{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:XFT4FZYMSQYJXU2ERCMKGWOULF","short_pith_number":"pith:XFT4FZYM","schema_version":"1.0","canonical_sha256":"b967c2e70c94309bd3448898a359d4596bef1b8b5fdb1a1e843e56a39b3697f5","source":{"kind":"arxiv","id":"1710.00685","version":2},"attestation_state":"computed","paper":{"title":"Effect of the $K\\overline{K}$ and $\\eta\\eta$ channels and interference phenomena in the two-pion and $K\\overline{K}$ transitions of charmonia and bottomonia","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Miroslav Nagy, Petr Byd\\v{z}ovsk\\'y, Robert Kami\\'nski, Thomas Gutsche, Valery E. Lyubovitskij, Yury S. Surovtsev","submitted_at":"2017-10-02T14:25:10Z","abstract_excerpt":"It is shown that the basic shape of dipion and $K\\overline{K}$ mass spectra in decays $J/\\psi\\to\\phi(\\pi\\pi,K\\overline{K})$, $\\psi(2S)\\to J/\\psi\\,\\pi\\pi$, $Y(4260)\\to J/\\phi~\\pi\\pi$ and in the two-pion transitions of bottomonia states are explained by an unified mechanism based on the contribution of the $\\pi\\pi$, $K\\overline{K}$ and $\\eta\\eta$ coupled channels including their interference. The role of the individual $f_0$ resonances in making up the shape of the dipion mass distributions in the charmonia and bottomonia decays is considered."},"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":"1710.00685","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-10-02T14:25:10Z","cross_cats_sorted":[],"title_canon_sha256":"60e91ae6dc173ef02141b5999f385e94c1da750c07ab0ffc91190bb365bcb9c2","abstract_canon_sha256":"8992258bff2287e99fed31970266435b6972a35107db0d2d1e15db1b829737e0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:23:45.359265Z","signature_b64":"T3XlSpHXe8CsfWSB6Llb3uc36xNt4oWqC7Pp937HxzUCAh20q+5aN0vZSZ81FJSELCmBRFplFjFvGoJwOz9RDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b967c2e70c94309bd3448898a359d4596bef1b8b5fdb1a1e843e56a39b3697f5","last_reissued_at":"2026-05-18T00:23:45.358589Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:23:45.358589Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effect of the $K\\overline{K}$ and $\\eta\\eta$ channels and interference phenomena in the two-pion and $K\\overline{K}$ transitions of charmonia and bottomonia","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Miroslav Nagy, Petr Byd\\v{z}ovsk\\'y, Robert Kami\\'nski, Thomas Gutsche, Valery E. Lyubovitskij, Yury S. Surovtsev","submitted_at":"2017-10-02T14:25:10Z","abstract_excerpt":"It is shown that the basic shape of dipion and $K\\overline{K}$ mass spectra in decays $J/\\psi\\to\\phi(\\pi\\pi,K\\overline{K})$, $\\psi(2S)\\to J/\\psi\\,\\pi\\pi$, $Y(4260)\\to J/\\phi~\\pi\\pi$ and in the two-pion transitions of bottomonia states are explained by an unified mechanism based on the contribution of the $\\pi\\pi$, $K\\overline{K}$ and $\\eta\\eta$ coupled channels including their interference. The role of the individual $f_0$ resonances in making up the shape of the dipion mass distributions in the charmonia and bottomonia decays is considered."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.00685","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":"1710.00685","created_at":"2026-05-18T00:23:45.358682+00:00"},{"alias_kind":"arxiv_version","alias_value":"1710.00685v2","created_at":"2026-05-18T00:23:45.358682+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.00685","created_at":"2026-05-18T00:23:45.358682+00:00"},{"alias_kind":"pith_short_12","alias_value":"XFT4FZYMSQYJ","created_at":"2026-05-18T12:31:53.515858+00:00"},{"alias_kind":"pith_short_16","alias_value":"XFT4FZYMSQYJXU2E","created_at":"2026-05-18T12:31:53.515858+00:00"},{"alias_kind":"pith_short_8","alias_value":"XFT4FZYM","created_at":"2026-05-18T12:31:53.515858+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/XFT4FZYMSQYJXU2ERCMKGWOULF","json":"https://pith.science/pith/XFT4FZYMSQYJXU2ERCMKGWOULF.json","graph_json":"https://pith.science/api/pith-number/XFT4FZYMSQYJXU2ERCMKGWOULF/graph.json","events_json":"https://pith.science/api/pith-number/XFT4FZYMSQYJXU2ERCMKGWOULF/events.json","paper":"https://pith.science/paper/XFT4FZYM"},"agent_actions":{"view_html":"https://pith.science/pith/XFT4FZYMSQYJXU2ERCMKGWOULF","download_json":"https://pith.science/pith/XFT4FZYMSQYJXU2ERCMKGWOULF.json","view_paper":"https://pith.science/paper/XFT4FZYM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1710.00685&json=true","fetch_graph":"https://pith.science/api/pith-number/XFT4FZYMSQYJXU2ERCMKGWOULF/graph.json","fetch_events":"https://pith.science/api/pith-number/XFT4FZYMSQYJXU2ERCMKGWOULF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XFT4FZYMSQYJXU2ERCMKGWOULF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XFT4FZYMSQYJXU2ERCMKGWOULF/action/storage_attestation","attest_author":"https://pith.science/pith/XFT4FZYMSQYJXU2ERCMKGWOULF/action/author_attestation","sign_citation":"https://pith.science/pith/XFT4FZYMSQYJXU2ERCMKGWOULF/action/citation_signature","submit_replication":"https://pith.science/pith/XFT4FZYMSQYJXU2ERCMKGWOULF/action/replication_record"}},"created_at":"2026-05-18T00:23:45.358682+00:00","updated_at":"2026-05-18T00:23:45.358682+00:00"}