{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:V7ENXO7GINTR4JEPD3ZODZETUD","short_pith_number":"pith:V7ENXO7G","schema_version":"1.0","canonical_sha256":"afc8dbbbe643671e248f1ef2e1e493a0dfbeba98db5a7cc01998d5ec226e80da","source":{"kind":"arxiv","id":"2603.20414","version":2},"attestation_state":"computed","paper":{"title":"Inverse Electroweak Baryogenesis","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO"],"primary_cat":"hep-ph","authors_text":"Andreas Weiler, Jacopo Azzola, Oleksii Matsedonskyi","submitted_at":"2026-03-20T18:34:57Z","abstract_excerpt":"We propose a mechanism for baryogenesis in which the baryon asymmetry is generated as an equilibrium response of weak sphalerons in a region where electroweak sphaleron transitions remain unsuppressed, $h/T\\lesssim 1$. A nonzero equilibrium baryon density arises in the presence of an approximately conserved global charge, carried either by new states with nonzero hypercharge, or by Standard Model fields themselves. The required global charge asymmetry is generated during a phase transition that changes the strength of electroweak symmetry breaking, but need not coincide with the final electrow"},"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":"2603.20414","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2026-03-20T18:34:57Z","cross_cats_sorted":["astro-ph.CO"],"title_canon_sha256":"4317ec37c99b1092fba54e3268ab5a3ee0bc58b762708acd285c8ec129b7d488","abstract_canon_sha256":"0fcb8e2bd7dcdb38f9c5cc73f3c8f5875e4732e53a4724dd1a2bfaa2def055ca"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-20T00:01:40.383489Z","signature_b64":"h3qXtwBony6CHFo7MC1Ym1Yx1iGQqshq266Twkayx3t/YXa7XO25hOig9bKxsvR+RRm9bhRmkcMNwRQ3otzeAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"afc8dbbbe643671e248f1ef2e1e493a0dfbeba98db5a7cc01998d5ec226e80da","last_reissued_at":"2026-05-20T00:01:40.382787Z","signature_status":"signed_v1","first_computed_at":"2026-05-20T00:01:40.382787Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Inverse Electroweak Baryogenesis","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO"],"primary_cat":"hep-ph","authors_text":"Andreas Weiler, Jacopo Azzola, Oleksii Matsedonskyi","submitted_at":"2026-03-20T18:34:57Z","abstract_excerpt":"We propose a mechanism for baryogenesis in which the baryon asymmetry is generated as an equilibrium response of weak sphalerons in a region where electroweak sphaleron transitions remain unsuppressed, $h/T\\lesssim 1$. A nonzero equilibrium baryon density arises in the presence of an approximately conserved global charge, carried either by new states with nonzero hypercharge, or by Standard Model fields themselves. The required global charge asymmetry is generated during a phase transition that changes the strength of electroweak symmetry breaking, but need not coincide with the final electrow"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2603.20414","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/2603.20414/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":"2603.20414","created_at":"2026-05-20T00:01:40.382906+00:00"},{"alias_kind":"arxiv_version","alias_value":"2603.20414v2","created_at":"2026-05-20T00:01:40.382906+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2603.20414","created_at":"2026-05-20T00:01:40.382906+00:00"},{"alias_kind":"pith_short_12","alias_value":"V7ENXO7GINTR","created_at":"2026-05-20T00:01:40.382906+00:00"},{"alias_kind":"pith_short_16","alias_value":"V7ENXO7GINTR4JEP","created_at":"2026-05-20T00:01:40.382906+00:00"},{"alias_kind":"pith_short_8","alias_value":"V7ENXO7G","created_at":"2026-05-20T00:01:40.382906+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2604.16603","citing_title":"Baryon Asymmetry from Electroweak-Symmetric Domain Walls","ref_index":24,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/V7ENXO7GINTR4JEPD3ZODZETUD","json":"https://pith.science/pith/V7ENXO7GINTR4JEPD3ZODZETUD.json","graph_json":"https://pith.science/api/pith-number/V7ENXO7GINTR4JEPD3ZODZETUD/graph.json","events_json":"https://pith.science/api/pith-number/V7ENXO7GINTR4JEPD3ZODZETUD/events.json","paper":"https://pith.science/paper/V7ENXO7G"},"agent_actions":{"view_html":"https://pith.science/pith/V7ENXO7GINTR4JEPD3ZODZETUD","download_json":"https://pith.science/pith/V7ENXO7GINTR4JEPD3ZODZETUD.json","view_paper":"https://pith.science/paper/V7ENXO7G","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2603.20414&json=true","fetch_graph":"https://pith.science/api/pith-number/V7ENXO7GINTR4JEPD3ZODZETUD/graph.json","fetch_events":"https://pith.science/api/pith-number/V7ENXO7GINTR4JEPD3ZODZETUD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/V7ENXO7GINTR4JEPD3ZODZETUD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/V7ENXO7GINTR4JEPD3ZODZETUD/action/storage_attestation","attest_author":"https://pith.science/pith/V7ENXO7GINTR4JEPD3ZODZETUD/action/author_attestation","sign_citation":"https://pith.science/pith/V7ENXO7GINTR4JEPD3ZODZETUD/action/citation_signature","submit_replication":"https://pith.science/pith/V7ENXO7GINTR4JEPD3ZODZETUD/action/replication_record"}},"created_at":"2026-05-20T00:01:40.382906+00:00","updated_at":"2026-05-20T00:01:40.382906+00:00"}