Measurement of the He spin-structure functions and of neutron ( He) spin-dependent sum rules at 0.035 ≤ ≤ 0.24 GeV

V. Sulkosky (College of William and Mary, Williamsburg, USA; Thomas Jefferson National Accelerator Facility, Newport News, USA; University of Virginia, Charlottesville, USA) ; J.T. Singh (University of Virginia, Charlottesville, USA) ; C. Peng (Duke University, Durham, USA) ; J.P. Chen (Thomas Jefferson National Accelerator Facility, Newport News, USA) ; A. Deur (University of Virginia, Charlottesville, USA; Thomas Jefferson National Accelerator Facility, Newport News, USA) ; et al. - Show all 109 authors

The spin-structure functions g1 and g2, and the spin-dependent partial cross-section σTT have been extracted from the polarized cross-sections differences, Δσ(ν,Q2) and Δσ(ν,Q2) measured for the He3(e,e)X reaction, in the E97-110 experiment at Jefferson Lab. Polarized electrons with energies from 1.147 to 4.404 GeV were scattered at angles of 6 and 9 from a longitudinally or transversely polarized $^{3}$He target. The data cover the kinematic regions of the quasi-elastic, resonance production and beyond. From the extracted spin-structure functions, the first moments Γ1(Q2), Γ2(Q2) and ITT(Q2) are evaluated with high precision for the neutron in the Q2 range from 0.035 to 0.24GeV2. The comparison of the data and the chiral effective field theory predictions reveals the importance of proper treatment of the Δ degree of freedom for spin observables.

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  "titles": [
    {
      "source": "Elsevier", 
      "title": "Measurement of the He spin-structure functions and of neutron ( He) spin-dependent sum rules at 0.035 \u2264 \u2264 0.24 GeV"
    }
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      "value": "10.1016/j.physletb.2020.135428"
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      "journal_title": "Physics Letters B", 
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      "license": "CC-BY-3.0"
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      "statement": "The Author(s)", 
      "year": "2020"
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      "value": "Jefferson Lab E97-110 Collaboration"
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      "primary": "Physics Letters B"
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  ], 
  "abstracts": [
    {
      "source": "Elsevier", 
      "value": "The spin-structure functions <math><msub><mrow><mi>g</mi></mrow><mrow><mn>1</mn></mrow></msub></math> and <math><msub><mrow><mi>g</mi></mrow><mrow><mn>2</mn></mrow></msub></math>, and the spin-dependent partial cross-section <math><msub><mrow><mi>\u03c3</mi></mrow><mrow><mi>TT</mi></mrow></msub></math> have been extracted from the polarized cross-sections differences, <math><mi>\u0394</mi><msub><mrow><mi>\u03c3</mi></mrow><mrow><mo>\u2225</mo></mrow></msub><mrow><mo>(</mo><mi>\u03bd</mi><mo>,</mo><msup><mrow><mi>Q</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>)</mo></mrow></math> and <math><mi>\u0394</mi><msub><mrow><mi>\u03c3</mi></mrow><mrow><mo>\u22a5</mo></mrow></msub><mrow><mo>(</mo><mi>\u03bd</mi><mo>,</mo><msup><mrow><mi>Q</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>)</mo></mrow></math> measured for the <math><mover><mrow><mmultiscripts><mrow><mtext>He</mtext></mrow><mprescripts></mprescripts><none></none><mrow><mtext>3</mtext></mrow></mmultiscripts></mrow><mrow><mo>\u2192</mo></mrow></mover><mo>(</mo><mover><mrow><mtext>e</mtext></mrow><mrow><mo>\u2192</mo></mrow></mover><mo>,</mo><msup><mrow><mtext>e</mtext></mrow><mrow><mo>\u2032</mo></mrow></msup><mo>)</mo><mtext>X</mtext></math> reaction, in the E97-110 experiment at Jefferson Lab. Polarized electrons with energies from 1.147 to 4.404 GeV were scattered at angles of <math><msup><mrow><mn>6</mn></mrow><mrow><mo>\u2218</mo></mrow></msup></math> and <math><msup><mrow><mn>9</mn></mrow><mrow><mo>\u2218</mo></mrow></msup></math> from a longitudinally or transversely polarized $^{3}$He target. The data cover the kinematic regions of the quasi-elastic, resonance production and beyond. From the extracted spin-structure functions, the first moments <math><mover><mrow><msub><mrow><mi>\u0393</mi></mrow><mrow><mn>1</mn></mrow></msub></mrow><mo>\u203e</mo></mover><mrow><mo>(</mo><msup><mrow><mi>Q</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>)</mo></mrow></math>, <math><msub><mrow><mi>\u0393</mi></mrow><mrow><mn>2</mn></mrow></msub><mrow><mo>(</mo><msup><mrow><mi>Q</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>)</mo></mrow></math> and <math><msub><mrow><mi>I</mi></mrow><mrow><mi>TT</mi></mrow></msub><mrow><mo>(</mo><msup><mrow><mi>Q</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>)</mo></mrow></math> are evaluated with high precision for the neutron in the <math><msup><mrow><mi>Q</mi></mrow><mrow><mn>2</mn></mrow></msup></math> range from 0.035 to <math><mn>0.24</mn><mspace width=\"0.25em\"></mspace><msup><mrow><mtext>GeV</mtext></mrow><mrow><mn>2</mn></mrow></msup></math>. The comparison of the data and the chiral effective field theory predictions reveals the importance of proper treatment of the \u0394 degree of freedom for spin observables."
    }
  ], 
  "imprints": [
    {
      "date": "2020-06-10", 
      "publisher": "Elsevier"
    }
  ]
}
Published on:
10 June 2020
Publisher:
Elsevier
Published in:
Physics Letters B , Volume 805 C (2020)

Article ID: 135428
DOI:
https://doi.org/10.1016/j.physletb.2020.135428
Copyrights:
The Author(s)
Licence:
CC-BY-3.0

Fulltext files: