{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1994:FZWHOGEQJTJE7XIBSSHSDXOCYR","short_pith_number":"pith:FZWHOGEQ","schema_version":"1.0","canonical_sha256":"2e6c7718904cd24fdd01948f21ddc2c45f3ba4fda61967653b804e22b31daa3f","source":{"kind":"arxiv","id":"nucl-th/9408016","version":1},"attestation_state":"computed","paper":{"title":"An accurate nucleon-nucleon potential with charge-independence breaking","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"R.B.Wiringa, R.Schiavilla, V.G.J.Stoks","submitted_at":"1994-08-15T22:43:01Z","abstract_excerpt":"We present a new high-quality nucleon-nucleon potential with explicit charge dependence and charge asymmetry, which we designate Argonne $v_{18}$. The model has a charge-independent part with fourteen operator components that is an updated version of the Argonne $v_{14}$ potential. Three additional charge-dependent and one charge-asymmetric operators are added, along with a complete electromagnetic interaction. The potential has been fit directly to the Nijmegen $pp$ and $np$ scattering data base, low-energy $nn$ scattering parameters, and deuteron binding energy. With 40 adjustable parameters"},"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/9408016","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1994-08-15T22:43:01Z","cross_cats_sorted":[],"title_canon_sha256":"be82ac106f48489a4b8ffe7ca7eac3c7b70814dc66f767fb956c930b0026ecea","abstract_canon_sha256":"e5e1704981fbd80f310123fcb0c05286496ca99d765cbb02f426cc88244545ad"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:51:00.126440Z","signature_b64":"Ry5QMIy9UYvGb+4FxEQg/IhYLhfk3vHnkwY17STs0DLW/ITf73sosti89ruHKqIk5XdeupbRcWqy2yN8CupcBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2e6c7718904cd24fdd01948f21ddc2c45f3ba4fda61967653b804e22b31daa3f","last_reissued_at":"2026-07-04T15:51:00.126079Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:51:00.126079Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"An accurate nucleon-nucleon potential with charge-independence breaking","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"R.B.Wiringa, R.Schiavilla, V.G.J.Stoks","submitted_at":"1994-08-15T22:43:01Z","abstract_excerpt":"We present a new high-quality nucleon-nucleon potential with explicit charge dependence and charge asymmetry, which we designate Argonne $v_{18}$. The model has a charge-independent part with fourteen operator components that is an updated version of the Argonne $v_{14}$ potential. Three additional charge-dependent and one charge-asymmetric operators are added, along with a complete electromagnetic interaction. The potential has been fit directly to the Nijmegen $pp$ and $np$ scattering data base, low-energy $nn$ scattering parameters, and deuteron binding energy. With 40 adjustable parameters"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9408016","kind":"arxiv","version":1},"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/9408016/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/9408016","created_at":"2026-07-04T15:51:00.126138+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/9408016v1","created_at":"2026-07-04T15:51:00.126138+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/9408016","created_at":"2026-07-04T15:51:00.126138+00:00"},{"alias_kind":"pith_short_12","alias_value":"FZWHOGEQJTJE","created_at":"2026-07-04T15:51:00.126138+00:00"},{"alias_kind":"pith_short_16","alias_value":"FZWHOGEQJTJE7XIB","created_at":"2026-07-04T15:51:00.126138+00:00"},{"alias_kind":"pith_short_8","alias_value":"FZWHOGEQ","created_at":"2026-07-04T15:51:00.126138+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":8,"internal_anchor_count":6,"sample":[{"citing_arxiv_id":"2606.26926","citing_title":"Challenging chiral EFT with tritium beta decay","ref_index":59,"is_internal_anchor":true},{"citing_arxiv_id":"2606.09254","citing_title":"Meson-Nucleus Bound States with Neural-Network Quantum States","ref_index":52,"is_internal_anchor":true},{"citing_arxiv_id":"2602.19504","citing_title":"Three-body molecular states composed of $D^{(*)}$ and two nucleons","ref_index":29,"is_internal_anchor":true},{"citing_arxiv_id":"2504.08631","citing_title":"Can the strong interactions between hadrons be determined using femtoscopy?","ref_index":11,"is_internal_anchor":true},{"citing_arxiv_id":"2605.17139","citing_title":"Stable minimum principles for scattering states","ref_index":29,"is_internal_anchor":true},{"citing_arxiv_id":"2605.14006","citing_title":"Quantum Monte Carlo calculation of $\\delta_C$ in the superallowed beta decay of $^{10}$C","ref_index":23,"is_internal_anchor":true},{"citing_arxiv_id":"2605.08338","citing_title":"Revisiting predictions for cosmic-ray antinucleon fluxes from Galactic Dark Matter","ref_index":45,"is_internal_anchor":false},{"citing_arxiv_id":"2604.23110","citing_title":"On the Cancellation of Nuclear Effects in the Valence Region","ref_index":35,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FZWHOGEQJTJE7XIBSSHSDXOCYR","json":"https://pith.science/pith/FZWHOGEQJTJE7XIBSSHSDXOCYR.json","graph_json":"https://pith.science/api/pith-number/FZWHOGEQJTJE7XIBSSHSDXOCYR/graph.json","events_json":"https://pith.science/api/pith-number/FZWHOGEQJTJE7XIBSSHSDXOCYR/events.json","paper":"https://pith.science/paper/FZWHOGEQ"},"agent_actions":{"view_html":"https://pith.science/pith/FZWHOGEQJTJE7XIBSSHSDXOCYR","download_json":"https://pith.science/pith/FZWHOGEQJTJE7XIBSSHSDXOCYR.json","view_paper":"https://pith.science/paper/FZWHOGEQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/9408016&json=true","fetch_graph":"https://pith.science/api/pith-number/FZWHOGEQJTJE7XIBSSHSDXOCYR/graph.json","fetch_events":"https://pith.science/api/pith-number/FZWHOGEQJTJE7XIBSSHSDXOCYR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FZWHOGEQJTJE7XIBSSHSDXOCYR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FZWHOGEQJTJE7XIBSSHSDXOCYR/action/storage_attestation","attest_author":"https://pith.science/pith/FZWHOGEQJTJE7XIBSSHSDXOCYR/action/author_attestation","sign_citation":"https://pith.science/pith/FZWHOGEQJTJE7XIBSSHSDXOCYR/action/citation_signature","submit_replication":"https://pith.science/pith/FZWHOGEQJTJE7XIBSSHSDXOCYR/action/replication_record"}},"created_at":"2026-07-04T15:51:00.126138+00:00","updated_at":"2026-07-04T15:51:00.126138+00:00"}