{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:F5IDBZY2SCJKOIAZ6PUKBHZS46","short_pith_number":"pith:F5IDBZY2","schema_version":"1.0","canonical_sha256":"2f5030e71a9092a72019f3e8a09f32e7aeac0c063cebbd4e2a0e35c1f0a4c13f","source":{"kind":"arxiv","id":"1101.5362","version":2},"attestation_state":"computed","paper":{"title":"Isospin Breaking and chiral symmetry restoration","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.Gomez Nicola, R.Torres Andres","submitted_at":"2011-01-27T19:17:16Z","abstract_excerpt":"We analyze quark condensates and chiral (scalar) susceptibilities including isospin breaking effects at finite temperature $T$. These include $m_u\\neq m_d$ contributions as well as electromagnetic ($e\\neq 0$) corrections, both treated in a consistent chiral lagrangian framework to leading order in SU(2) and SU(3) Chiral Perturbation Theory, so that our predictions are model independent. The chiral restoration temperature extracted from $<\\bar q q>= <\\bar u u + \\bar d d >$ is almost unaffected, while the isospin breaking order parameter $<\\bar u u - \\bar d d >$ grows with $T$ for the three-flav"},"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":"1101.5362","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-01-27T19:17:16Z","cross_cats_sorted":[],"title_canon_sha256":"f421ef1d2b1a6f3c7c33323b4a14a5f73c63b779b44dcec5c75363310d0dddf7","abstract_canon_sha256":"fbd9a54f6a5cc81aa44db9af6631ee86b57c40910f0221737c7a16bcdb36b8f9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:23:45.426724Z","signature_b64":"6n8ZHGjZ8yXuRSvST8+MxFwM5UMB+ZnKvqM5I68blj7Lx46/Jo25gTMWQaKbnL7dfjgNzDMJxM+bWG1JZbXdBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2f5030e71a9092a72019f3e8a09f32e7aeac0c063cebbd4e2a0e35c1f0a4c13f","last_reissued_at":"2026-05-18T04:23:45.426278Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:23:45.426278Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Isospin Breaking and chiral symmetry restoration","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.Gomez Nicola, R.Torres Andres","submitted_at":"2011-01-27T19:17:16Z","abstract_excerpt":"We analyze quark condensates and chiral (scalar) susceptibilities including isospin breaking effects at finite temperature $T$. These include $m_u\\neq m_d$ contributions as well as electromagnetic ($e\\neq 0$) corrections, both treated in a consistent chiral lagrangian framework to leading order in SU(2) and SU(3) Chiral Perturbation Theory, so that our predictions are model independent. The chiral restoration temperature extracted from $<\\bar q q>= <\\bar u u + \\bar d d >$ is almost unaffected, while the isospin breaking order parameter $<\\bar u u - \\bar d d >$ grows with $T$ for the three-flav"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1101.5362","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":""},"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":"1101.5362","created_at":"2026-05-18T04:23:45.426345+00:00"},{"alias_kind":"arxiv_version","alias_value":"1101.5362v2","created_at":"2026-05-18T04:23:45.426345+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1101.5362","created_at":"2026-05-18T04:23:45.426345+00:00"},{"alias_kind":"pith_short_12","alias_value":"F5IDBZY2SCJK","created_at":"2026-05-18T12:26:28.662955+00:00"},{"alias_kind":"pith_short_16","alias_value":"F5IDBZY2SCJKOIAZ","created_at":"2026-05-18T12:26:28.662955+00:00"},{"alias_kind":"pith_short_8","alias_value":"F5IDBZY2","created_at":"2026-05-18T12:26:28.662955+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/F5IDBZY2SCJKOIAZ6PUKBHZS46","json":"https://pith.science/pith/F5IDBZY2SCJKOIAZ6PUKBHZS46.json","graph_json":"https://pith.science/api/pith-number/F5IDBZY2SCJKOIAZ6PUKBHZS46/graph.json","events_json":"https://pith.science/api/pith-number/F5IDBZY2SCJKOIAZ6PUKBHZS46/events.json","paper":"https://pith.science/paper/F5IDBZY2"},"agent_actions":{"view_html":"https://pith.science/pith/F5IDBZY2SCJKOIAZ6PUKBHZS46","download_json":"https://pith.science/pith/F5IDBZY2SCJKOIAZ6PUKBHZS46.json","view_paper":"https://pith.science/paper/F5IDBZY2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1101.5362&json=true","fetch_graph":"https://pith.science/api/pith-number/F5IDBZY2SCJKOIAZ6PUKBHZS46/graph.json","fetch_events":"https://pith.science/api/pith-number/F5IDBZY2SCJKOIAZ6PUKBHZS46/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/F5IDBZY2SCJKOIAZ6PUKBHZS46/action/timestamp_anchor","attest_storage":"https://pith.science/pith/F5IDBZY2SCJKOIAZ6PUKBHZS46/action/storage_attestation","attest_author":"https://pith.science/pith/F5IDBZY2SCJKOIAZ6PUKBHZS46/action/author_attestation","sign_citation":"https://pith.science/pith/F5IDBZY2SCJKOIAZ6PUKBHZS46/action/citation_signature","submit_replication":"https://pith.science/pith/F5IDBZY2SCJKOIAZ6PUKBHZS46/action/replication_record"}},"created_at":"2026-05-18T04:23:45.426345+00:00","updated_at":"2026-05-18T04:23:45.426345+00:00"}