{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:XGAJKEGHRSAOKKOFI73UNR4RJ4","short_pith_number":"pith:XGAJKEGH","schema_version":"1.0","canonical_sha256":"b9809510c78c80e529c547f746c7914f31914bf9e15b342d211526b7acf535d1","source":{"kind":"arxiv","id":"2402.03057","version":3},"attestation_state":"computed","paper":{"title":"How many vector charmonium(-like) states sit in the energy range from $4.2$ to $4.35$ GeV?","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Christoph Hanhart, Daniel Winney, Leon von Detten, Qiang Zhao, Qian Wang, Vadim Baru","submitted_at":"2024-02-05T14:45:07Z","abstract_excerpt":"In recent years many vector charmonium(-like) states were reported by different electron-positron collider experiments above $4.2$ GeV. However, so far, there not only exists sizable tension in the parameters of those states, but there is also no consensus on the number of the vector states in this energy range. To some extend, this might be caused by the fact that the experimental data were typically analyzed in single channel analyses employing overlapping Breit-Wigner functions, in particular ignoring the effect of opening thresholds. In this study, we focus on the mass range between $4.2$ "},"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":"2402.03057","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-02-05T14:45:07Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"920f5a0659935b0044ff11fa3c5eed230d5c8f18d696f4d8c47b87fbc06ff680","abstract_canon_sha256":"857f36a44a509c7e4ea35e68808bebf808ac29c0b1f69c6ec72c2a183eb4c9e4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:36:22.152348Z","signature_b64":"2t+tCtc+ItG13zvde2faaEcEGT0ry8bVDhUsoFpnV2HXJHvqTnHCMr9ALIxYUIM6dP6e4xGXJkLUcTpNn0cRBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b9809510c78c80e529c547f746c7914f31914bf9e15b342d211526b7acf535d1","last_reissued_at":"2026-07-05T08:36:22.151912Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:36:22.151912Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"How many vector charmonium(-like) states sit in the energy range from $4.2$ to $4.35$ GeV?","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Christoph Hanhart, Daniel Winney, Leon von Detten, Qiang Zhao, Qian Wang, Vadim Baru","submitted_at":"2024-02-05T14:45:07Z","abstract_excerpt":"In recent years many vector charmonium(-like) states were reported by different electron-positron collider experiments above $4.2$ GeV. However, so far, there not only exists sizable tension in the parameters of those states, but there is also no consensus on the number of the vector states in this energy range. To some extend, this might be caused by the fact that the experimental data were typically analyzed in single channel analyses employing overlapping Breit-Wigner functions, in particular ignoring the effect of opening thresholds. In this study, we focus on the mass range between $4.2$ "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2402.03057","kind":"arxiv","version":3},"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/2402.03057/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":"2402.03057","created_at":"2026-07-05T08:36:22.151965+00:00"},{"alias_kind":"arxiv_version","alias_value":"2402.03057v3","created_at":"2026-07-05T08:36:22.151965+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2402.03057","created_at":"2026-07-05T08:36:22.151965+00:00"},{"alias_kind":"pith_short_12","alias_value":"XGAJKEGHRSAO","created_at":"2026-07-05T08:36:22.151965+00:00"},{"alias_kind":"pith_short_16","alias_value":"XGAJKEGHRSAOKKOF","created_at":"2026-07-05T08:36:22.151965+00:00"},{"alias_kind":"pith_short_8","alias_value":"XGAJKEGH","created_at":"2026-07-05T08:36:22.151965+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.07225","citing_title":"Simultaneous Dalitz-plot decomposition of the $e^+ e^- \\to J/\\psi \\, \\pi \\, \\pi \\, (K \\bar{K})$ processes in the 4.13-4.36 GeV region using dispersive final-state interactions","ref_index":46,"is_internal_anchor":false},{"citing_arxiv_id":"2606.06180","citing_title":"Vector charmonium(-like) states in the energy range of 4.1-4.6 GeV","ref_index":73,"is_internal_anchor":false},{"citing_arxiv_id":"2604.25607","citing_title":"Determination of the $Z_c(3900)$ and the $Z_{cs}(3985)$ states from joint analysis of experimental and lattice data","ref_index":40,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XGAJKEGHRSAOKKOFI73UNR4RJ4","json":"https://pith.science/pith/XGAJKEGHRSAOKKOFI73UNR4RJ4.json","graph_json":"https://pith.science/api/pith-number/XGAJKEGHRSAOKKOFI73UNR4RJ4/graph.json","events_json":"https://pith.science/api/pith-number/XGAJKEGHRSAOKKOFI73UNR4RJ4/events.json","paper":"https://pith.science/paper/XGAJKEGH"},"agent_actions":{"view_html":"https://pith.science/pith/XGAJKEGHRSAOKKOFI73UNR4RJ4","download_json":"https://pith.science/pith/XGAJKEGHRSAOKKOFI73UNR4RJ4.json","view_paper":"https://pith.science/paper/XGAJKEGH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2402.03057&json=true","fetch_graph":"https://pith.science/api/pith-number/XGAJKEGHRSAOKKOFI73UNR4RJ4/graph.json","fetch_events":"https://pith.science/api/pith-number/XGAJKEGHRSAOKKOFI73UNR4RJ4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XGAJKEGHRSAOKKOFI73UNR4RJ4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XGAJKEGHRSAOKKOFI73UNR4RJ4/action/storage_attestation","attest_author":"https://pith.science/pith/XGAJKEGHRSAOKKOFI73UNR4RJ4/action/author_attestation","sign_citation":"https://pith.science/pith/XGAJKEGHRSAOKKOFI73UNR4RJ4/action/citation_signature","submit_replication":"https://pith.science/pith/XGAJKEGHRSAOKKOFI73UNR4RJ4/action/replication_record"}},"created_at":"2026-07-05T08:36:22.151965+00:00","updated_at":"2026-07-05T08:36:22.151965+00:00"}