{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:PY7F4DE5KPGSS6DYIU7GDYWGCS","short_pith_number":"pith:PY7F4DE5","schema_version":"1.0","canonical_sha256":"7e3e5e0c9d53cd297878453e61e2c61497a47ad98fb29e1f4f94d4b6d81a77fb","source":{"kind":"arxiv","id":"2107.04957","version":1},"attestation_state":"computed","paper":{"title":"Prediction of an $\\Omega_{bbb}\\Omega_{bbb}$ dibaryon in the extended one-boson exchange model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"Li-Sheng Geng, Ming-Zhu Liu","submitted_at":"2021-07-11T03:54:54Z","abstract_excerpt":"Ever since Yukawa proposed that the pion is responsible for mediating the nucleon-nucleon interaction, meson exchanges have been widely used in understanding hadron-hadron interactions. The most studied mesons are the $\\sigma$, $\\pi$, $\\rho$, and $\\omega$, while other heavier mesons are often argued to be less relevant because they lead to short range interactions. However, the ranges of interactions should be compared with the size of the system under study but not in absolute terms. In this work, we propose that one charmoninium exchange is responsible for the formation of the $\\Omega_{ccc}\\"},"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":"2107.04957","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2021-07-11T03:54:54Z","cross_cats_sorted":["hep-ex","hep-lat"],"title_canon_sha256":"d0c4fa7962e3263db45670b5c7c2e3317bb44744cfce402a80d12b1147fd869a","abstract_canon_sha256":"c39e1221828b1d083e82aee7a8265c97e29e480a1dd5066a59d47b897161e9ed"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:38:23.137098Z","signature_b64":"HW2pCLYRUAB+MBoQEt9hSUkR+4D6bGMTNXDCh9M6fURl/S/rubnp9jEk0tstYUpvEdQEq9Sd/mCqVwo3zwtcDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7e3e5e0c9d53cd297878453e61e2c61497a47ad98fb29e1f4f94d4b6d81a77fb","last_reissued_at":"2026-07-05T03:38:23.136676Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:38:23.136676Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Prediction of an $\\Omega_{bbb}\\Omega_{bbb}$ dibaryon in the extended one-boson exchange model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"Li-Sheng Geng, Ming-Zhu Liu","submitted_at":"2021-07-11T03:54:54Z","abstract_excerpt":"Ever since Yukawa proposed that the pion is responsible for mediating the nucleon-nucleon interaction, meson exchanges have been widely used in understanding hadron-hadron interactions. The most studied mesons are the $\\sigma$, $\\pi$, $\\rho$, and $\\omega$, while other heavier mesons are often argued to be less relevant because they lead to short range interactions. However, the ranges of interactions should be compared with the size of the system under study but not in absolute terms. In this work, we propose that one charmoninium exchange is responsible for the formation of the $\\Omega_{ccc}\\"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2107.04957","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/2107.04957/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":"2107.04957","created_at":"2026-07-05T03:38:23.136742+00:00"},{"alias_kind":"arxiv_version","alias_value":"2107.04957v1","created_at":"2026-07-05T03:38:23.136742+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2107.04957","created_at":"2026-07-05T03:38:23.136742+00:00"},{"alias_kind":"pith_short_12","alias_value":"PY7F4DE5KPGS","created_at":"2026-07-05T03:38:23.136742+00:00"},{"alias_kind":"pith_short_16","alias_value":"PY7F4DE5KPGSS6DY","created_at":"2026-07-05T03:38:23.136742+00:00"},{"alias_kind":"pith_short_8","alias_value":"PY7F4DE5","created_at":"2026-07-05T03:38:23.136742+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.10660","citing_title":"Lattice QCD Study of Positive Parity Dibaryons with Maximal Charm and Strangeness","ref_index":20,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PY7F4DE5KPGSS6DYIU7GDYWGCS","json":"https://pith.science/pith/PY7F4DE5KPGSS6DYIU7GDYWGCS.json","graph_json":"https://pith.science/api/pith-number/PY7F4DE5KPGSS6DYIU7GDYWGCS/graph.json","events_json":"https://pith.science/api/pith-number/PY7F4DE5KPGSS6DYIU7GDYWGCS/events.json","paper":"https://pith.science/paper/PY7F4DE5"},"agent_actions":{"view_html":"https://pith.science/pith/PY7F4DE5KPGSS6DYIU7GDYWGCS","download_json":"https://pith.science/pith/PY7F4DE5KPGSS6DYIU7GDYWGCS.json","view_paper":"https://pith.science/paper/PY7F4DE5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2107.04957&json=true","fetch_graph":"https://pith.science/api/pith-number/PY7F4DE5KPGSS6DYIU7GDYWGCS/graph.json","fetch_events":"https://pith.science/api/pith-number/PY7F4DE5KPGSS6DYIU7GDYWGCS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PY7F4DE5KPGSS6DYIU7GDYWGCS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PY7F4DE5KPGSS6DYIU7GDYWGCS/action/storage_attestation","attest_author":"https://pith.science/pith/PY7F4DE5KPGSS6DYIU7GDYWGCS/action/author_attestation","sign_citation":"https://pith.science/pith/PY7F4DE5KPGSS6DYIU7GDYWGCS/action/citation_signature","submit_replication":"https://pith.science/pith/PY7F4DE5KPGSS6DYIU7GDYWGCS/action/replication_record"}},"created_at":"2026-07-05T03:38:23.136742+00:00","updated_at":"2026-07-05T03:38:23.136742+00:00"}