{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:V6XIV6SBHOPCFD4O7KAK6P56AF","short_pith_number":"pith:V6XIV6SB","schema_version":"1.0","canonical_sha256":"afae8afa413b9e228f8efa80af3fbe0158fdee9f5864985ec5eb74a814aa1472","source":{"kind":"arxiv","id":"1407.3684","version":1},"attestation_state":"computed","paper":{"title":"Resolving the puzzling decay patterns of charged $Z_c$ and $Z_b$ states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Li Ma, Li-Ping Sun, Shi-Lin Zhu, Xiang Liu, Xiao-Hai Liu","submitted_at":"2014-07-14T15:01:46Z","abstract_excerpt":"We investigate the ratio of the branching fractions of the molecular candidates decaying into the ground and radially excited states within the quark interchange model. Our numerical results suggest that these molecular candidates are more likely to decay into the radially excited states than into ground states. Especially, the ratio $\\Gamma[Z_c(4430)\\to \\pi\\psi(2S)]$/$\\Gamma[Z_c(4430)\\to \\pi J/\\psi]\\sim 9.8$ is close to the experimental measurement, which supports the interpretation of $Z_c(4430)$ as the $\\bar{D}D^*(2S)$ molecular state. The ratios of the branching fractions of $Z_b(10610)$ a"},"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":"1407.3684","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-14T15:01:46Z","cross_cats_sorted":["hep-ex","nucl-th"],"title_canon_sha256":"bd865a024d2ae6bc86bd7f8a2e8d0a85479d5e8f79b8365105015351393ef360","abstract_canon_sha256":"8f0d84089a13eecd1fd27545bd51e443723616fabc9d5c6278dd0f6edb5bbdd7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:39:47.992269Z","signature_b64":"wyml96D9C3dJvytF0SJa9k5hmMrpn6u4bVgViX6kC/SOAmC8h2UWN1hQn9MaCs4YE7BCmqhY0dZn59wcasvIDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"afae8afa413b9e228f8efa80af3fbe0158fdee9f5864985ec5eb74a814aa1472","last_reissued_at":"2026-05-18T02:39:47.991795Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:39:47.991795Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Resolving the puzzling decay patterns of charged $Z_c$ and $Z_b$ states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Li Ma, Li-Ping Sun, Shi-Lin Zhu, Xiang Liu, Xiao-Hai Liu","submitted_at":"2014-07-14T15:01:46Z","abstract_excerpt":"We investigate the ratio of the branching fractions of the molecular candidates decaying into the ground and radially excited states within the quark interchange model. Our numerical results suggest that these molecular candidates are more likely to decay into the radially excited states than into ground states. Especially, the ratio $\\Gamma[Z_c(4430)\\to \\pi\\psi(2S)]$/$\\Gamma[Z_c(4430)\\to \\pi J/\\psi]\\sim 9.8$ is close to the experimental measurement, which supports the interpretation of $Z_c(4430)$ as the $\\bar{D}D^*(2S)$ molecular state. The ratios of the branching fractions of $Z_b(10610)$ a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.3684","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":""},"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":"1407.3684","created_at":"2026-05-18T02:39:47.991863+00:00"},{"alias_kind":"arxiv_version","alias_value":"1407.3684v1","created_at":"2026-05-18T02:39:47.991863+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.3684","created_at":"2026-05-18T02:39:47.991863+00:00"},{"alias_kind":"pith_short_12","alias_value":"V6XIV6SBHOPC","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_16","alias_value":"V6XIV6SBHOPCFD4O","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_8","alias_value":"V6XIV6SB","created_at":"2026-05-18T12:28:52.271510+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/V6XIV6SBHOPCFD4O7KAK6P56AF","json":"https://pith.science/pith/V6XIV6SBHOPCFD4O7KAK6P56AF.json","graph_json":"https://pith.science/api/pith-number/V6XIV6SBHOPCFD4O7KAK6P56AF/graph.json","events_json":"https://pith.science/api/pith-number/V6XIV6SBHOPCFD4O7KAK6P56AF/events.json","paper":"https://pith.science/paper/V6XIV6SB"},"agent_actions":{"view_html":"https://pith.science/pith/V6XIV6SBHOPCFD4O7KAK6P56AF","download_json":"https://pith.science/pith/V6XIV6SBHOPCFD4O7KAK6P56AF.json","view_paper":"https://pith.science/paper/V6XIV6SB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1407.3684&json=true","fetch_graph":"https://pith.science/api/pith-number/V6XIV6SBHOPCFD4O7KAK6P56AF/graph.json","fetch_events":"https://pith.science/api/pith-number/V6XIV6SBHOPCFD4O7KAK6P56AF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/V6XIV6SBHOPCFD4O7KAK6P56AF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/V6XIV6SBHOPCFD4O7KAK6P56AF/action/storage_attestation","attest_author":"https://pith.science/pith/V6XIV6SBHOPCFD4O7KAK6P56AF/action/author_attestation","sign_citation":"https://pith.science/pith/V6XIV6SBHOPCFD4O7KAK6P56AF/action/citation_signature","submit_replication":"https://pith.science/pith/V6XIV6SBHOPCFD4O7KAK6P56AF/action/replication_record"}},"created_at":"2026-05-18T02:39:47.991863+00:00","updated_at":"2026-05-18T02:39:47.991863+00:00"}