{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:66I5SU2GQFH72F47L5ZKREE6GI","short_pith_number":"pith:66I5SU2G","schema_version":"1.0","canonical_sha256":"f791d95346814ffd179f5f72a8909e322b99db2d6e24e4a2d61e2e4dada035ce","source":{"kind":"arxiv","id":"1305.7279","version":3},"attestation_state":"computed","paper":{"title":"The longitudinal response function of the deuteron in chiral effective field theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"C.-J. Yang, Daniel R. Phillips","submitted_at":"2013-05-31T01:02:35Z","abstract_excerpt":"We use chiral effective field theory (EFT) to make predictions for the longitudinal electromagnetic response function of the deuteron, f_L, which is measured in d(e,e'N) reactions. In this case the impulse approximation gives the full chiral EFT result up to corrections that are of O(P^4) relative to leading. By varying the cutoff in the chiral EFT calculations between 0.6 and 1 GeV we conclude that the calculation is accurate to better than 10 % for values of q^2 within 4 fm^{-2} of the quasi-free peak, up to final-state energies E_{np}=60 MeV. In these regions chiral EFT is in reasonable agr"},"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":"1305.7279","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-05-31T01:02:35Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"2eab4161cd92382897252a4d409472a7679aac198cf481cff7cf7213779877a3","abstract_canon_sha256":"3de7d1588f5e3b3d738215d9cc208935362d16e8f90c4777bb6f604cd56794be"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:10:45.713724Z","signature_b64":"ao2sJ7vdJTwi2j2sX3VBk9JirxsuNHrSK1h3fZcBV0G+bzb2oDwUffzxjyl9mExrW3f4hmRkhaoEOOms4VbHDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f791d95346814ffd179f5f72a8909e322b99db2d6e24e4a2d61e2e4dada035ce","last_reissued_at":"2026-05-18T03:10:45.712964Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:10:45.712964Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The longitudinal response function of the deuteron in chiral effective field theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"C.-J. Yang, Daniel R. Phillips","submitted_at":"2013-05-31T01:02:35Z","abstract_excerpt":"We use chiral effective field theory (EFT) to make predictions for the longitudinal electromagnetic response function of the deuteron, f_L, which is measured in d(e,e'N) reactions. In this case the impulse approximation gives the full chiral EFT result up to corrections that are of O(P^4) relative to leading. By varying the cutoff in the chiral EFT calculations between 0.6 and 1 GeV we conclude that the calculation is accurate to better than 10 % for values of q^2 within 4 fm^{-2} of the quasi-free peak, up to final-state energies E_{np}=60 MeV. In these regions chiral EFT is in reasonable agr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1305.7279","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":"1305.7279","created_at":"2026-05-18T03:10:45.713089+00:00"},{"alias_kind":"arxiv_version","alias_value":"1305.7279v3","created_at":"2026-05-18T03:10:45.713089+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1305.7279","created_at":"2026-05-18T03:10:45.713089+00:00"},{"alias_kind":"pith_short_12","alias_value":"66I5SU2GQFH7","created_at":"2026-05-18T12:27:36.564083+00:00"},{"alias_kind":"pith_short_16","alias_value":"66I5SU2GQFH72F47","created_at":"2026-05-18T12:27:36.564083+00:00"},{"alias_kind":"pith_short_8","alias_value":"66I5SU2G","created_at":"2026-05-18T12:27:36.564083+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/66I5SU2GQFH72F47L5ZKREE6GI","json":"https://pith.science/pith/66I5SU2GQFH72F47L5ZKREE6GI.json","graph_json":"https://pith.science/api/pith-number/66I5SU2GQFH72F47L5ZKREE6GI/graph.json","events_json":"https://pith.science/api/pith-number/66I5SU2GQFH72F47L5ZKREE6GI/events.json","paper":"https://pith.science/paper/66I5SU2G"},"agent_actions":{"view_html":"https://pith.science/pith/66I5SU2GQFH72F47L5ZKREE6GI","download_json":"https://pith.science/pith/66I5SU2GQFH72F47L5ZKREE6GI.json","view_paper":"https://pith.science/paper/66I5SU2G","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1305.7279&json=true","fetch_graph":"https://pith.science/api/pith-number/66I5SU2GQFH72F47L5ZKREE6GI/graph.json","fetch_events":"https://pith.science/api/pith-number/66I5SU2GQFH72F47L5ZKREE6GI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/66I5SU2GQFH72F47L5ZKREE6GI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/66I5SU2GQFH72F47L5ZKREE6GI/action/storage_attestation","attest_author":"https://pith.science/pith/66I5SU2GQFH72F47L5ZKREE6GI/action/author_attestation","sign_citation":"https://pith.science/pith/66I5SU2GQFH72F47L5ZKREE6GI/action/citation_signature","submit_replication":"https://pith.science/pith/66I5SU2GQFH72F47L5ZKREE6GI/action/replication_record"}},"created_at":"2026-05-18T03:10:45.713089+00:00","updated_at":"2026-05-18T03:10:45.713089+00:00"}