{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:MZFOSBFPPZZ5M255CFH7BZASRI","short_pith_number":"pith:MZFOSBFP","schema_version":"1.0","canonical_sha256":"664ae904af7e73d66bbd114ff0e4128a099ac7f76ece5a262f51fb4c0ceff1b4","source":{"kind":"arxiv","id":"nucl-th/9906091","version":2},"attestation_state":"computed","paper":{"title":"Deuteron electromagnetic properties and the viability of effective field theory methods in the two-nucleon system","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"D. R. Phillips (U. Washington, T. D. Cohen (U. Maryland), U. Maryland)","submitted_at":"1999-06-29T12:36:32Z","abstract_excerpt":"The central tenet of effective theory is that the details of short-distance physics will not have a significant impact on low-energy observables. Here we perform an analysis of electron-deuteron scattering at low momentum transfers which is based on effective field theory. We show that in our approach the deuteron electromagnetic form factors $F_C$ and $F_M$ indeed are largely insensitive to the short-range $NN$ potential at momenta $Q$ up to about 700 MeV. We also find that the effective field theory approach to deuteron electromagnetic structure provides a systematic justification for many f"},"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":"nucl-th/9906091","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1999-06-29T12:36:32Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"8319c512cf59b42e6b478fd64a6b050474ac1d0cfa856d150002dbb15db59240","abstract_canon_sha256":"e3cd14ba396503df994432eb876075bbda21ace929749b3b525bdffc79028e17"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:41:20.335694Z","signature_b64":"/xG5DyEWOGB5LhO59fI4UnhbHdysBSly6hP2TyYBaq47I7evCnlhrSJcIK4BPDUrXyAKRlOLuwjuALxkUTRNBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"664ae904af7e73d66bbd114ff0e4128a099ac7f76ece5a262f51fb4c0ceff1b4","last_reissued_at":"2026-07-04T15:41:20.335278Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:41:20.335278Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Deuteron electromagnetic properties and the viability of effective field theory methods in the two-nucleon system","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"D. R. Phillips (U. Washington, T. D. Cohen (U. Maryland), U. Maryland)","submitted_at":"1999-06-29T12:36:32Z","abstract_excerpt":"The central tenet of effective theory is that the details of short-distance physics will not have a significant impact on low-energy observables. Here we perform an analysis of electron-deuteron scattering at low momentum transfers which is based on effective field theory. We show that in our approach the deuteron electromagnetic form factors $F_C$ and $F_M$ indeed are largely insensitive to the short-range $NN$ potential at momenta $Q$ up to about 700 MeV. We also find that the effective field theory approach to deuteron electromagnetic structure provides a systematic justification for many f"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9906091","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/nucl-th/9906091/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"nucl-th/9906091","created_at":"2026-07-04T15:41:20.335339+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/9906091v2","created_at":"2026-07-04T15:41:20.335339+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/9906091","created_at":"2026-07-04T15:41:20.335339+00:00"},{"alias_kind":"pith_short_12","alias_value":"MZFOSBFPPZZ5","created_at":"2026-07-04T15:41:20.335339+00:00"},{"alias_kind":"pith_short_16","alias_value":"MZFOSBFPPZZ5M255","created_at":"2026-07-04T15:41:20.335339+00:00"},{"alias_kind":"pith_short_8","alias_value":"MZFOSBFP","created_at":"2026-07-04T15:41:20.335339+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.19909","citing_title":"Gravitational form factors of the deuteron","ref_index":16,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MZFOSBFPPZZ5M255CFH7BZASRI","json":"https://pith.science/pith/MZFOSBFPPZZ5M255CFH7BZASRI.json","graph_json":"https://pith.science/api/pith-number/MZFOSBFPPZZ5M255CFH7BZASRI/graph.json","events_json":"https://pith.science/api/pith-number/MZFOSBFPPZZ5M255CFH7BZASRI/events.json","paper":"https://pith.science/paper/MZFOSBFP"},"agent_actions":{"view_html":"https://pith.science/pith/MZFOSBFPPZZ5M255CFH7BZASRI","download_json":"https://pith.science/pith/MZFOSBFPPZZ5M255CFH7BZASRI.json","view_paper":"https://pith.science/paper/MZFOSBFP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/9906091&json=true","fetch_graph":"https://pith.science/api/pith-number/MZFOSBFPPZZ5M255CFH7BZASRI/graph.json","fetch_events":"https://pith.science/api/pith-number/MZFOSBFPPZZ5M255CFH7BZASRI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MZFOSBFPPZZ5M255CFH7BZASRI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MZFOSBFPPZZ5M255CFH7BZASRI/action/storage_attestation","attest_author":"https://pith.science/pith/MZFOSBFPPZZ5M255CFH7BZASRI/action/author_attestation","sign_citation":"https://pith.science/pith/MZFOSBFPPZZ5M255CFH7BZASRI/action/citation_signature","submit_replication":"https://pith.science/pith/MZFOSBFPPZZ5M255CFH7BZASRI/action/replication_record"}},"created_at":"2026-07-04T15:41:20.335339+00:00","updated_at":"2026-07-04T15:41:20.335339+00:00"}