{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:GNTBMXT2CENCY4LVAI6SVNTCAT","short_pith_number":"pith:GNTBMXT2","schema_version":"1.0","canonical_sha256":"3366165e7a111a2c7175023d2ab66204cdb966cbf8beee6d9081f376b4aae6e4","source":{"kind":"arxiv","id":"hep-ph/0107200","version":2},"attestation_state":"computed","paper":{"title":"Renormalization in Self-Consistent Approximations schemes at Finite Temperature I: Theory","license":"","headline":"","cross_cats":["cond-mat","nucl-th"],"primary_cat":"hep-ph","authors_text":"H. Hees, J. Knoll","submitted_at":"2001-07-18T20:59:15Z","abstract_excerpt":"Within finite temperature field theory, we show that truncated non-perturbative self-consistent Dyson resummation schemes can be renormalized with local counter-terms defined at the vacuum level. The requirements are that the underlying theory is renormalizable and that the self-consistent scheme follows Baym''s $\\Phi$-derivable concept. The scheme generates both, the renormalized self-consistent equations of motion and the closed equations for the infinite set of counter terms. At the same time the corresponding 2PI-generating functional and the thermodynamical potential can be renormalized, "},"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/0107200","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-07-18T20:59:15Z","cross_cats_sorted":["cond-mat","nucl-th"],"title_canon_sha256":"528d3be2033259571f46d933aa0d2cb79097e64f146f005067cc55ec974c5c81","abstract_canon_sha256":"1294540132b1158edb5cb8153f60c103ff61d5861f6f2e25cfd8f138ec5e6ff9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:27:25.344884Z","signature_b64":"vyriNU5VbkXUi/7MEqEOt4zp82gBvR7SVrmezk6v1cs1m/rMuxIMDwd2g0aIJmZXppyHNcaoqOU3tcDxRy6kDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3366165e7a111a2c7175023d2ab66204cdb966cbf8beee6d9081f376b4aae6e4","last_reissued_at":"2026-07-04T16:27:25.344338Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:27:25.344338Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Renormalization in Self-Consistent Approximations schemes at Finite Temperature I: Theory","license":"","headline":"","cross_cats":["cond-mat","nucl-th"],"primary_cat":"hep-ph","authors_text":"H. Hees, J. Knoll","submitted_at":"2001-07-18T20:59:15Z","abstract_excerpt":"Within finite temperature field theory, we show that truncated non-perturbative self-consistent Dyson resummation schemes can be renormalized with local counter-terms defined at the vacuum level. The requirements are that the underlying theory is renormalizable and that the self-consistent scheme follows Baym''s $\\Phi$-derivable concept. The scheme generates both, the renormalized self-consistent equations of motion and the closed equations for the infinite set of counter terms. At the same time the corresponding 2PI-generating functional and the thermodynamical potential can be renormalized, "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0107200","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/hep-ph/0107200/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":"hep-ph/0107200","created_at":"2026-07-04T16:27:25.344407+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0107200v2","created_at":"2026-07-04T16:27:25.344407+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0107200","created_at":"2026-07-04T16:27:25.344407+00:00"},{"alias_kind":"pith_short_12","alias_value":"GNTBMXT2CENC","created_at":"2026-07-04T16:27:25.344407+00:00"},{"alias_kind":"pith_short_16","alias_value":"GNTBMXT2CENCY4LV","created_at":"2026-07-04T16:27:25.344407+00:00"},{"alias_kind":"pith_short_8","alias_value":"GNTBMXT2","created_at":"2026-07-04T16:27:25.344407+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2512.18830","citing_title":"Emergent chiral spin symmetry, non-perturbative dynamics and thermoparticles in hot QCD","ref_index":32,"is_internal_anchor":true},{"citing_arxiv_id":"2604.11553","citing_title":"Self-consistent computation of pair production from non-relativistic effective field theories in the Keldysh-Schwinger formalism","ref_index":63,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GNTBMXT2CENCY4LVAI6SVNTCAT","json":"https://pith.science/pith/GNTBMXT2CENCY4LVAI6SVNTCAT.json","graph_json":"https://pith.science/api/pith-number/GNTBMXT2CENCY4LVAI6SVNTCAT/graph.json","events_json":"https://pith.science/api/pith-number/GNTBMXT2CENCY4LVAI6SVNTCAT/events.json","paper":"https://pith.science/paper/GNTBMXT2"},"agent_actions":{"view_html":"https://pith.science/pith/GNTBMXT2CENCY4LVAI6SVNTCAT","download_json":"https://pith.science/pith/GNTBMXT2CENCY4LVAI6SVNTCAT.json","view_paper":"https://pith.science/paper/GNTBMXT2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0107200&json=true","fetch_graph":"https://pith.science/api/pith-number/GNTBMXT2CENCY4LVAI6SVNTCAT/graph.json","fetch_events":"https://pith.science/api/pith-number/GNTBMXT2CENCY4LVAI6SVNTCAT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GNTBMXT2CENCY4LVAI6SVNTCAT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GNTBMXT2CENCY4LVAI6SVNTCAT/action/storage_attestation","attest_author":"https://pith.science/pith/GNTBMXT2CENCY4LVAI6SVNTCAT/action/author_attestation","sign_citation":"https://pith.science/pith/GNTBMXT2CENCY4LVAI6SVNTCAT/action/citation_signature","submit_replication":"https://pith.science/pith/GNTBMXT2CENCY4LVAI6SVNTCAT/action/replication_record"}},"created_at":"2026-07-04T16:27:25.344407+00:00","updated_at":"2026-07-04T16:27:25.344407+00:00"}