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Precision Measurement of the Neutron Spin Asymmetries and Spin-dependent Structure Functions in the Valence Quark Region

X. Zheng

TL;DR

The paper delivers high-precision neutron spin observables in the valence region by scattering polarized electrons off polarized ^3He and extracting A1^n, A2^n, g1^n, and g2^n at x up to 0.60. Using rigorous nuclear corrections and radiative analyses, it finds A1^n crossing zero near x≈0.47 and becoming positive at larger x, with A2^n and g2^n measured to high precision and the higher-twist matrix element d2^n showing a positive signal. The results, combined with world proton data, yield polarized quark distributions: Δu/u agrees with several models, while Δd/d challenges LO pQCD with hadron helicity conservation, suggesting significant quark orbital angular momentum effects in the valence region. Overall, the work provides critical inputs for QCD-based PDFs and tests of nucleon spin structure in a regime where valence quarks dominate. It also demonstrates the efficacy of a ^3He target as an effective neutron probe and reinforces the role of higher-twist dynamics in spin-dependent observables.

Abstract

We report on measurements of the neutron spin asymmetries $A_{1,2}^n$ and polarized structure functions $g_{1,2}^n$ at three kinematics in the deep inelastic region, with $x=0.33$, 0.47 and 0.60 and $Q^2=2.7$, 3.5 and 4.8 (GeV/c)$^2$, respectively. These measurements were performed using a 5.7 GeV longitudinally-polarized electron beam and a polarized $^3$He target. The results for $A_1^n$ and $g_1^n$ at $x=0.33$ are consistent with previous world data and, at the two higher $x$ points, have improved the precision of the world data by about an order of magnitude. The new $A_1^n$ data show a zero crossing around $x=0.47$ and the value at $x=0.60$ is significantly positive. These results agree with a next-to-leading order QCD analysis of previous world data. The trend of data at high $x$ agrees with constituent quark model predictions but disagrees with that from leading-order perturbative QCD (pQCD) assuming hadron helicity conservation. Results for $A_2^n$ and $g_2^n$ have a precision comparable to the best world data in this kinematic region. Combined with previous world data, the moment $d_2^n$ was evaluated and the new result has improved the precision of this quantity by about a factor of two. When combined with the world proton data, polarized quark distribution functions were extracted from the new $g_1^n/F_1^n$ values based on the quark parton model. While results for $Δu/u$ agree well with predictions from various models, results for $Δd/d$ disagree with the leading-order pQCD prediction when hadron helicity conservation is imposed.

Precision Measurement of the Neutron Spin Asymmetries and Spin-dependent Structure Functions in the Valence Quark Region

TL;DR

The paper delivers high-precision neutron spin observables in the valence region by scattering polarized electrons off polarized ^3He and extracting A1^n, A2^n, g1^n, and g2^n at x up to 0.60. Using rigorous nuclear corrections and radiative analyses, it finds A1^n crossing zero near x≈0.47 and becoming positive at larger x, with A2^n and g2^n measured to high precision and the higher-twist matrix element d2^n showing a positive signal. The results, combined with world proton data, yield polarized quark distributions: Δu/u agrees with several models, while Δd/d challenges LO pQCD with hadron helicity conservation, suggesting significant quark orbital angular momentum effects in the valence region. Overall, the work provides critical inputs for QCD-based PDFs and tests of nucleon spin structure in a regime where valence quarks dominate. It also demonstrates the efficacy of a ^3He target as an effective neutron probe and reinforces the role of higher-twist dynamics in spin-dependent observables.

Abstract

We report on measurements of the neutron spin asymmetries and polarized structure functions at three kinematics in the deep inelastic region, with , 0.47 and 0.60 and , 3.5 and 4.8 (GeV/c), respectively. These measurements were performed using a 5.7 GeV longitudinally-polarized electron beam and a polarized He target. The results for and at are consistent with previous world data and, at the two higher points, have improved the precision of the world data by about an order of magnitude. The new data show a zero crossing around and the value at is significantly positive. These results agree with a next-to-leading order QCD analysis of previous world data. The trend of data at high agrees with constituent quark model predictions but disagrees with that from leading-order perturbative QCD (pQCD) assuming hadron helicity conservation. Results for and have a precision comparable to the best world data in this kinematic region. Combined with previous world data, the moment was evaluated and the new result has improved the precision of this quantity by about a factor of two. When combined with the world proton data, polarized quark distribution functions were extracted from the new values based on the quark parton model. While results for agree well with predictions from various models, results for disagree with the leading-order pQCD prediction when hadron helicity conservation is imposed.

Paper Structure

This paper contains 49 sections, 63 equations, 26 figures, 13 tables.

Figures (26)

  • Figure 1: Previous data on $A_1^n$data:a1ng1n-e142data:a1ng1n-e154data:g1n-smcdata:a1ng1n-hermesdata:a1pa1n-e143data:g1pg1n-e155 and various theoretical predictions: $A_1^n$ from SU(6) symmetry (solid line at zero) theory:su6close, hyperfine-perturbed RCQM (shaded band) theory:cqm, BBS parameterization at $Q^2=4$ (GeV/c)$^2$ (higher solid) theory:bbs, LSS(BBS) parameterization at $Q^2=4$ (GeV/c)$^2$ (dashed) theory:lssbbs, statistical model at $Q^2=4$ (GeV/c)$^2$ (long-dashed) theory:stat, quark-hadron duality using two different SU(6) breaking mechanisms (dash-dot-dotted and dash-dot-dot-dotted)theory:dual_new, and non-meson cloudy bag model (dash-dotted) theory:bag; $g_1^n/F_1^n$ from LSS2001 parameterization at $Q^2=5$ (GeV/c)$^2$ (lower solid) theory:lss2001 and from chiral soliton models theory:chi_weigel at $Q^2=3$ (GeV/c)$^2$ (long dash-dotted) and theory:chi_waka at $Q^2=4.8$ (GeV/c)$^2$ (dotted).
  • Figure 2: World data on $A_1^p$data:a1pa1n-e143data:a1pg1p-emcdata:a1pg1p-smcdata:g1pg1n-e155data:g1p-hermes and predictions for $g_1^p/F_1^p$ at $Q^2=5$ (GeV/c)$^2$ from the E155 experimental fit (long dash-dot-dotted) data:g1pg1n-e155 and a new fit as described in Section \ref{['result:neutron']} (long dash-dot-dot-dotted). The solid curve corresponds to the prediction for $g_1^n/F_1^n$ from LSS(2001) parameterization at $Q^2=5$ (GeV/c)$^2$. Other curves are the same as in Fig. \ref{['fig:a1nmodel_all']} except that there is no prediction for the proton from BBS and LSS(BBS) parameterizations.
  • Figure 3: An illustration of $^3$He wavefunction. The $S$, $S^\prime$ and $D$ state contributions are from calculations using the AV18 two-nucleon interaction and the Tucson-Melbourne three-nucleon force, as given in Ref. theory:PnPp_nogga.
  • Figure 4: (Color online) Top-view of the experimental hall A (not to scale).
  • Figure 5: Helicity signal and the helicity status of DAQ in toggle (top) and pseudorandom (bottom) modes.
  • ...and 21 more figures