{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:LM3DMYAIWTVK7GSDC5SAMRSNEE","short_pith_number":"pith:LM3DMYAI","schema_version":"1.0","canonical_sha256":"5b36366008b4eaaf9a43176406464d2120e5d19401e567fe562cc12961d519b6","source":{"kind":"arxiv","id":"2412.20829","version":1},"attestation_state":"computed","paper":{"title":"Quantum flux operators in the fermionic theory and their supersymmetric extension","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Jiang Long, Si-Mao Guo, Wen-Bin Liu","submitted_at":"2024-12-30T09:53:07Z","abstract_excerpt":"We construct quantum flux operators with respect to the Poincar\\'e symmetry in the massless Dirac theory at future null infinity. An anomalous helicity flux operator emerges from the commutator of the superrotation generators. The helicity flux operator corresponds to the local chiral symmetry which is the analog of superduality in the gauge theories. We also find its relation to the non-closure of the Lie transport of the spinor field around a loop. We discuss various algebras formed by these operators and constrain the test functions by the requirement of eliminating the non-local terms and "},"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":"2412.20829","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2024-12-30T09:53:07Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"092b81d8bad7da62ea4d3bf889f047656f8c3bc9732b6c3d80213761283440f3","abstract_canon_sha256":"bddad9baca9c620f3f0b3ec2519a017f98ef75651805550aba44ced31ba8245a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:55:23.098165Z","signature_b64":"b+iOM1qcPD34cIh1RcdqUSo8o/6dn55IO3ji6ejEUosd9NJiYI0zy6a7OFRh+SiiSffFxHSQ4d6kAe7I90YBDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5b36366008b4eaaf9a43176406464d2120e5d19401e567fe562cc12961d519b6","last_reissued_at":"2026-07-05T09:55:23.095431Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:55:23.095431Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum flux operators in the fermionic theory and their supersymmetric extension","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Jiang Long, Si-Mao Guo, Wen-Bin Liu","submitted_at":"2024-12-30T09:53:07Z","abstract_excerpt":"We construct quantum flux operators with respect to the Poincar\\'e symmetry in the massless Dirac theory at future null infinity. An anomalous helicity flux operator emerges from the commutator of the superrotation generators. The helicity flux operator corresponds to the local chiral symmetry which is the analog of superduality in the gauge theories. We also find its relation to the non-closure of the Lie transport of the spinor field around a loop. We discuss various algebras formed by these operators and constrain the test functions by the requirement of eliminating the non-local terms and "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2412.20829","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/2412.20829/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":"2412.20829","created_at":"2026-07-05T09:55:23.096939+00:00"},{"alias_kind":"arxiv_version","alias_value":"2412.20829v1","created_at":"2026-07-05T09:55:23.096939+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2412.20829","created_at":"2026-07-05T09:55:23.096939+00:00"},{"alias_kind":"pith_short_12","alias_value":"LM3DMYAIWTVK","created_at":"2026-07-05T09:55:23.096939+00:00"},{"alias_kind":"pith_short_16","alias_value":"LM3DMYAIWTVK7GSD","created_at":"2026-07-05T09:55:23.096939+00:00"},{"alias_kind":"pith_short_8","alias_value":"LM3DMYAI","created_at":"2026-07-05T09:55:23.096939+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2508.01446","citing_title":"Radiation in Fluid/Gravity and the Flat Limit","ref_index":241,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LM3DMYAIWTVK7GSDC5SAMRSNEE","json":"https://pith.science/pith/LM3DMYAIWTVK7GSDC5SAMRSNEE.json","graph_json":"https://pith.science/api/pith-number/LM3DMYAIWTVK7GSDC5SAMRSNEE/graph.json","events_json":"https://pith.science/api/pith-number/LM3DMYAIWTVK7GSDC5SAMRSNEE/events.json","paper":"https://pith.science/paper/LM3DMYAI"},"agent_actions":{"view_html":"https://pith.science/pith/LM3DMYAIWTVK7GSDC5SAMRSNEE","download_json":"https://pith.science/pith/LM3DMYAIWTVK7GSDC5SAMRSNEE.json","view_paper":"https://pith.science/paper/LM3DMYAI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2412.20829&json=true","fetch_graph":"https://pith.science/api/pith-number/LM3DMYAIWTVK7GSDC5SAMRSNEE/graph.json","fetch_events":"https://pith.science/api/pith-number/LM3DMYAIWTVK7GSDC5SAMRSNEE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LM3DMYAIWTVK7GSDC5SAMRSNEE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LM3DMYAIWTVK7GSDC5SAMRSNEE/action/storage_attestation","attest_author":"https://pith.science/pith/LM3DMYAIWTVK7GSDC5SAMRSNEE/action/author_attestation","sign_citation":"https://pith.science/pith/LM3DMYAIWTVK7GSDC5SAMRSNEE/action/citation_signature","submit_replication":"https://pith.science/pith/LM3DMYAIWTVK7GSDC5SAMRSNEE/action/replication_record"}},"created_at":"2026-07-05T09:55:23.096939+00:00","updated_at":"2026-07-05T09:55:23.096939+00:00"}