{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:3KK525R2D7SHJNVP22Z7ZJFBHX","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"12ea48ac822a1a59a898496c047de4e9c1c5517e927c2a602534eb672be43822","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-05-17T08:29:49Z","title_canon_sha256":"ea05c28ea9d20c5edaa9bb88c8b53fa295838471a23d41df10d764f975e9e8fd"},"schema_version":"1.0","source":{"id":"2605.17322","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.17322","created_at":"2026-05-20T00:03:52Z"},{"alias_kind":"arxiv_version","alias_value":"2605.17322v1","created_at":"2026-05-20T00:03:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.17322","created_at":"2026-05-20T00:03:52Z"},{"alias_kind":"pith_short_12","alias_value":"3KK525R2D7SH","created_at":"2026-05-20T00:03:52Z"},{"alias_kind":"pith_short_16","alias_value":"3KK525R2D7SHJNVP","created_at":"2026-05-20T00:03:52Z"},{"alias_kind":"pith_short_8","alias_value":"3KK525R2","created_at":"2026-05-20T00:03:52Z"}],"graph_snapshots":[{"event_id":"sha256:c7047a87ab24a3218acee192d2e6a0edb6140052f4cbee60967d19c12bd71a49","target":"graph","created_at":"2026-05-20T00:03:52Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[{"findings_count":0,"name":"claim_evidence","ran_at":"2026-05-19T21:41:57.816234Z","status":"completed","version":"1.0.0"},{"findings_count":0,"name":"ai_meta_artifact","ran_at":"2026-05-19T21:33:23.748654Z","status":"skipped","version":"1.0.0"}],"endpoint":"/pith/2605.17322/integrity.json","findings":[],"snapshot_sha256":"b1a05fb42a9a230d9d155e639c3ec8a3c043ed4e4370e745d65a4f99f81e96c2","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In this work, we enumerated the mass spectra of the experimentally unobserved $1F$-wave states with the the orbital angular momentum $L$ = 3 for the singly heavy $\\Sigma_{Q}$, $\\Xi^{\\prime}_{Q}$, and $\\Omega_{Q}$ $(Q=c, b)$ baryons in the framework of quark-diquark configuration using the Regge trajectory model and the scaling rules. To determine the effective masses of the heavy quark and two light quarks, the relativistic effective mass formula are employed by combining the Coulomb potential. Within the spin-dependent Hamiltonian, we construct the mass shift forms as a non-diagonal symmetric","authors_text":"Ji-Hai Pan, Ji-Si Pan","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-05-17T08:29:49Z","title":"Investigating the mass spectra of $1F$-wave singly heavy $\\Sigma_{Q}$, $\\Xi^{\\prime}_{Q}$, and $\\Omega_{Q}$ baryons"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2605.17322","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:d1717b090b47ddf53bbc2adadbc759fd1cbd5618ccdfd6f9fd556447fc619a6a","target":"record","created_at":"2026-05-20T00:03:52Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"12ea48ac822a1a59a898496c047de4e9c1c5517e927c2a602534eb672be43822","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-05-17T08:29:49Z","title_canon_sha256":"ea05c28ea9d20c5edaa9bb88c8b53fa295838471a23d41df10d764f975e9e8fd"},"schema_version":"1.0","source":{"id":"2605.17322","kind":"arxiv","version":1}},"canonical_sha256":"da95dd763a1fe474b6afd6b3fca4a13dc5e1c5cb83e3408f2a22d99208792d82","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"da95dd763a1fe474b6afd6b3fca4a13dc5e1c5cb83e3408f2a22d99208792d82","first_computed_at":"2026-05-20T00:03:52.070536Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-20T00:03:52.070536Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"fXgFJ5e7ifJ+eu253JnWExvnTeldzCqTZHboJnlhKl7xZVRnVejbyUNSEWLsqlcV3wrbWrpgubwM9D2hrDZHCA==","signature_status":"signed_v1","signed_at":"2026-05-20T00:03:52.072045Z","signed_message":"canonical_sha256_bytes"},"source_id":"2605.17322","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d1717b090b47ddf53bbc2adadbc759fd1cbd5618ccdfd6f9fd556447fc619a6a","sha256:c7047a87ab24a3218acee192d2e6a0edb6140052f4cbee60967d19c12bd71a49"],"state_sha256":"0e8c7181173ab356b93b32f52f5a740f476c4f76d922fc9d28ef05e6da50e0da"}