{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:GHTJLSHHQTDZTEWVRJ6SY5HAK4","short_pith_number":"pith:GHTJLSHH","schema_version":"1.0","canonical_sha256":"31e695c8e784c79992d58a7d2c74e05712a3ff92f43aab5182f940b673a8ad69","source":{"kind":"arxiv","id":"2011.03448","version":1},"attestation_state":"computed","paper":{"title":"Partial decay widths of $\\phi(2170)$ to kaonic resonances","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"A. Martinez Torres, Brenda B. Malabarba, K. P. Khemchandani, Xiu-Lei Ren","submitted_at":"2020-11-06T15:56:28Z","abstract_excerpt":"In this work we study the strong decays of $\\phi(2170)$ to final states involving the kaonic resonances $K(1460)$, $K_1(1270)$ and $K_1(1400)$, on which experimental data have recently been extracted by the BESIII Collaboration. The formalism developed here is based on interpreting $\\phi(2170)$ and $K(1460)$ as states arising from three-hadron dynamics, which is inspired by our earlier works. For $K_1(1270)$ and $K_1(1400)$ we investigate different descriptions, such as a mixture of states belonging to the nonet of axial resonances, or the former one as a state originating from the vector-pseu"},"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":"2011.03448","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-11-06T15:56:28Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"ac58262ba7891cd64004c9c3581756d1a653db99ea8b0901f16c07b233f89a7e","abstract_canon_sha256":"82dd5ff2ceb74be381f89340a1ecc4e8a482f965c7b1f2e9bb0a844bef7296d6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:12:11.825514Z","signature_b64":"FJHnxQlRbsmysV2JCLR2PGOHZ7V4uPsTomUsjyJuJJj7LS3wcQ+wEWKf0r1KSGh0+zAt2FB1iullDopTrqiVDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"31e695c8e784c79992d58a7d2c74e05712a3ff92f43aab5182f940b673a8ad69","last_reissued_at":"2026-07-05T02:12:11.825025Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:12:11.825025Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Partial decay widths of $\\phi(2170)$ to kaonic resonances","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"A. Martinez Torres, Brenda B. Malabarba, K. P. Khemchandani, Xiu-Lei Ren","submitted_at":"2020-11-06T15:56:28Z","abstract_excerpt":"In this work we study the strong decays of $\\phi(2170)$ to final states involving the kaonic resonances $K(1460)$, $K_1(1270)$ and $K_1(1400)$, on which experimental data have recently been extracted by the BESIII Collaboration. The formalism developed here is based on interpreting $\\phi(2170)$ and $K(1460)$ as states arising from three-hadron dynamics, which is inspired by our earlier works. For $K_1(1270)$ and $K_1(1400)$ we investigate different descriptions, such as a mixture of states belonging to the nonet of axial resonances, or the former one as a state originating from the vector-pseu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2011.03448","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/2011.03448/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":"2011.03448","created_at":"2026-07-05T02:12:11.825084+00:00"},{"alias_kind":"arxiv_version","alias_value":"2011.03448v1","created_at":"2026-07-05T02:12:11.825084+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2011.03448","created_at":"2026-07-05T02:12:11.825084+00:00"},{"alias_kind":"pith_short_12","alias_value":"GHTJLSHHQTDZ","created_at":"2026-07-05T02:12:11.825084+00:00"},{"alias_kind":"pith_short_16","alias_value":"GHTJLSHHQTDZTEWV","created_at":"2026-07-05T02:12:11.825084+00:00"},{"alias_kind":"pith_short_8","alias_value":"GHTJLSHH","created_at":"2026-07-05T02:12:11.825084+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2512.24370","citing_title":"$D^*\\pi$ interaction from the lineshape of $D_1(2420)$ in $B$-decays","ref_index":24,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GHTJLSHHQTDZTEWVRJ6SY5HAK4","json":"https://pith.science/pith/GHTJLSHHQTDZTEWVRJ6SY5HAK4.json","graph_json":"https://pith.science/api/pith-number/GHTJLSHHQTDZTEWVRJ6SY5HAK4/graph.json","events_json":"https://pith.science/api/pith-number/GHTJLSHHQTDZTEWVRJ6SY5HAK4/events.json","paper":"https://pith.science/paper/GHTJLSHH"},"agent_actions":{"view_html":"https://pith.science/pith/GHTJLSHHQTDZTEWVRJ6SY5HAK4","download_json":"https://pith.science/pith/GHTJLSHHQTDZTEWVRJ6SY5HAK4.json","view_paper":"https://pith.science/paper/GHTJLSHH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2011.03448&json=true","fetch_graph":"https://pith.science/api/pith-number/GHTJLSHHQTDZTEWVRJ6SY5HAK4/graph.json","fetch_events":"https://pith.science/api/pith-number/GHTJLSHHQTDZTEWVRJ6SY5HAK4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GHTJLSHHQTDZTEWVRJ6SY5HAK4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GHTJLSHHQTDZTEWVRJ6SY5HAK4/action/storage_attestation","attest_author":"https://pith.science/pith/GHTJLSHHQTDZTEWVRJ6SY5HAK4/action/author_attestation","sign_citation":"https://pith.science/pith/GHTJLSHHQTDZTEWVRJ6SY5HAK4/action/citation_signature","submit_replication":"https://pith.science/pith/GHTJLSHHQTDZTEWVRJ6SY5HAK4/action/replication_record"}},"created_at":"2026-07-05T02:12:11.825084+00:00","updated_at":"2026-07-05T02:12:11.825084+00:00"}