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Some Inequalities for the Generalized Parton Distribution E(x,0,t)

Matthias Burkardt

TL;DR

This paper derives positivity-based constraints on the generalized parton distribution $E(x,0,t)$ by working in impact parameter space and relating $E$ to forward PDFs. The main results are inequalities that bound integrals and the value of $E$ in terms of $q_\pm(x)$ and the slope of $H_+(x,0,t)$ at $t=0$, making the constraints more directly usable with data. In the $x\to1$ limit, $E(x,0,0)$ is shown to vanish faster than the unpolarized distribution, and the authors provide a bound on the second moment of $E$, offering a practical way to limit $E$'s contribution to the quark angular momentum sum rule. Overall, these momentum-space inequalities enhance model-independent constraints on $E$ and its role in nucleon spin structure.

Abstract

We discuss some constraints on the $x$ and $t$-dependence of $E(x,0,t)$ that arise from positivity bounds in the impact parameter representation. In addition, we show that $E(x,0,0)$ for the nucleon vanishes for $x\to 1$ at least as rapidly as $(1-x)^4$. Finally we provide an inequality that limits the contribution from $E$ to the angular momentum sum rule.

Some Inequalities for the Generalized Parton Distribution E(x,0,t)

TL;DR

This paper derives positivity-based constraints on the generalized parton distribution by working in impact parameter space and relating to forward PDFs. The main results are inequalities that bound integrals and the value of in terms of and the slope of at , making the constraints more directly usable with data. In the limit, is shown to vanish faster than the unpolarized distribution, and the authors provide a bound on the second moment of , offering a practical way to limit 's contribution to the quark angular momentum sum rule. Overall, these momentum-space inequalities enhance model-independent constraints on and its role in nucleon spin structure.

Abstract

We discuss some constraints on the and -dependence of that arise from positivity bounds in the impact parameter representation. In addition, we show that for the nucleon vanishes for at least as rapidly as . Finally we provide an inequality that limits the contribution from to the angular momentum sum rule.

Paper Structure

This paper contains 3 sections, 20 equations.