QCD and QED dynamics of the EMC effect
Leonid Frankfurt, Mark Strikman

TL;DR
This paper uses QCD sum rules to analyze the EMC effect, revealing non-nucleonic degrees of freedom, the role of photon contributions, and the impact of short-range correlations on nuclear structure functions.
Contribution
It introduces a QCD-based framework to understand the EMC effect, emphasizing non-nucleonic components and photon contributions, and challenges existing models for x>0.6.
Findings
Non-nucleonic degrees of freedom cause deviations in the EMC ratio.
Photon contributions from Lorentz-transformed Coulomb fields are significant.
Short-range correlations influence the EMC effect at high x.
Abstract
Applying exact QCD sum rules for the baryon charge and energy-momentum we demonstrate that if nucleons are the only degrees of freedom of nuclear wave function, the structure function of a nucleus would be the additive sum of the nucleon distributions at the same Bjorken x = AQ^2/2(p_Aq)< 0.5 up to very small Fermi motion corrections if x>0.05. Thus the difference of the EMC ratio from one reveals the presence of non-nucleonic degrees of freedom in nuclei. Using exact QCD sum rules we show that the ratio R_A(x_p,Q^2) used in experimental studies, where x_p = Q^2/2q_0 m_p deviates from one even if a nucleus consists of nucleons with small momenta only. Use of the Bjorken x leads to additional decrease of R_A(x,Q^2) as compared to the x_p plots. Coherent contribution of equivalent photons into photon component of parton wave function of a nucleus unambiguously follows from Lorentz…
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