon at the NLP accuracy and in fact it is the only NLP $\sim (\Lambda_{\rm QCD}/Q)^1 \sim (\sqrt{-t}/Q)^1$ contribution in that case.
We therefore conclude that the DVCS amplitude for a longitudinally polarized virtual photon, where the leading power $\sim (\Lambda_{\rm QCD}/Q)^0 \sim (\sqrt{-t}/Q)^0$ contribution vanishes, is free of non-target collinear contributions and the collinear factorization in terms of twist-3 GPDs holds in that case as well.

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