{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:FTTSOLMHZMASYBUO4W4WD3U7T5","short_pith_number":"pith:FTTSOLMH","schema_version":"1.0","canonical_sha256":"2ce7272d87cb012c068ee5b961ee9f9f5e16db3731b4850b340998fb888631bd","source":{"kind":"arxiv","id":"1709.10233","version":1},"attestation_state":"computed","paper":{"title":"The Mass and Decay Properties of the $1^{-+}$ Light Hybrid Meson","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hong-Ying Jin, T.G. Steele, Zhu-feng Zhang, Zhuo-Ran Huang","submitted_at":"2017-09-29T04:23:42Z","abstract_excerpt":"We calculate the complete form of the dimension-8 condensate contributions in the two-point correlator of the ($1^{-+}$,$0^{++}$) light hybrid current considering the operator mixing under renormalization. We find the inclusion these higher power corrections as well as the update of $\\langle g^3G^3\\rangle$ increase the QCD sum rule mass prediction for the $1^{-+}$ light hybrid. The obtained conservative mass range 1.72--2.60 GeV does not favor the $\\pi_1(1400)$ and the $\\pi_1(1600)$ to be pure hybrid states and suggests the $\\pi_1(2015)$ observed by E852 is more likely to have much of a hybrid"},"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":"1709.10233","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-09-29T04:23:42Z","cross_cats_sorted":[],"title_canon_sha256":"c6d77041a43c56ae6d824af9559d89a3b175eadcff97e0ccc57f7d85df2c9a28","abstract_canon_sha256":"e9b86399e62dd4d7159f8f3d0bae37dce19538d39ac24fdec406b69b2fce6dd1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:34:03.843990Z","signature_b64":"1gOAQvQ1r0YqS+QaWon8dpV7gVjMDfeN6My0ZBrVi4la7DcytkDZm75ICe8a7j/pEE96/hDKhmFRmyqjfpzxAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2ce7272d87cb012c068ee5b961ee9f9f5e16db3731b4850b340998fb888631bd","last_reissued_at":"2026-05-18T00:34:03.843262Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:34:03.843262Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Mass and Decay Properties of the $1^{-+}$ Light Hybrid Meson","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hong-Ying Jin, T.G. Steele, Zhu-feng Zhang, Zhuo-Ran Huang","submitted_at":"2017-09-29T04:23:42Z","abstract_excerpt":"We calculate the complete form of the dimension-8 condensate contributions in the two-point correlator of the ($1^{-+}$,$0^{++}$) light hybrid current considering the operator mixing under renormalization. We find the inclusion these higher power corrections as well as the update of $\\langle g^3G^3\\rangle$ increase the QCD sum rule mass prediction for the $1^{-+}$ light hybrid. The obtained conservative mass range 1.72--2.60 GeV does not favor the $\\pi_1(1400)$ and the $\\pi_1(1600)$ to be pure hybrid states and suggests the $\\pi_1(2015)$ observed by E852 is more likely to have much of a hybrid"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.10233","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":"1709.10233","created_at":"2026-05-18T00:34:03.843391+00:00"},{"alias_kind":"arxiv_version","alias_value":"1709.10233v1","created_at":"2026-05-18T00:34:03.843391+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.10233","created_at":"2026-05-18T00:34:03.843391+00:00"},{"alias_kind":"pith_short_12","alias_value":"FTTSOLMHZMAS","created_at":"2026-05-18T12:31:15.632608+00:00"},{"alias_kind":"pith_short_16","alias_value":"FTTSOLMHZMASYBUO","created_at":"2026-05-18T12:31:15.632608+00:00"},{"alias_kind":"pith_short_8","alias_value":"FTTSOLMH","created_at":"2026-05-18T12:31:15.632608+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/FTTSOLMHZMASYBUO4W4WD3U7T5","json":"https://pith.science/pith/FTTSOLMHZMASYBUO4W4WD3U7T5.json","graph_json":"https://pith.science/api/pith-number/FTTSOLMHZMASYBUO4W4WD3U7T5/graph.json","events_json":"https://pith.science/api/pith-number/FTTSOLMHZMASYBUO4W4WD3U7T5/events.json","paper":"https://pith.science/paper/FTTSOLMH"},"agent_actions":{"view_html":"https://pith.science/pith/FTTSOLMHZMASYBUO4W4WD3U7T5","download_json":"https://pith.science/pith/FTTSOLMHZMASYBUO4W4WD3U7T5.json","view_paper":"https://pith.science/paper/FTTSOLMH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1709.10233&json=true","fetch_graph":"https://pith.science/api/pith-number/FTTSOLMHZMASYBUO4W4WD3U7T5/graph.json","fetch_events":"https://pith.science/api/pith-number/FTTSOLMHZMASYBUO4W4WD3U7T5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FTTSOLMHZMASYBUO4W4WD3U7T5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FTTSOLMHZMASYBUO4W4WD3U7T5/action/storage_attestation","attest_author":"https://pith.science/pith/FTTSOLMHZMASYBUO4W4WD3U7T5/action/author_attestation","sign_citation":"https://pith.science/pith/FTTSOLMHZMASYBUO4W4WD3U7T5/action/citation_signature","submit_replication":"https://pith.science/pith/FTTSOLMHZMASYBUO4W4WD3U7T5/action/replication_record"}},"created_at":"2026-05-18T00:34:03.843391+00:00","updated_at":"2026-05-18T00:34:03.843391+00:00"}