The spin-structure functions and , and the spin-dependent partial cross-section have been extracted from the polarized cross-sections differences, and measured for the 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 and 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 , and are evaluated with high precision for the neutron in the range from 0.035 to . 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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"Wojtsekhowski", "given_names": "B.", "full_name": "Wojtsekhowski, B." }, { "affiliations": [ { "country": "South Korea", "value": "Kyungpook National University, Taegu City, South Korea" } ], "surname": "Woo", "given_names": "S.", "full_name": "Woo, S." }, { "affiliations": [ { "country": "USA", "value": "Temple University, Philadelphia, USA" } ], "surname": "Yao", "given_names": "H.", "full_name": "Yao, H." }, { "affiliations": [ { "country": "USA", "value": "Rutgers, The State University of New Jersey, Piscataway, USA" } ], "surname": "Yuan", "given_names": "J.", "full_name": "Yuan, J." }, { "affiliations": [ { "country": "USA", "value": "Massachusetts Institute of Technology, Cambridge, USA" } ], "surname": "Zhan", "given_names": "X.", "full_name": "Zhan, X." }, { "affiliations": [ { "country": "USA", "value": "Argonne National Laboratory, Argonne, USA" } ], "surname": "Zheng", "given_names": "X.", "full_name": "Zheng, X." }, { "affiliations": [ { "country": "USA", "value": "Massachusetts Institute of Technology, Cambridge, USA" } ], "surname": "Zhu", "given_names": "L.", "full_name": "Zhu, L." } ], "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" } ], "dois": [ { "value": "10.1016/j.physletb.2020.135428" } ], "publication_info": [ { "journal_volume": "805 C", "journal_title": "Physics Letters B", "material": "article", "artid": "135428", "year": 2020 } ], "$schema": "http://repo.scoap3.org/schemas/hep.json", "acquisition_source": { "date": "2021-08-25T09:43:18.830633", "source": "Elsevier", "method": "Elsevier", "submission_number": "0598b3fc058711ecb53772fd3742099d" }, "license": [ { "url": "http://creativecommons.org/licenses/by/3.0/", "license": "CC-BY-3.0" } ], "copyright": [ { "holder": "The Author(s)", "statement": "The Author(s)", "year": "2020" } ], "control_number": "54022", "record_creation_date": "2020-04-23T23:30:31.030139", "_files": [ { "checksum": "md5:bff3bf66194b378fa88cacf36c72633c", "filetype": "xml", "bucket": "70f6743d-36f3-4d67-8b4d-73841a25c0b8", "version_id": "890fccb3-3648-4565-9ad4-a06d3e0780af", "key": "10.1016/j.physletb.2020.135428.xml", "size": 195154 }, { "checksum": "md5:767113f25b6da077e178cfaedc8d1326", "filetype": "pdf", "bucket": "70f6743d-36f3-4d67-8b4d-73841a25c0b8", "version_id": "f0c27e65-8076-43a9-b38b-edd63dc43144", "key": "10.1016/j.physletb.2020.135428.pdf", "size": 508160 }, { "checksum": "md5:767113f25b6da077e178cfaedc8d1326", "filetype": "pdf/a", "bucket": "70f6743d-36f3-4d67-8b4d-73841a25c0b8", "version_id": "09f7771d-bc35-4eca-aeed-acd1533d4ee8", "key": "10.1016/j.physletb.2020.135428_a.pdf", "size": 508160 } ], "collaborations": [ { "value": "Jefferson Lab E97-110 Collaboration" } ], "collections": [ { "primary": "Physics Letters B" } ], "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" } ] }