{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:LDBT53XMCU5MGN3OA4W7XAPAGQ","short_pith_number":"pith:LDBT53XM","schema_version":"1.0","canonical_sha256":"58c33eeeec153ac3376e072dfb81e0343600a1a36adf6d250a2bb94140de5837","source":{"kind":"arxiv","id":"1908.11484","version":5},"attestation_state":"computed","paper":{"title":"$\\Omega$-deuteron Interaction in Folding Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Faisal Etminan, Mohammad Mehdi Firoozabadi","submitted_at":"2019-08-29T23:51:43Z","abstract_excerpt":"A simple single folding model for $\\Omega$-deuteron with maximal spin $\\left(I\\right)J^{P}=\\left(0\\right)5/2^{+}$ is investigated. $\\Omega$ is assumed to orbit an unperturbed deuteron in a $\\Omega$-deuteron potential based on a separable $\\Omega$-nucleon potential from lattice QCD. We show that the effective central folding potential of $\\Omega d$ in the $^{5}S_{2}$ channel has a simple Wood-Saxon form, and approximate the upper bound for the binding energy of $\\Omega$ particle on a deuteron. In order to investigate how changes in the wave functions affect the results, we consider four analyti"},"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":"1908.11484","kind":"arxiv","version":5},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-08-29T23:51:43Z","cross_cats_sorted":[],"title_canon_sha256":"c6d9ac5a9f94b8afaf40ca9572d8b4922ff9be8dcaa43f59b83d8c6508ee7fa6","abstract_canon_sha256":"1f8f6ff0f26835168b68c5de617712dc60139aea3c9c2b4723ddba3b47fef49c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:39:52.740073Z","signature_b64":"PTsTIPu0PNZUH5gfofImojVLsE+YxtHaR7h77Cu28PVS3bi7U8jYysBN/9dkO6Efj8Qm6u//BJLVkNDzJUiHDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"58c33eeeec153ac3376e072dfb81e0343600a1a36adf6d250a2bb94140de5837","last_reissued_at":"2026-07-05T03:39:52.739728Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:39:52.739728Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$\\Omega$-deuteron Interaction in Folding Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Faisal Etminan, Mohammad Mehdi Firoozabadi","submitted_at":"2019-08-29T23:51:43Z","abstract_excerpt":"A simple single folding model for $\\Omega$-deuteron with maximal spin $\\left(I\\right)J^{P}=\\left(0\\right)5/2^{+}$ is investigated. $\\Omega$ is assumed to orbit an unperturbed deuteron in a $\\Omega$-deuteron potential based on a separable $\\Omega$-nucleon potential from lattice QCD. We show that the effective central folding potential of $\\Omega d$ in the $^{5}S_{2}$ channel has a simple Wood-Saxon form, and approximate the upper bound for the binding energy of $\\Omega$ particle on a deuteron. In order to investigate how changes in the wave functions affect the results, we consider four analyti"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1908.11484","kind":"arxiv","version":5},"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/1908.11484/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":"1908.11484","created_at":"2026-07-05T03:39:52.739782+00:00"},{"alias_kind":"arxiv_version","alias_value":"1908.11484v5","created_at":"2026-07-05T03:39:52.739782+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1908.11484","created_at":"2026-07-05T03:39:52.739782+00:00"},{"alias_kind":"pith_short_12","alias_value":"LDBT53XMCU5M","created_at":"2026-07-05T03:39:52.739782+00:00"},{"alias_kind":"pith_short_16","alias_value":"LDBT53XMCU5MGN3O","created_at":"2026-07-05T03:39:52.739782+00:00"},{"alias_kind":"pith_short_8","alias_value":"LDBT53XM","created_at":"2026-07-05T03:39:52.739782+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/LDBT53XMCU5MGN3OA4W7XAPAGQ","json":"https://pith.science/pith/LDBT53XMCU5MGN3OA4W7XAPAGQ.json","graph_json":"https://pith.science/api/pith-number/LDBT53XMCU5MGN3OA4W7XAPAGQ/graph.json","events_json":"https://pith.science/api/pith-number/LDBT53XMCU5MGN3OA4W7XAPAGQ/events.json","paper":"https://pith.science/paper/LDBT53XM"},"agent_actions":{"view_html":"https://pith.science/pith/LDBT53XMCU5MGN3OA4W7XAPAGQ","download_json":"https://pith.science/pith/LDBT53XMCU5MGN3OA4W7XAPAGQ.json","view_paper":"https://pith.science/paper/LDBT53XM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1908.11484&json=true","fetch_graph":"https://pith.science/api/pith-number/LDBT53XMCU5MGN3OA4W7XAPAGQ/graph.json","fetch_events":"https://pith.science/api/pith-number/LDBT53XMCU5MGN3OA4W7XAPAGQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LDBT53XMCU5MGN3OA4W7XAPAGQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LDBT53XMCU5MGN3OA4W7XAPAGQ/action/storage_attestation","attest_author":"https://pith.science/pith/LDBT53XMCU5MGN3OA4W7XAPAGQ/action/author_attestation","sign_citation":"https://pith.science/pith/LDBT53XMCU5MGN3OA4W7XAPAGQ/action/citation_signature","submit_replication":"https://pith.science/pith/LDBT53XMCU5MGN3OA4W7XAPAGQ/action/replication_record"}},"created_at":"2026-07-05T03:39:52.739782+00:00","updated_at":"2026-07-05T03:39:52.739782+00:00"}