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Excitation energies covered the resonance and the onset of the deep inelastic regions. We have determined for the first time the $Q^2$ evolution of $\\Gamma_1(Q^2)=\\int_0^{1} g_1(x,Q^2) dx$, $\\Gamma_2(Q^2)=\\int_0^1 g_2(x,Q^2) dx$ and $d_2 (Q^2) = \\int_0^1 x^2[ 2g_1(x,Q^2) + 3g_2(x,Q^2)] dx$ for the neutron in the range 0.1 GeV$^2$ $\\leq Q^2 \\"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"hep-ex/0310003","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ex","submitted_at":"2003-10-01T13:19:25Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"d787898bd6b88e130f214fed6b7deb2f383f2a5607c8856ef2c6f04abaf8fdce","abstract_canon_sha256":"50276c0810adbe350cb39e0e1b940025d0bcce3d8222648a9c92b180acb542c5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:47:31.727392Z","signature_b64":"WNGzlZ9G6582cbhlVZ6DbwKTfHe8RlNH5iEuKNyJi39I5fCzAvECBSMWhs166Udf05Wm9kJWahaqDSWIVb2BAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"99698cdbccecfb1f25182a31b2e03132b0575a02f3617db80dd7cabea6afb865","last_reissued_at":"2026-05-18T03:47:31.726565Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:47:31.726565Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Q^2 Evolution of the Neutron Spin Structure Moments using a He-3 Target","license":"","headline":"","cross_cats":["nucl-ex"],"primary_cat":"hep-ex","authors_text":"et al, J. Berthot, L. Auerbach, T. Averett, the Jefferson Lab E94-010 Collaboration: M. Amarian","submitted_at":"2003-10-01T13:19:25Z","abstract_excerpt":"We have measured the spin structure functions $g_1$ and $g_2$ of $^3$He in a double-spin experiment by inclusively scattering polarized electrons at energies ranging from 0.862 to 5.07 GeV off a polarized $^3$He target at a 15.5$^{\\circ}$ scattering angle. Excitation energies covered the resonance and the onset of the deep inelastic regions. We have determined for the first time the $Q^2$ evolution of $\\Gamma_1(Q^2)=\\int_0^{1} g_1(x,Q^2) dx$, $\\Gamma_2(Q^2)=\\int_0^1 g_2(x,Q^2) dx$ and $d_2 (Q^2) = \\int_0^1 x^2[ 2g_1(x,Q^2) + 3g_2(x,Q^2)] dx$ for the neutron in the range 0.1 GeV$^2$ $\\leq Q^2 \\"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ex/0310003","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-ex/0310003","created_at":"2026-05-18T03:47:31.726706+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ex/0310003v3","created_at":"2026-05-18T03:47:31.726706+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ex/0310003","created_at":"2026-05-18T03:47:31.726706+00:00"},{"alias_kind":"pith_short_12","alias_value":"TFUYZW6M5T5R","created_at":"2026-05-18T12:25:52.051335+00:00"},{"alias_kind":"pith_short_16","alias_value":"TFUYZW6M5T5R6JIY","created_at":"2026-05-18T12:25:52.051335+00:00"},{"alias_kind":"pith_short_8","alias_value":"TFUYZW6M","created_at":"2026-05-18T12:25:52.051335+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TFUYZW6M5T5R6JIYFIY3FYBRGK","json":"https://pith.science/pith/TFUYZW6M5T5R6JIYFIY3FYBRGK.json","graph_json":"https://pith.science/api/pith-number/TFUYZW6M5T5R6JIYFIY3FYBRGK/graph.json","events_json":"https://pith.science/api/pith-number/TFUYZW6M5T5R6JIYFIY3FYBRGK/events.json","paper":"https://pith.science/paper/TFUYZW6M"},"agent_actions":{"view_html":"https://pith.science/pith/TFUYZW6M5T5R6JIYFIY3FYBRGK","download_json":"https://pith.science/pith/TFUYZW6M5T5R6JIYFIY3FYBRGK.json","view_paper":"https://pith.science/paper/TFUYZW6M","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ex/0310003&json=true","fetch_graph":"https://pith.science/api/pith-number/TFUYZW6M5T5R6JIYFIY3FYBRGK/graph.json","fetch_events":"https://pith.science/api/pith-number/TFUYZW6M5T5R6JIYFIY3FYBRGK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TFUYZW6M5T5R6JIYFIY3FYBRGK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TFUYZW6M5T5R6JIYFIY3FYBRGK/action/storage_attestation","attest_author":"https://pith.science/pith/TFUYZW6M5T5R6JIYFIY3FYBRGK/action/author_attestation","sign_citation":"https://pith.science/pith/TFUYZW6M5T5R6JIYFIY3FYBRGK/action/citation_signature","submit_replication":"https://pith.science/pith/TFUYZW6M5T5R6JIYFIY3FYBRGK/action/replication_record"}},"created_at":"2026-05-18T03:47:31.726706+00:00","updated_at":"2026-05-18T03:47:31.726706+00:00"}