{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:VIHRCOD6NEWIC7Q3WYKJ7GPWHS","short_pith_number":"pith:VIHRCOD6","schema_version":"1.0","canonical_sha256":"aa0f11387e692c817e1bb6149f99f63cb8566c869625769f42c6137c646a700b","source":{"kind":"arxiv","id":"hep-ph/0108113","version":1},"attestation_state":"computed","paper":{"title":"Non-Equilibrium Large N Yukawa Dynamics: marching through the Landau pole","license":"","headline":"","cross_cats":["astro-ph","hep-th"],"primary_cat":"hep-ph","authors_text":"Daniel Boyanovsky, Hector J. de Vega, Matthew R. Martin, Richard Holman","submitted_at":"2001-08-13T20:09:58Z","abstract_excerpt":"The non-equilibrium dynamics of a Yukawa theory with N fermions coupled to a scalar field is studied in the large N limit with the goal of comparing the dynamics predicted from the renormalization group improved effective potential to that obtained including the fermionic backreaction. The effective potential is of the Coleman-Weinberg type. Its renormalization group improvement is unbounded from below and features a Landau pole. When viewed self-consistently, the initial time singularity does not arise. The different regimes of the dynamics of the fully renormalized theory are studied both an"},"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/0108113","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-08-13T20:09:58Z","cross_cats_sorted":["astro-ph","hep-th"],"title_canon_sha256":"3369d4c64a5ddb2a33a519e428b025937875478b288be6dc7a5160cd39369996","abstract_canon_sha256":"b9e20133e407f1f7a9bd9fa9c16dbe54538af9d8493c9b5eb36680a38c9c81c2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:36:39.468186Z","signature_b64":"i6UJcSzrEHB0yAYJNdyViDfWi20PmJuJe07CwuSyNl4quhPVV6KOmpMs2Wc09p8X0G6NHVItBmbRLR0+4PuiCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aa0f11387e692c817e1bb6149f99f63cb8566c869625769f42c6137c646a700b","last_reissued_at":"2026-05-18T02:36:39.467588Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:36:39.467588Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-Equilibrium Large N Yukawa Dynamics: marching through the Landau pole","license":"","headline":"","cross_cats":["astro-ph","hep-th"],"primary_cat":"hep-ph","authors_text":"Daniel Boyanovsky, Hector J. de Vega, Matthew R. Martin, Richard Holman","submitted_at":"2001-08-13T20:09:58Z","abstract_excerpt":"The non-equilibrium dynamics of a Yukawa theory with N fermions coupled to a scalar field is studied in the large N limit with the goal of comparing the dynamics predicted from the renormalization group improved effective potential to that obtained including the fermionic backreaction. The effective potential is of the Coleman-Weinberg type. Its renormalization group improvement is unbounded from below and features a Landau pole. When viewed self-consistently, the initial time singularity does not arise. The different regimes of the dynamics of the fully renormalized theory are studied both an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0108113","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":""},"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/0108113","created_at":"2026-05-18T02:36:39.467654+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0108113v1","created_at":"2026-05-18T02:36:39.467654+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0108113","created_at":"2026-05-18T02:36:39.467654+00:00"},{"alias_kind":"pith_short_12","alias_value":"VIHRCOD6NEWI","created_at":"2026-05-18T12:25:50.845339+00:00"},{"alias_kind":"pith_short_16","alias_value":"VIHRCOD6NEWIC7Q3","created_at":"2026-05-18T12:25:50.845339+00:00"},{"alias_kind":"pith_short_8","alias_value":"VIHRCOD6","created_at":"2026-05-18T12:25:50.845339+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/VIHRCOD6NEWIC7Q3WYKJ7GPWHS","json":"https://pith.science/pith/VIHRCOD6NEWIC7Q3WYKJ7GPWHS.json","graph_json":"https://pith.science/api/pith-number/VIHRCOD6NEWIC7Q3WYKJ7GPWHS/graph.json","events_json":"https://pith.science/api/pith-number/VIHRCOD6NEWIC7Q3WYKJ7GPWHS/events.json","paper":"https://pith.science/paper/VIHRCOD6"},"agent_actions":{"view_html":"https://pith.science/pith/VIHRCOD6NEWIC7Q3WYKJ7GPWHS","download_json":"https://pith.science/pith/VIHRCOD6NEWIC7Q3WYKJ7GPWHS.json","view_paper":"https://pith.science/paper/VIHRCOD6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0108113&json=true","fetch_graph":"https://pith.science/api/pith-number/VIHRCOD6NEWIC7Q3WYKJ7GPWHS/graph.json","fetch_events":"https://pith.science/api/pith-number/VIHRCOD6NEWIC7Q3WYKJ7GPWHS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VIHRCOD6NEWIC7Q3WYKJ7GPWHS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VIHRCOD6NEWIC7Q3WYKJ7GPWHS/action/storage_attestation","attest_author":"https://pith.science/pith/VIHRCOD6NEWIC7Q3WYKJ7GPWHS/action/author_attestation","sign_citation":"https://pith.science/pith/VIHRCOD6NEWIC7Q3WYKJ7GPWHS/action/citation_signature","submit_replication":"https://pith.science/pith/VIHRCOD6NEWIC7Q3WYKJ7GPWHS/action/replication_record"}},"created_at":"2026-05-18T02:36:39.467654+00:00","updated_at":"2026-05-18T02:36:39.467654+00:00"}