{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:OT5QOZKURPR6UT6L3LS3RRAPUC","short_pith_number":"pith:OT5QOZKU","schema_version":"1.0","canonical_sha256":"74fb0765548be3ea4fcbdae5b8c40fa09655b03d46e154287be30c6e3dc4870b","source":{"kind":"arxiv","id":"1304.3636","version":1},"attestation_state":"computed","paper":{"title":"Triply heavy baryon mass estimated within pNRQCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-ph"],"primary_cat":"nucl-th","authors_text":"Felipe J. Llanes-Estrada, Olga I. Pavlova (Univ. Complutense Madrid), Richard Williams (Univ. of Graz)","submitted_at":"2013-04-12T13:55:26Z","abstract_excerpt":"Potential-NRQCD offers an effective-theory based approach to heavy-quark physics. While meson Q-anti_Q computations are tractable in pure alpha_s-perturbation theory, more complex many-body quark systems transcend it. A possibility inherited from nuclear physics is to employ the perturbative static potentials in a numerical diagonalization, eventually obtaining the exact lowest eigenvalue in each channel for a given-order perturbative potential. The power counting is manifest in the potential instead of the spectrum. The NNLO-potential for the 3-body problem is already available, so we have ad"},"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":"1304.3636","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-04-12T13:55:26Z","cross_cats_sorted":["hep-lat","hep-ph"],"title_canon_sha256":"cf18f312bc0558bca4f7dce08608255290326f8f2765e5930ece3363549f4110","abstract_canon_sha256":"1f72f92bb0587fdd9d5ab547cb1ffa63adc9dfaefbbbf492d566b20c2dc0cb3d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:28:07.000264Z","signature_b64":"sgMY0YCuAzhKNmPKwE6EpiarHIOCq1wupj5LUaorhj4ozc/Mqwl94dA/vGrMhgfrBGYmdmmFx3RSqcaCdlyGAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"74fb0765548be3ea4fcbdae5b8c40fa09655b03d46e154287be30c6e3dc4870b","last_reissued_at":"2026-05-18T03:28:06.999565Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:28:06.999565Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Triply heavy baryon mass estimated within pNRQCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-ph"],"primary_cat":"nucl-th","authors_text":"Felipe J. Llanes-Estrada, Olga I. Pavlova (Univ. Complutense Madrid), Richard Williams (Univ. of Graz)","submitted_at":"2013-04-12T13:55:26Z","abstract_excerpt":"Potential-NRQCD offers an effective-theory based approach to heavy-quark physics. While meson Q-anti_Q computations are tractable in pure alpha_s-perturbation theory, more complex many-body quark systems transcend it. A possibility inherited from nuclear physics is to employ the perturbative static potentials in a numerical diagonalization, eventually obtaining the exact lowest eigenvalue in each channel for a given-order perturbative potential. The power counting is manifest in the potential instead of the spectrum. The NNLO-potential for the 3-body problem is already available, so we have ad"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1304.3636","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":""},"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":"1304.3636","created_at":"2026-05-18T03:28:06.999648+00:00"},{"alias_kind":"arxiv_version","alias_value":"1304.3636v1","created_at":"2026-05-18T03:28:06.999648+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1304.3636","created_at":"2026-05-18T03:28:06.999648+00:00"},{"alias_kind":"pith_short_12","alias_value":"OT5QOZKURPR6","created_at":"2026-05-18T12:27:54.935989+00:00"},{"alias_kind":"pith_short_16","alias_value":"OT5QOZKURPR6UT6L","created_at":"2026-05-18T12:27:54.935989+00:00"},{"alias_kind":"pith_short_8","alias_value":"OT5QOZKU","created_at":"2026-05-18T12:27:54.935989+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/OT5QOZKURPR6UT6L3LS3RRAPUC","json":"https://pith.science/pith/OT5QOZKURPR6UT6L3LS3RRAPUC.json","graph_json":"https://pith.science/api/pith-number/OT5QOZKURPR6UT6L3LS3RRAPUC/graph.json","events_json":"https://pith.science/api/pith-number/OT5QOZKURPR6UT6L3LS3RRAPUC/events.json","paper":"https://pith.science/paper/OT5QOZKU"},"agent_actions":{"view_html":"https://pith.science/pith/OT5QOZKURPR6UT6L3LS3RRAPUC","download_json":"https://pith.science/pith/OT5QOZKURPR6UT6L3LS3RRAPUC.json","view_paper":"https://pith.science/paper/OT5QOZKU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1304.3636&json=true","fetch_graph":"https://pith.science/api/pith-number/OT5QOZKURPR6UT6L3LS3RRAPUC/graph.json","fetch_events":"https://pith.science/api/pith-number/OT5QOZKURPR6UT6L3LS3RRAPUC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OT5QOZKURPR6UT6L3LS3RRAPUC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OT5QOZKURPR6UT6L3LS3RRAPUC/action/storage_attestation","attest_author":"https://pith.science/pith/OT5QOZKURPR6UT6L3LS3RRAPUC/action/author_attestation","sign_citation":"https://pith.science/pith/OT5QOZKURPR6UT6L3LS3RRAPUC/action/citation_signature","submit_replication":"https://pith.science/pith/OT5QOZKURPR6UT6L3LS3RRAPUC/action/replication_record"}},"created_at":"2026-05-18T03:28:06.999648+00:00","updated_at":"2026-05-18T03:28:06.999648+00:00"}