{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:MGSY5DPAK5OX3VYJF2BMBPJ424","short_pith_number":"pith:MGSY5DPA","schema_version":"1.0","canonical_sha256":"61a58e8de0575d7dd7092e82c0bd3cd72128587e8b148799232e13fc95fae423","source":{"kind":"arxiv","id":"2603.01652","version":2},"attestation_state":"computed","paper":{"title":"Schwinger--Keldysh formulation of electromagnetic leptogenesis in an EFT framework","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Rin Takada","submitted_at":"2026-03-02T09:33:01Z","abstract_excerpt":"Can the electromagnetic dipole interactions probed in precision experiments be the same interactions that generated the baryon asymmetry of the Universe? We address this question by formulating low-scale electromagnetic leptogenesis (EMLG) as a gauge-invariant EFT, rather than as a broken-phase dipole ansatz. The point is not only to connect leptogenesis to laboratory dipole observables, but first to test whether the dipole-dominated dynamics itself can satisfy the cosmological viability requirement.\n  Starting from a softly broken $Z_2$ UV completion, we match onto the $\\nu$SMEFT dipole opera"},"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":"2603.01652","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2026-03-02T09:33:01Z","cross_cats_sorted":[],"title_canon_sha256":"2da7113af11749bcfc1e00601c7f8f80177879cd1e17ba4ad0b354f91aac7c7e","abstract_canon_sha256":"e4f3e16cb393057470db53d1c150a28dae35e6c83d5e9382c17eb3d6a2105eea"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-30T01:16:28.658000Z","signature_b64":"RtCCA3N/eETJSIGG4n1EnKbzRM25XBQn1nRTxPutx1DmKg4vLh7kZzrf4ktI7bEw7ALaicVFcSbaM3vCFgitAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"61a58e8de0575d7dd7092e82c0bd3cd72128587e8b148799232e13fc95fae423","last_reissued_at":"2026-06-30T01:16:28.657172Z","signature_status":"signed_v1","first_computed_at":"2026-06-30T01:16:28.657172Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Schwinger--Keldysh formulation of electromagnetic leptogenesis in an EFT framework","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Rin Takada","submitted_at":"2026-03-02T09:33:01Z","abstract_excerpt":"Can the electromagnetic dipole interactions probed in precision experiments be the same interactions that generated the baryon asymmetry of the Universe? We address this question by formulating low-scale electromagnetic leptogenesis (EMLG) as a gauge-invariant EFT, rather than as a broken-phase dipole ansatz. The point is not only to connect leptogenesis to laboratory dipole observables, but first to test whether the dipole-dominated dynamics itself can satisfy the cosmological viability requirement.\n  Starting from a softly broken $Z_2$ UV completion, we match onto the $\\nu$SMEFT dipole opera"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2603.01652","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/2603.01652/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":"2603.01652","created_at":"2026-06-30T01:16:28.657253+00:00"},{"alias_kind":"arxiv_version","alias_value":"2603.01652v2","created_at":"2026-06-30T01:16:28.657253+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2603.01652","created_at":"2026-06-30T01:16:28.657253+00:00"},{"alias_kind":"pith_short_12","alias_value":"MGSY5DPAK5OX","created_at":"2026-06-30T01:16:28.657253+00:00"},{"alias_kind":"pith_short_16","alias_value":"MGSY5DPAK5OX3VYJ","created_at":"2026-06-30T01:16:28.657253+00:00"},{"alias_kind":"pith_short_8","alias_value":"MGSY5DPA","created_at":"2026-06-30T01:16:28.657253+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/MGSY5DPAK5OX3VYJF2BMBPJ424","json":"https://pith.science/pith/MGSY5DPAK5OX3VYJF2BMBPJ424.json","graph_json":"https://pith.science/api/pith-number/MGSY5DPAK5OX3VYJF2BMBPJ424/graph.json","events_json":"https://pith.science/api/pith-number/MGSY5DPAK5OX3VYJF2BMBPJ424/events.json","paper":"https://pith.science/paper/MGSY5DPA"},"agent_actions":{"view_html":"https://pith.science/pith/MGSY5DPAK5OX3VYJF2BMBPJ424","download_json":"https://pith.science/pith/MGSY5DPAK5OX3VYJF2BMBPJ424.json","view_paper":"https://pith.science/paper/MGSY5DPA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2603.01652&json=true","fetch_graph":"https://pith.science/api/pith-number/MGSY5DPAK5OX3VYJF2BMBPJ424/graph.json","fetch_events":"https://pith.science/api/pith-number/MGSY5DPAK5OX3VYJF2BMBPJ424/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MGSY5DPAK5OX3VYJF2BMBPJ424/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MGSY5DPAK5OX3VYJF2BMBPJ424/action/storage_attestation","attest_author":"https://pith.science/pith/MGSY5DPAK5OX3VYJF2BMBPJ424/action/author_attestation","sign_citation":"https://pith.science/pith/MGSY5DPAK5OX3VYJF2BMBPJ424/action/citation_signature","submit_replication":"https://pith.science/pith/MGSY5DPAK5OX3VYJF2BMBPJ424/action/replication_record"}},"created_at":"2026-06-30T01:16:28.657253+00:00","updated_at":"2026-06-30T01:16:28.657253+00:00"}