{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:LQB6TXBZUDAI4RL3QM52RCCOJR","short_pith_number":"pith:LQB6TXBZ","schema_version":"1.0","canonical_sha256":"5c03e9dc39a0c08e457b833ba8884e4c5e9b74aa64bb0a8570764a2dec3d525f","source":{"kind":"arxiv","id":"1008.4083","version":4},"attestation_state":"computed","paper":{"title":"Relative phases in Dalitz plot amplitudes for $D^0 \\to K_S \\pi^+ \\pi^-$ and $D^0 \\to \\pi^0 K^+ K^-$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Bhubanjyoti Bhattacharya, Jonathan L. Rosner","submitted_at":"2010-08-24T16:20:09Z","abstract_excerpt":"Relative phases of amplitudes for $D$ meson decays to a light pseudoscalar meson $P$ and a light vector meson $V$ decaying to two pseudoscalar mesons will lead to characteristic interferences on the three-body Dalitz plot. These phases may be compared with predictions of a flavor-symmetric treatment which extracts contributing amplitudes and their relative phases from a fit to $D \\to PV$ decay rates. Good agreement was found previously for the cases of $D^0 \\to K^- \\pi^+ \\pi^0$ and $D^0 \\to \\pi^+ \\pi^- \\pi^0$. The present work is devoted to the decays $D^0 \\to K_S \\pi^+ \\pi^-$ and $D^0 \\to \\pi"},"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":"1008.4083","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-08-24T16:20:09Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"daa572e08b753d4a03772648396da7f1304b425c7c731c1701be7b3644baa687","abstract_canon_sha256":"61f62ada662565e8bdc94f79473eee994264c58c2d8bc4d4ee5ca18d5d253a1d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:36:33.084798Z","signature_b64":"68QuHvCQMX/oDg/LUXn5xZ6adKCY8Mih2ZGzSivCIMoyehwmyILTuIw1ZcO/3H7jTTlYdp3HyhHokabVY/3xDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5c03e9dc39a0c08e457b833ba8884e4c5e9b74aa64bb0a8570764a2dec3d525f","last_reissued_at":"2026-05-18T04:36:33.084345Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:36:33.084345Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Relative phases in Dalitz plot amplitudes for $D^0 \\to K_S \\pi^+ \\pi^-$ and $D^0 \\to \\pi^0 K^+ K^-$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Bhubanjyoti Bhattacharya, Jonathan L. Rosner","submitted_at":"2010-08-24T16:20:09Z","abstract_excerpt":"Relative phases of amplitudes for $D$ meson decays to a light pseudoscalar meson $P$ and a light vector meson $V$ decaying to two pseudoscalar mesons will lead to characteristic interferences on the three-body Dalitz plot. These phases may be compared with predictions of a flavor-symmetric treatment which extracts contributing amplitudes and their relative phases from a fit to $D \\to PV$ decay rates. Good agreement was found previously for the cases of $D^0 \\to K^- \\pi^+ \\pi^0$ and $D^0 \\to \\pi^+ \\pi^- \\pi^0$. The present work is devoted to the decays $D^0 \\to K_S \\pi^+ \\pi^-$ and $D^0 \\to \\pi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1008.4083","kind":"arxiv","version":4},"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":"1008.4083","created_at":"2026-05-18T04:36:33.084414+00:00"},{"alias_kind":"arxiv_version","alias_value":"1008.4083v4","created_at":"2026-05-18T04:36:33.084414+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1008.4083","created_at":"2026-05-18T04:36:33.084414+00:00"},{"alias_kind":"pith_short_12","alias_value":"LQB6TXBZUDAI","created_at":"2026-05-18T12:26:10.704358+00:00"},{"alias_kind":"pith_short_16","alias_value":"LQB6TXBZUDAI4RL3","created_at":"2026-05-18T12:26:10.704358+00:00"},{"alias_kind":"pith_short_8","alias_value":"LQB6TXBZ","created_at":"2026-05-18T12:26:10.704358+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/LQB6TXBZUDAI4RL3QM52RCCOJR","json":"https://pith.science/pith/LQB6TXBZUDAI4RL3QM52RCCOJR.json","graph_json":"https://pith.science/api/pith-number/LQB6TXBZUDAI4RL3QM52RCCOJR/graph.json","events_json":"https://pith.science/api/pith-number/LQB6TXBZUDAI4RL3QM52RCCOJR/events.json","paper":"https://pith.science/paper/LQB6TXBZ"},"agent_actions":{"view_html":"https://pith.science/pith/LQB6TXBZUDAI4RL3QM52RCCOJR","download_json":"https://pith.science/pith/LQB6TXBZUDAI4RL3QM52RCCOJR.json","view_paper":"https://pith.science/paper/LQB6TXBZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1008.4083&json=true","fetch_graph":"https://pith.science/api/pith-number/LQB6TXBZUDAI4RL3QM52RCCOJR/graph.json","fetch_events":"https://pith.science/api/pith-number/LQB6TXBZUDAI4RL3QM52RCCOJR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LQB6TXBZUDAI4RL3QM52RCCOJR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LQB6TXBZUDAI4RL3QM52RCCOJR/action/storage_attestation","attest_author":"https://pith.science/pith/LQB6TXBZUDAI4RL3QM52RCCOJR/action/author_attestation","sign_citation":"https://pith.science/pith/LQB6TXBZUDAI4RL3QM52RCCOJR/action/citation_signature","submit_replication":"https://pith.science/pith/LQB6TXBZUDAI4RL3QM52RCCOJR/action/replication_record"}},"created_at":"2026-05-18T04:36:33.084414+00:00","updated_at":"2026-05-18T04:36:33.084414+00:00"}