Momentum Flow Mechanisms and Color-Lorentz Forces on Quarks in the Nucleon
Xiangdong Ji, Chen Yang
TL;DR
This work reframes nucleon momentum conservation in terms of a continuous momentum current density derived from the QCD energy–momentum tensor, decomposed into quark kinetic, gluon tensor, and trace anomaly components. By combining lattice QCD results and experimental fits for gravitational form factors, it maps the coordinate-space momentum flow and color-Lorentz forces, showing that the trace anomaly contributes a sizable negative-pressure term that drives confinement with an average force of about 1 GeV/fm. The analysis clarifies that momentum flow is not simply a mechanical pressure but a balance of kinetic transport and interaction forces, highlighting the crucial role and current uncertainties of the anomaly sector through the scalar form factor $G_s(q^2)$ (and related $C/D$ form factors). It also discusses frame-dependent simplifications in the infinite-momentum limit, where $T^{++}$ dominates, and outlines paths to reduce uncertainties in future measurements and analyses.
Abstract
Momentum conservation in the nucleon is examined in terms of continuous flow of the momentum current density (or in short, momentum flow), which receives contributions from both kinetic motion and interacting forces involving quarks and gluons. While quarks conduct momentum flow through their kinetic motion and the gluon scalar (anomaly) contributes via pure interactions, the gluon stress tensor has both effects. The quarks momentum flow encodes the information of the color-Lorentz force density on them, and the momentum conservation allows to trace its origin to the gluon tensor and anomaly (a ``negative pressure'' potential). From the state-of-the-art lattice calculations and experimental fits on the form factors of the QCD energy-momentum tensor, we exhibit pictures of the momentum flow and the color-Lorentz forces on the quarks in the nucleon. In particular, the anomaly contributes a critical attractive force with a strength similar to that of a heavy-quark confinement potential.
