{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:D5OC7W4ZK22PXF5LFQVEONQKQX","short_pith_number":"pith:D5OC7W4Z","schema_version":"1.0","canonical_sha256":"1f5c2fdb9956b4fb97ab2c2a47360a85cd4f3410172ebb5c5bd6735669d07eff","source":{"kind":"arxiv","id":"2104.00439","version":1},"attestation_state":"computed","paper":{"title":"Spectroscopic Investigation of Light Strange S=-1 $\\Lambda$, $\\Sigma$ and S=-2 $\\Xi$ Baryons","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ajay Kumar Rai, Chandni Menapara","submitted_at":"2021-04-01T12:46:54Z","abstract_excerpt":"The present study is dedicated to light-strange $\\Lambda$ with strangeness S=-1, isospin I=0; $\\Sigma$ with S=-1, I=1 and $\\Xi$ baryon with S=-2 and $I=\\frac{1}{2}$. In this article, hypercentral Constituent Quark Model with linear confining potential has been employed along with first order correction term to obtain the resonance masses for nearly upto 4 GeV. The calculated states include 1S-5S, 1P-4P, 1D-3D, 1F-2F and 1G (in few case) along with all the possible spin-parity assignments. Regge Trajectories have been explored for the linearly of the calculated masses for $(n,M^{2})$ and $(J,M^"},"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":"2104.00439","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2021-04-01T12:46:54Z","cross_cats_sorted":[],"title_canon_sha256":"c9410486aa256c704d9d18536bb1dfb960d72491726937dc815deabeba3fb249","abstract_canon_sha256":"fe81049c80d9f499ec638e5cadd6b29c138696d39a022dd02eee6d861a7f1e8c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:55:13.405582Z","signature_b64":"ZajL6vkGKCQbDHPn04q29b9SC8i6yf8/1F4KgyCjrQa/Qif3IopCmhsAvZdYhl+Yy+dYPFttZKyw9OtgggjnBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1f5c2fdb9956b4fb97ab2c2a47360a85cd4f3410172ebb5c5bd6735669d07eff","last_reissued_at":"2026-07-05T02:55:13.405105Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:55:13.405105Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Spectroscopic Investigation of Light Strange S=-1 $\\Lambda$, $\\Sigma$ and S=-2 $\\Xi$ Baryons","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ajay Kumar Rai, Chandni Menapara","submitted_at":"2021-04-01T12:46:54Z","abstract_excerpt":"The present study is dedicated to light-strange $\\Lambda$ with strangeness S=-1, isospin I=0; $\\Sigma$ with S=-1, I=1 and $\\Xi$ baryon with S=-2 and $I=\\frac{1}{2}$. In this article, hypercentral Constituent Quark Model with linear confining potential has been employed along with first order correction term to obtain the resonance masses for nearly upto 4 GeV. The calculated states include 1S-5S, 1P-4P, 1D-3D, 1F-2F and 1G (in few case) along with all the possible spin-parity assignments. Regge Trajectories have been explored for the linearly of the calculated masses for $(n,M^{2})$ and $(J,M^"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2104.00439","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/2104.00439/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":"2104.00439","created_at":"2026-07-05T02:55:13.405161+00:00"},{"alias_kind":"arxiv_version","alias_value":"2104.00439v1","created_at":"2026-07-05T02:55:13.405161+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2104.00439","created_at":"2026-07-05T02:55:13.405161+00:00"},{"alias_kind":"pith_short_12","alias_value":"D5OC7W4ZK22P","created_at":"2026-07-05T02:55:13.405161+00:00"},{"alias_kind":"pith_short_16","alias_value":"D5OC7W4ZK22PXF5L","created_at":"2026-07-05T02:55:13.405161+00:00"},{"alias_kind":"pith_short_8","alias_value":"D5OC7W4Z","created_at":"2026-07-05T02:55:13.405161+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2603.04141","citing_title":"Experimental Advances on Light Baryon Spectroscopy at BESIII Experiment","ref_index":5,"is_internal_anchor":false},{"citing_arxiv_id":"2603.04141","citing_title":"Experimental Advances on Light Baryon Spectroscopy at BESIII Experiment","ref_index":5,"is_internal_anchor":false},{"citing_arxiv_id":"2604.27028","citing_title":"Observation of a Doubly-strange Hyperon $\\Xi(1720)$ in $J/\\psi\\rightarrow{}K^{-}\\Sigma^0\\bar{\\Xi}^{+}+c.c.$","ref_index":6,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/D5OC7W4ZK22PXF5LFQVEONQKQX","json":"https://pith.science/pith/D5OC7W4ZK22PXF5LFQVEONQKQX.json","graph_json":"https://pith.science/api/pith-number/D5OC7W4ZK22PXF5LFQVEONQKQX/graph.json","events_json":"https://pith.science/api/pith-number/D5OC7W4ZK22PXF5LFQVEONQKQX/events.json","paper":"https://pith.science/paper/D5OC7W4Z"},"agent_actions":{"view_html":"https://pith.science/pith/D5OC7W4ZK22PXF5LFQVEONQKQX","download_json":"https://pith.science/pith/D5OC7W4ZK22PXF5LFQVEONQKQX.json","view_paper":"https://pith.science/paper/D5OC7W4Z","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2104.00439&json=true","fetch_graph":"https://pith.science/api/pith-number/D5OC7W4ZK22PXF5LFQVEONQKQX/graph.json","fetch_events":"https://pith.science/api/pith-number/D5OC7W4ZK22PXF5LFQVEONQKQX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/D5OC7W4ZK22PXF5LFQVEONQKQX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/D5OC7W4ZK22PXF5LFQVEONQKQX/action/storage_attestation","attest_author":"https://pith.science/pith/D5OC7W4ZK22PXF5LFQVEONQKQX/action/author_attestation","sign_citation":"https://pith.science/pith/D5OC7W4ZK22PXF5LFQVEONQKQX/action/citation_signature","submit_replication":"https://pith.science/pith/D5OC7W4ZK22PXF5LFQVEONQKQX/action/replication_record"}},"created_at":"2026-07-05T02:55:13.405161+00:00","updated_at":"2026-07-05T02:55:13.405161+00:00"}