Abstract

We revisit the scale evolution of the quark and gluon spin contributions to the proton spin, $\frac{1}{2}\Delta \Sigma$ and $\Delta G$, using the three-loop results for the spin-dependent evolution kernels available in the literature. We argue that the evolution of the quark spin contribution may actually be extended to four-loop order, and that to all orders a single anomalous dimension governs the evolution of both $\Delta \Sigma$ and $\Delta G$. We present analytical solutions of the evolution equations for $\Delta \Sigma$ and $\Delta G$ and investigate their scale dependence both to large and down to lower "hadronic" scales. We find that the solutions remain perturbatively stable even to low scales, where they come closer to simple quark model expectations. We discuss a curious scenario for the proton spin, in which even the gluon spin contribution is essentially scale independent and has a finite asymptotic value as the scale becomes large. We finally also show that perturbative three-loop evolution leads to a larger spin contribution of strange anti-quarks than of strange quarks.

Highlights

  • The decomposition of the proton spin in terms of the contributions by quarks and antiquarks, gluons, and orbital motion is a key focus of modern nuclear and particle physics

  • We argue that the evolution of the quark spin contribution may be extended to the four-loop order, and that to all orders a single anomalous dimension governs the evolution of both ΔΣ and ΔG

  • We have presented a set of studies of the evolution of the quark and gluon spin contributions to the proton spin at higher orders in perturbation theory, motivated by the recent calculations of the helicity splitting functions at full next-to-next-to-leading order (NNLO) [10,11,12]

Read more

Summary

INTRODUCTION

The decomposition of the proton spin in terms of the contributions by quarks and antiquarks, gluons, and orbital motion is a key focus of modern nuclear and particle physics. The two physically most relevant spin sum rules for the proton are the Ji decomposition [2], which ascribes the proton spin to gaugeinvariant contributions by quark spins and orbital angular momenta, and total gluon angular momentum, and the Jaffe-Manohar decomposition [1], in which there are four separate pieces corresponding to quark and gluon spin and orbital contributions, respectively. The Jaffe-Manohar sum rule corresponds to the canonical decomposition of the proton’s angular momentum. It may be regarded as a “partonic” spin sum rule, since both the quark and gluon spin pieces are related to parton. ΔΣ and ΔG may be obtained from the first moments of the helicity parton distributions Δqðx; Q2Þ, Δqðx; Q2Þ (where q 1⁄4 u; d; s; ...) and Δgðx; Q2Þ of the proton:

Nf Z 1
EVOLUTION EQUATIONS
FIRST MOMENTS OF THE SPLITTING FUNCTIONS
HIGHER-ORDER SOLUTIONS IN THE SINGLET SECTOR
NONSINGLET EVOLUTION OF THE VALENCE QUARK SPIN CONTRIBUTION
Findings
CONCLUSIONS
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call