{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:3US3ACYS3LCKQJKVE4WSWVRTMC","short_pith_number":"pith:3US3ACYS","schema_version":"1.0","canonical_sha256":"dd25b00b12dac4a82555272d2b563360920c15eee152662520e4e293cbb3f689","source":{"kind":"arxiv","id":"2407.12190","version":2},"attestation_state":"computed","paper":{"title":"On a possible $^{3}_{\\phi}$H hypernucleus with HAL QCD interaction","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Branislav Vlahovic, Igor Filikhin, Roman Ya. Kezerashvili","submitted_at":"2024-07-16T21:34:51Z","abstract_excerpt":"Within the framework of the Faddeev formalism in configuration space, we investigate bound states in the $\\phi NN$ system with total isospin $T=0$ and $T=1$. The recently proposed lattice HAL QCD $\\phi N$ potential in the $^{4}S_{3/2}$ channel does not support either $\\phi N$ or $\\phi NN$ bound states. The HAL QCD $\\phi N$ potential in the $^{2}S_{1/2}$ channel suggests the bound states for $\\phi N$ and $\\phi NN (S=0)$ systems. However, the binding energies are highly sensitive to variations of the enhancement factor $\\beta$, and the $\\phi NN$ system is extremely strongly bound in the state $S"},"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":"2407.12190","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2024-07-16T21:34:51Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"7ca6d56af2c5ff21b02a573854df9958c447d49d0e5c9497dd4cf5adf090a1c7","abstract_canon_sha256":"aa18718fc1f9aba6c77ceb420ea9dcddbb266004758e2e5b59f17d9a289cb256"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:57:05.693985Z","signature_b64":"fLfV6revE5cf8zU9E14dsUeVzXuVKLFOoNicVgFu7R5imoP3Fl58Z6A+G3TNKgqHF+i+/Ig1eDuaXmAstTrnBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dd25b00b12dac4a82555272d2b563360920c15eee152662520e4e293cbb3f689","last_reissued_at":"2026-07-05T08:57:05.693530Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:57:05.693530Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On a possible $^{3}_{\\phi}$H hypernucleus with HAL QCD interaction","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Branislav Vlahovic, Igor Filikhin, Roman Ya. Kezerashvili","submitted_at":"2024-07-16T21:34:51Z","abstract_excerpt":"Within the framework of the Faddeev formalism in configuration space, we investigate bound states in the $\\phi NN$ system with total isospin $T=0$ and $T=1$. The recently proposed lattice HAL QCD $\\phi N$ potential in the $^{4}S_{3/2}$ channel does not support either $\\phi N$ or $\\phi NN$ bound states. The HAL QCD $\\phi N$ potential in the $^{2}S_{1/2}$ channel suggests the bound states for $\\phi N$ and $\\phi NN (S=0)$ systems. However, the binding energies are highly sensitive to variations of the enhancement factor $\\beta$, and the $\\phi NN$ system is extremely strongly bound in the state $S"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2407.12190","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/2407.12190/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":"2407.12190","created_at":"2026-07-05T08:57:05.693584+00:00"},{"alias_kind":"arxiv_version","alias_value":"2407.12190v2","created_at":"2026-07-05T08:57:05.693584+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2407.12190","created_at":"2026-07-05T08:57:05.693584+00:00"},{"alias_kind":"pith_short_12","alias_value":"3US3ACYS3LCK","created_at":"2026-07-05T08:57:05.693584+00:00"},{"alias_kind":"pith_short_16","alias_value":"3US3ACYS3LCKQJKV","created_at":"2026-07-05T08:57:05.693584+00:00"},{"alias_kind":"pith_short_8","alias_value":"3US3ACYS","created_at":"2026-07-05T08:57:05.693584+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.09254","citing_title":"Meson-Nucleus Bound States with Neural-Network Quantum States","ref_index":36,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3US3ACYS3LCKQJKVE4WSWVRTMC","json":"https://pith.science/pith/3US3ACYS3LCKQJKVE4WSWVRTMC.json","graph_json":"https://pith.science/api/pith-number/3US3ACYS3LCKQJKVE4WSWVRTMC/graph.json","events_json":"https://pith.science/api/pith-number/3US3ACYS3LCKQJKVE4WSWVRTMC/events.json","paper":"https://pith.science/paper/3US3ACYS"},"agent_actions":{"view_html":"https://pith.science/pith/3US3ACYS3LCKQJKVE4WSWVRTMC","download_json":"https://pith.science/pith/3US3ACYS3LCKQJKVE4WSWVRTMC.json","view_paper":"https://pith.science/paper/3US3ACYS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2407.12190&json=true","fetch_graph":"https://pith.science/api/pith-number/3US3ACYS3LCKQJKVE4WSWVRTMC/graph.json","fetch_events":"https://pith.science/api/pith-number/3US3ACYS3LCKQJKVE4WSWVRTMC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3US3ACYS3LCKQJKVE4WSWVRTMC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3US3ACYS3LCKQJKVE4WSWVRTMC/action/storage_attestation","attest_author":"https://pith.science/pith/3US3ACYS3LCKQJKVE4WSWVRTMC/action/author_attestation","sign_citation":"https://pith.science/pith/3US3ACYS3LCKQJKVE4WSWVRTMC/action/citation_signature","submit_replication":"https://pith.science/pith/3US3ACYS3LCKQJKVE4WSWVRTMC/action/replication_record"}},"created_at":"2026-07-05T08:57:05.693584+00:00","updated_at":"2026-07-05T08:57:05.693584+00:00"}