{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:XKDJH2DKIGVLDKWMMT4B6UAH6A","short_pith_number":"pith:XKDJH2DK","schema_version":"1.0","canonical_sha256":"ba8693e86a41aab1aacc64f81f5007f03100e9df79536da6f0a2d231e069da52","source":{"kind":"arxiv","id":"hep-ph/0604252","version":2},"attestation_state":"computed","paper":{"title":"Chromo-polarizability and pipi final state interaction","license":"","headline":"","cross_cats":["hep-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Feng-Kun Guo, Huan-Ching Chiang, Peng-Nian Shen","submitted_at":"2006-04-27T19:13:52Z","abstract_excerpt":"The chromo-polarizability of a quarkonium state is a measure of the amplitude of the $E1$-$E1$ chromo-electric interaction of the quarkonium with soft gluon fields and can be measured in the heavy quarkonium decays. Based on the chiral unitary approach, formulas with modification caused by the $S$ wave $\\pi\\pi$ final state interaction (FSI) for measuring the chromo-polarizabilities are given. It is shown that the effect of the $S$ wave $\\pi\\pi$ FSI is very important in extracting chromo-polarizabilities from the experimental data. The resultant values with the FSI are reduced to about 1/3 of t"},"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":"hep-ph/0604252","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2006-04-27T19:13:52Z","cross_cats_sorted":["hep-ex","nucl-th"],"title_canon_sha256":"c58f168f10ca1c7b67fb0dee69f2e568c6dcabfcd51ec10baee3b5e06b7931c1","abstract_canon_sha256":"0d5935eb21b902e2cbfdc413dc41d9041714e5dacd094c83eab6ff2ca3ecb480"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:19:52.033590Z","signature_b64":"KnscTQL1obofeIO8vJmMqCj/co2ZPo7lcAbijkabU77wsZKf+DIXT3Hu9nU8PJyHD3B8PJUQAARTEOMaKkkrAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ba8693e86a41aab1aacc64f81f5007f03100e9df79536da6f0a2d231e069da52","last_reissued_at":"2026-07-04T15:19:52.033161Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:19:52.033161Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Chromo-polarizability and pipi final state interaction","license":"","headline":"","cross_cats":["hep-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Feng-Kun Guo, Huan-Ching Chiang, Peng-Nian Shen","submitted_at":"2006-04-27T19:13:52Z","abstract_excerpt":"The chromo-polarizability of a quarkonium state is a measure of the amplitude of the $E1$-$E1$ chromo-electric interaction of the quarkonium with soft gluon fields and can be measured in the heavy quarkonium decays. Based on the chiral unitary approach, formulas with modification caused by the $S$ wave $\\pi\\pi$ final state interaction (FSI) for measuring the chromo-polarizabilities are given. It is shown that the effect of the $S$ wave $\\pi\\pi$ FSI is very important in extracting chromo-polarizabilities from the experimental data. The resultant values with the FSI are reduced to about 1/3 of t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0604252","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/0604252/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"hep-ph/0604252","created_at":"2026-07-04T15:19:52.033222+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0604252v2","created_at":"2026-07-04T15:19:52.033222+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0604252","created_at":"2026-07-04T15:19:52.033222+00:00"},{"alias_kind":"pith_short_12","alias_value":"XKDJH2DKIGVL","created_at":"2026-07-04T15:19:52.033222+00:00"},{"alias_kind":"pith_short_16","alias_value":"XKDJH2DKIGVLDKWM","created_at":"2026-07-04T15:19:52.033222+00:00"},{"alias_kind":"pith_short_8","alias_value":"XKDJH2DK","created_at":"2026-07-04T15:19:52.033222+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2608.00611","citing_title":"Complex chromoelectric polarizability of a heavy-quarkonium resonance: pole definition and channel-complete pNRQCD matching","ref_index":9,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XKDJH2DKIGVLDKWMMT4B6UAH6A","json":"https://pith.science/pith/XKDJH2DKIGVLDKWMMT4B6UAH6A.json","graph_json":"https://pith.science/api/pith-number/XKDJH2DKIGVLDKWMMT4B6UAH6A/graph.json","events_json":"https://pith.science/api/pith-number/XKDJH2DKIGVLDKWMMT4B6UAH6A/events.json","paper":"https://pith.science/paper/XKDJH2DK"},"agent_actions":{"view_html":"https://pith.science/pith/XKDJH2DKIGVLDKWMMT4B6UAH6A","download_json":"https://pith.science/pith/XKDJH2DKIGVLDKWMMT4B6UAH6A.json","view_paper":"https://pith.science/paper/XKDJH2DK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0604252&json=true","fetch_graph":"https://pith.science/api/pith-number/XKDJH2DKIGVLDKWMMT4B6UAH6A/graph.json","fetch_events":"https://pith.science/api/pith-number/XKDJH2DKIGVLDKWMMT4B6UAH6A/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XKDJH2DKIGVLDKWMMT4B6UAH6A/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XKDJH2DKIGVLDKWMMT4B6UAH6A/action/storage_attestation","attest_author":"https://pith.science/pith/XKDJH2DKIGVLDKWMMT4B6UAH6A/action/author_attestation","sign_citation":"https://pith.science/pith/XKDJH2DKIGVLDKWMMT4B6UAH6A/action/citation_signature","submit_replication":"https://pith.science/pith/XKDJH2DKIGVLDKWMMT4B6UAH6A/action/replication_record"}},"created_at":"2026-07-04T15:19:52.033222+00:00","updated_at":"2026-07-04T15:19:52.033222+00:00"}