{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:KEPOWNKAEAI5JU3MRLD6J5AD6Z","short_pith_number":"pith:KEPOWNKA","schema_version":"1.0","canonical_sha256":"511eeb35402011d4d36c8ac7e4f403f647bd30c3da681ff2c7406dc57c7044b7","source":{"kind":"arxiv","id":"2402.06914","version":2},"attestation_state":"computed","paper":{"title":"Examination of the $ \\phi-NN $ bound-state problem with lattice QCD $ N-\\phi $ potentials","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Amanullah Aalimi, Faisal Etminan","submitted_at":"2024-02-10T09:24:46Z","abstract_excerpt":"The developed Faddeev three-body equations are solved to search for bound-state solutions of a phi-meson $ \\left(\\phi\\right) $ and two nucleons $ \\left( \\textrm{NN} \\right) $ system. The newly published spin $ 3/2 $ $ \\textrm{N-\\ensuremath{\\phi}} $ potential based on the $ \\left(\\textrm{2+1}\\right) $-flavor lattice QCD simulations near physical point, and realistic $ \\textrm{NN} $ Malfliet-Tjon (MT) potential, are employed. Our numerical calculations for $ (I)J^{\\pi}=(0)2^{-}$ $ \\phi\\textrm{-d} $ system in maximum spin leads to ground state binding energy of about $ 7 $ MeV and a matter radius"},"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":"2402.06914","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2024-02-10T09:24:46Z","cross_cats_sorted":[],"title_canon_sha256":"a4a8e60c10f9f4ff18080a0bf61a68792563cb4eac6c8853da30b6e2b3a5e62a","abstract_canon_sha256":"fe9ee45dd14ac4f60d77372dfe723a10540672c9a03b1b1b0a5a5a35aad14eae"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:28:05.844009Z","signature_b64":"X7ElP6z30qlFpOvSUpS6XMeM1AkAtUNa037qXNMS3xPccaciQdIrk058NtMAEi1KY4N2sX80lfvonkOF1bWTBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"511eeb35402011d4d36c8ac7e4f403f647bd30c3da681ff2c7406dc57c7044b7","last_reissued_at":"2026-07-05T08:28:05.843587Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:28:05.843587Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Examination of the $ \\phi-NN $ bound-state problem with lattice QCD $ N-\\phi $ potentials","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Amanullah Aalimi, Faisal Etminan","submitted_at":"2024-02-10T09:24:46Z","abstract_excerpt":"The developed Faddeev three-body equations are solved to search for bound-state solutions of a phi-meson $ \\left(\\phi\\right) $ and two nucleons $ \\left( \\textrm{NN} \\right) $ system. The newly published spin $ 3/2 $ $ \\textrm{N-\\ensuremath{\\phi}} $ potential based on the $ \\left(\\textrm{2+1}\\right) $-flavor lattice QCD simulations near physical point, and realistic $ \\textrm{NN} $ Malfliet-Tjon (MT) potential, are employed. Our numerical calculations for $ (I)J^{\\pi}=(0)2^{-}$ $ \\phi\\textrm{-d} $ system in maximum spin leads to ground state binding energy of about $ 7 $ MeV and a matter radius"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2402.06914","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/2402.06914/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":"2402.06914","created_at":"2026-07-05T08:28:05.843646+00:00"},{"alias_kind":"arxiv_version","alias_value":"2402.06914v2","created_at":"2026-07-05T08:28:05.843646+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2402.06914","created_at":"2026-07-05T08:28:05.843646+00:00"},{"alias_kind":"pith_short_12","alias_value":"KEPOWNKAEAI5","created_at":"2026-07-05T08:28:05.843646+00:00"},{"alias_kind":"pith_short_16","alias_value":"KEPOWNKAEAI5JU3M","created_at":"2026-07-05T08:28:05.843646+00:00"},{"alias_kind":"pith_short_8","alias_value":"KEPOWNKA","created_at":"2026-07-05T08:28:05.843646+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2608.03162","citing_title":"Faddeev equations for the $J/\\psi\\,NN$ and $\\phi\\,NN$ three-body systems in momentum space","ref_index":97,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KEPOWNKAEAI5JU3MRLD6J5AD6Z","json":"https://pith.science/pith/KEPOWNKAEAI5JU3MRLD6J5AD6Z.json","graph_json":"https://pith.science/api/pith-number/KEPOWNKAEAI5JU3MRLD6J5AD6Z/graph.json","events_json":"https://pith.science/api/pith-number/KEPOWNKAEAI5JU3MRLD6J5AD6Z/events.json","paper":"https://pith.science/paper/KEPOWNKA"},"agent_actions":{"view_html":"https://pith.science/pith/KEPOWNKAEAI5JU3MRLD6J5AD6Z","download_json":"https://pith.science/pith/KEPOWNKAEAI5JU3MRLD6J5AD6Z.json","view_paper":"https://pith.science/paper/KEPOWNKA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2402.06914&json=true","fetch_graph":"https://pith.science/api/pith-number/KEPOWNKAEAI5JU3MRLD6J5AD6Z/graph.json","fetch_events":"https://pith.science/api/pith-number/KEPOWNKAEAI5JU3MRLD6J5AD6Z/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KEPOWNKAEAI5JU3MRLD6J5AD6Z/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KEPOWNKAEAI5JU3MRLD6J5AD6Z/action/storage_attestation","attest_author":"https://pith.science/pith/KEPOWNKAEAI5JU3MRLD6J5AD6Z/action/author_attestation","sign_citation":"https://pith.science/pith/KEPOWNKAEAI5JU3MRLD6J5AD6Z/action/citation_signature","submit_replication":"https://pith.science/pith/KEPOWNKAEAI5JU3MRLD6J5AD6Z/action/replication_record"}},"created_at":"2026-07-05T08:28:05.843646+00:00","updated_at":"2026-07-05T08:28:05.843646+00:00"}