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We use both the tensor current $\\bar\\psi\\sigma_{\\mu\\nu}\\psi$ and the derivative current $\\bar{\\psi}\\overleftrightarrow{D}_\\mu\\gamma_5\\psi$ as interpolating currents to calculate the partial decay width of the $b_1\\pi$ decay mode. Comparing the sum rules obtained by using different currents, we obtain $\\Gamma(\\pi_1\\to b_1\\pi)$ = 8--23, 32--86 and 52--151\\,MeV for $m_{1^{-+}}$ = 1.6, 1.8 and 2.0\\,GeV respectively, which favour the results from the flux tube models "},"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":"1608.03028","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-08-10T02:20:02Z","cross_cats_sorted":[],"title_canon_sha256":"acd8bc9aa321ee3eeb36bfc1cd2b8e6c575f197ff7b118e4fed322b22c1625b2","abstract_canon_sha256":"33ae5e53209ee7617e143148f6ede3d4773f10939ad3099cf3fb74b79450cf9a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:03:17.637232Z","signature_b64":"qgMIlaXCN6BuQTaNBG0Qw5Wn03Unw0NDMnKml3mvMRrRWCbIc2NvCMmXA8xfhq7z/AkhDbOn8TX24wexi7RLBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2bc6fc3a89ee86538bbdd1e3556fe4bcb7520a9faa0e9635facad487049b2512","last_reissued_at":"2026-05-18T01:03:17.636542Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:03:17.636542Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Revisiting the b1 pi and rho pi decay modes of the 1-+ light hybrid state with light-cone QCD sum rules","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hong Ying Jin, T.G. 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Comparing the sum rules obtained by using different currents, we obtain $\\Gamma(\\pi_1\\to b_1\\pi)$ = 8--23, 32--86 and 52--151\\,MeV for $m_{1^{-+}}$ = 1.6, 1.8 and 2.0\\,GeV respectively, which favour the results from the flux tube models "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.03028","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":"1608.03028","created_at":"2026-05-18T01:03:17.636648+00:00"},{"alias_kind":"arxiv_version","alias_value":"1608.03028v2","created_at":"2026-05-18T01:03:17.636648+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.03028","created_at":"2026-05-18T01:03:17.636648+00:00"},{"alias_kind":"pith_short_12","alias_value":"FPDPYOUJ52DF","created_at":"2026-05-18T12:30:15.759754+00:00"},{"alias_kind":"pith_short_16","alias_value":"FPDPYOUJ52DFHC55","created_at":"2026-05-18T12:30:15.759754+00:00"},{"alias_kind":"pith_short_8","alias_value":"FPDPYOUJ","created_at":"2026-05-18T12:30:15.759754+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2511.22111","citing_title":"Systematic study of exotic $1^{-+}$ tetraquark spectroscopy","ref_index":37,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FPDPYOUJ52DFHC552HRVK37EXS","json":"https://pith.science/pith/FPDPYOUJ52DFHC552HRVK37EXS.json","graph_json":"https://pith.science/api/pith-number/FPDPYOUJ52DFHC552HRVK37EXS/graph.json","events_json":"https://pith.science/api/pith-number/FPDPYOUJ52DFHC552HRVK37EXS/events.json","paper":"https://pith.science/paper/FPDPYOUJ"},"agent_actions":{"view_html":"https://pith.science/pith/FPDPYOUJ52DFHC552HRVK37EXS","download_json":"https://pith.science/pith/FPDPYOUJ52DFHC552HRVK37EXS.json","view_paper":"https://pith.science/paper/FPDPYOUJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1608.03028&json=true","fetch_graph":"https://pith.science/api/pith-number/FPDPYOUJ52DFHC552HRVK37EXS/graph.json","fetch_events":"https://pith.science/api/pith-number/FPDPYOUJ52DFHC552HRVK37EXS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FPDPYOUJ52DFHC552HRVK37EXS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FPDPYOUJ52DFHC552HRVK37EXS/action/storage_attestation","attest_author":"https://pith.science/pith/FPDPYOUJ52DFHC552HRVK37EXS/action/author_attestation","sign_citation":"https://pith.science/pith/FPDPYOUJ52DFHC552HRVK37EXS/action/citation_signature","submit_replication":"https://pith.science/pith/FPDPYOUJ52DFHC552HRVK37EXS/action/replication_record"}},"created_at":"2026-05-18T01:03:17.636648+00:00","updated_at":"2026-05-18T01:03:17.636648+00:00"}