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For the spin-triplet systems, we take into account the mixing between the ${}^3S_1$ and ${}^3D_1$ channels. For the baryon-baryon system $\\Xi_{cc}\\Xi_{cc}$ with $(R,I) = (\\bar{3}, 1/2)$ and $(\\bar{3}, 0)$, where $R$ and $I$ represent the group representation and the isospin of the system, respectively, there"},"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":"1704.01009","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-04-04T13:47:05Z","cross_cats_sorted":["hep-ex","nucl-th"],"title_canon_sha256":"455d5e455fd400ef2ef91528e8f5ad9c165e83ac44995743f4471160007738b1","abstract_canon_sha256":"c86130c65215f3cce747f873a69428e704e4f332ed4071f60d67c9b28a1c530d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:41:24.334179Z","signature_b64":"aSFGCMt7gpypuWm25fQxRPTAi7DkxFjeBHnscKCOtD7fRRjJfmhiksGViEUB6UqpVE5f74k6+EtcFbb19rKgBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cfdcc7602cb5b2a805adb5f4c5da939f4d9ab8057e51f1bea40a109a53c407ec","last_reissued_at":"2026-05-18T00:41:24.333601Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:41:24.333601Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Deuteron-like states composed of two doubly charmed baryons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Lu Meng, Ning Li, Shi-Lin Zhu","submitted_at":"2017-04-04T13:47:05Z","abstract_excerpt":"We present a systematic investigation of the possible molecular states composed of a pair of doubly charmed baryons ($\\Xi_{cc}\\Xi_{cc}$) or one doubly charmed baryon and one doubly charmed antibaryon $(\\Xi_{cc}\\bar{\\Xi}_{cc})$ within the framework of the one-boson-exchange-potential model. For the spin-triplet systems, we take into account the mixing between the ${}^3S_1$ and ${}^3D_1$ channels. For the baryon-baryon system $\\Xi_{cc}\\Xi_{cc}$ with $(R,I) = (\\bar{3}, 1/2)$ and $(\\bar{3}, 0)$, where $R$ and $I$ represent the group representation and the isospin of the system, respectively, there"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.01009","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":""},"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":"1704.01009","created_at":"2026-05-18T00:41:24.333719+00:00"},{"alias_kind":"arxiv_version","alias_value":"1704.01009v2","created_at":"2026-05-18T00:41:24.333719+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.01009","created_at":"2026-05-18T00:41:24.333719+00:00"},{"alias_kind":"pith_short_12","alias_value":"Z7OMOYBMWWZK","created_at":"2026-05-18T12:31:59.375834+00:00"},{"alias_kind":"pith_short_16","alias_value":"Z7OMOYBMWWZKQBNN","created_at":"2026-05-18T12:31:59.375834+00:00"},{"alias_kind":"pith_short_8","alias_value":"Z7OMOYBM","created_at":"2026-05-18T12:31:59.375834+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/Z7OMOYBMWWZKQBNNWX2MLWUTT5","json":"https://pith.science/pith/Z7OMOYBMWWZKQBNNWX2MLWUTT5.json","graph_json":"https://pith.science/api/pith-number/Z7OMOYBMWWZKQBNNWX2MLWUTT5/graph.json","events_json":"https://pith.science/api/pith-number/Z7OMOYBMWWZKQBNNWX2MLWUTT5/events.json","paper":"https://pith.science/paper/Z7OMOYBM"},"agent_actions":{"view_html":"https://pith.science/pith/Z7OMOYBMWWZKQBNNWX2MLWUTT5","download_json":"https://pith.science/pith/Z7OMOYBMWWZKQBNNWX2MLWUTT5.json","view_paper":"https://pith.science/paper/Z7OMOYBM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1704.01009&json=true","fetch_graph":"https://pith.science/api/pith-number/Z7OMOYBMWWZKQBNNWX2MLWUTT5/graph.json","fetch_events":"https://pith.science/api/pith-number/Z7OMOYBMWWZKQBNNWX2MLWUTT5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Z7OMOYBMWWZKQBNNWX2MLWUTT5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Z7OMOYBMWWZKQBNNWX2MLWUTT5/action/storage_attestation","attest_author":"https://pith.science/pith/Z7OMOYBMWWZKQBNNWX2MLWUTT5/action/author_attestation","sign_citation":"https://pith.science/pith/Z7OMOYBMWWZKQBNNWX2MLWUTT5/action/citation_signature","submit_replication":"https://pith.science/pith/Z7OMOYBMWWZKQBNNWX2MLWUTT5/action/replication_record"}},"created_at":"2026-05-18T00:41:24.333719+00:00","updated_at":"2026-05-18T00:41:24.333719+00:00"}