{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:AAYH26VEGSFXN65PBZUIWDIVWZ","short_pith_number":"pith:AAYH26VE","schema_version":"1.0","canonical_sha256":"00307d7aa4348b76fbaf0e688b0d15b66c4c7822fc5ae9c908d7b091a0a5d028","source":{"kind":"arxiv","id":"2607.06667","version":1},"attestation_state":"computed","paper":{"title":"Anomaly Realization in Charge-Flux Detector Correlators","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Andrey V. Sadofyev, Jo\\~ao Barata, Ratmir Jumanov","submitted_at":"2026-07-07T18:00:02Z","abstract_excerpt":"Quantum anomalies provide a bridge between ultraviolet properties of a theory and its infrared sector. We study how this connection appears in axial-charge-flow observables. In the simplest example, an axial-charge detector probes the fermionic cut of the anomalous triangle and resolves its infrared content as an angular distribution. The massless limit does not commute with the angular integration: a contribution suppressed at fixed angle collapses onto the two beam-collinear directions while retaining the finite integrated sum rule fixed by the axial anomaly. We then replace the axial-charge"},"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":"2607.06667","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-07-07T18:00:02Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"3d2c2daf513f7ad02cf806fba730a49c1ed22b0d7e0f7c054913c2119a1dc2fd","abstract_canon_sha256":"1dfa9d0d059e3321efbb51d38705722cfc7dbb5f06a56f6e1885935a64844cc9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-09T00:19:22.552959Z","signature_b64":"v7fOEJSYMNSaK8R9T2JBNf9p6dqnKOkCdqXKCJcMQAt9gWxA/1m1QWoQxRUhkk//24hhMLd0vfxMGrE6WNMtCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"00307d7aa4348b76fbaf0e688b0d15b66c4c7822fc5ae9c908d7b091a0a5d028","last_reissued_at":"2026-07-09T00:19:22.552508Z","signature_status":"signed_v1","first_computed_at":"2026-07-09T00:19:22.552508Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Anomaly Realization in Charge-Flux Detector Correlators","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Andrey V. Sadofyev, Jo\\~ao Barata, Ratmir Jumanov","submitted_at":"2026-07-07T18:00:02Z","abstract_excerpt":"Quantum anomalies provide a bridge between ultraviolet properties of a theory and its infrared sector. We study how this connection appears in axial-charge-flow observables. In the simplest example, an axial-charge detector probes the fermionic cut of the anomalous triangle and resolves its infrared content as an angular distribution. The massless limit does not commute with the angular integration: a contribution suppressed at fixed angle collapses onto the two beam-collinear directions while retaining the finite integrated sum rule fixed by the axial anomaly. We then replace the axial-charge"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.06667","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2607.06667/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":"2607.06667","created_at":"2026-07-09T00:19:22.552571+00:00"},{"alias_kind":"arxiv_version","alias_value":"2607.06667v1","created_at":"2026-07-09T00:19:22.552571+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.06667","created_at":"2026-07-09T00:19:22.552571+00:00"},{"alias_kind":"pith_short_12","alias_value":"AAYH26VEGSFX","created_at":"2026-07-09T00:19:22.552571+00:00"},{"alias_kind":"pith_short_16","alias_value":"AAYH26VEGSFXN65P","created_at":"2026-07-09T00:19:22.552571+00:00"},{"alias_kind":"pith_short_8","alias_value":"AAYH26VE","created_at":"2026-07-09T00:19:22.552571+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/AAYH26VEGSFXN65PBZUIWDIVWZ","json":"https://pith.science/pith/AAYH26VEGSFXN65PBZUIWDIVWZ.json","graph_json":"https://pith.science/api/pith-number/AAYH26VEGSFXN65PBZUIWDIVWZ/graph.json","events_json":"https://pith.science/api/pith-number/AAYH26VEGSFXN65PBZUIWDIVWZ/events.json","paper":"https://pith.science/paper/AAYH26VE"},"agent_actions":{"view_html":"https://pith.science/pith/AAYH26VEGSFXN65PBZUIWDIVWZ","download_json":"https://pith.science/pith/AAYH26VEGSFXN65PBZUIWDIVWZ.json","view_paper":"https://pith.science/paper/AAYH26VE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2607.06667&json=true","fetch_graph":"https://pith.science/api/pith-number/AAYH26VEGSFXN65PBZUIWDIVWZ/graph.json","fetch_events":"https://pith.science/api/pith-number/AAYH26VEGSFXN65PBZUIWDIVWZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AAYH26VEGSFXN65PBZUIWDIVWZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AAYH26VEGSFXN65PBZUIWDIVWZ/action/storage_attestation","attest_author":"https://pith.science/pith/AAYH26VEGSFXN65PBZUIWDIVWZ/action/author_attestation","sign_citation":"https://pith.science/pith/AAYH26VEGSFXN65PBZUIWDIVWZ/action/citation_signature","submit_replication":"https://pith.science/pith/AAYH26VEGSFXN65PBZUIWDIVWZ/action/replication_record"}},"created_at":"2026-07-09T00:19:22.552571+00:00","updated_at":"2026-07-09T00:19:22.552571+00:00"}