{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:NX2OI6OX5LN22CPZGHRX35GJSH","short_pith_number":"pith:NX2OI6OX","schema_version":"1.0","canonical_sha256":"6df4e479d7eadbad09f931e37df4c991f094452286e2384a057ecabbe80d96ed","source":{"kind":"arxiv","id":"1301.2523","version":2},"attestation_state":"computed","paper":{"title":"QCD Topology at Finite Temperature: Statistical Mechanics of Selfdual Dyons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Edward Shuryak, Pietro Faccioli","submitted_at":"2013-01-11T15:52:13Z","abstract_excerpt":"Topological phenomena in gauge theories have long been recognized as the driving force for chiral symmetry breaking and confinement. These phenomena can be conveniently investigated in the semi-classical picture, in which the topological charge is entirely carried by (anti-)self-dual gauge configurations. In such an approach, it has been shown that near the critical temperature, the non-zero expectation value of the Polyakov loop (holonomy) triggers the \"Higgsing\" of the color group, generating the splitting of instantons into $N_c$ self-dual dyons.\n  A number of lattice simulations have provi"},"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":"1301.2523","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-01-11T15:52:13Z","cross_cats_sorted":["hep-lat","nucl-th"],"title_canon_sha256":"928c93db958ba1c010149fcf0d11c6acf67287eeecbaf583d3f21bd24cc6dad7","abstract_canon_sha256":"0126032afd6fb35755c438c313159a11a4afc8298d0504976a7176965aa6cf15"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:27:54.188898Z","signature_b64":"rWkbcSiRvd8TLl6znZmOzbOkFUfqJoHfsY+AdZuUEmhTSSsuaGbL73RdpfvoyxQbuKNt7WOi8/Hfj7XsAXGNAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6df4e479d7eadbad09f931e37df4c991f094452286e2384a057ecabbe80d96ed","last_reissued_at":"2026-05-18T03:27:54.188228Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:27:54.188228Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"QCD Topology at Finite Temperature: Statistical Mechanics of Selfdual Dyons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Edward Shuryak, Pietro Faccioli","submitted_at":"2013-01-11T15:52:13Z","abstract_excerpt":"Topological phenomena in gauge theories have long been recognized as the driving force for chiral symmetry breaking and confinement. These phenomena can be conveniently investigated in the semi-classical picture, in which the topological charge is entirely carried by (anti-)self-dual gauge configurations. In such an approach, it has been shown that near the critical temperature, the non-zero expectation value of the Polyakov loop (holonomy) triggers the \"Higgsing\" of the color group, generating the splitting of instantons into $N_c$ self-dual dyons.\n  A number of lattice simulations have provi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1301.2523","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":"1301.2523","created_at":"2026-05-18T03:27:54.188330+00:00"},{"alias_kind":"arxiv_version","alias_value":"1301.2523v2","created_at":"2026-05-18T03:27:54.188330+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1301.2523","created_at":"2026-05-18T03:27:54.188330+00:00"},{"alias_kind":"pith_short_12","alias_value":"NX2OI6OX5LN2","created_at":"2026-05-18T12:27:52.871228+00:00"},{"alias_kind":"pith_short_16","alias_value":"NX2OI6OX5LN22CPZ","created_at":"2026-05-18T12:27:52.871228+00:00"},{"alias_kind":"pith_short_8","alias_value":"NX2OI6OX","created_at":"2026-05-18T12:27:52.871228+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1908.08709","citing_title":"Density and correlations of topological objects near the transition temperature in lattice gluodynamics","ref_index":6,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NX2OI6OX5LN22CPZGHRX35GJSH","json":"https://pith.science/pith/NX2OI6OX5LN22CPZGHRX35GJSH.json","graph_json":"https://pith.science/api/pith-number/NX2OI6OX5LN22CPZGHRX35GJSH/graph.json","events_json":"https://pith.science/api/pith-number/NX2OI6OX5LN22CPZGHRX35GJSH/events.json","paper":"https://pith.science/paper/NX2OI6OX"},"agent_actions":{"view_html":"https://pith.science/pith/NX2OI6OX5LN22CPZGHRX35GJSH","download_json":"https://pith.science/pith/NX2OI6OX5LN22CPZGHRX35GJSH.json","view_paper":"https://pith.science/paper/NX2OI6OX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1301.2523&json=true","fetch_graph":"https://pith.science/api/pith-number/NX2OI6OX5LN22CPZGHRX35GJSH/graph.json","fetch_events":"https://pith.science/api/pith-number/NX2OI6OX5LN22CPZGHRX35GJSH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NX2OI6OX5LN22CPZGHRX35GJSH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NX2OI6OX5LN22CPZGHRX35GJSH/action/storage_attestation","attest_author":"https://pith.science/pith/NX2OI6OX5LN22CPZGHRX35GJSH/action/author_attestation","sign_citation":"https://pith.science/pith/NX2OI6OX5LN22CPZGHRX35GJSH/action/citation_signature","submit_replication":"https://pith.science/pith/NX2OI6OX5LN22CPZGHRX35GJSH/action/replication_record"}},"created_at":"2026-05-18T03:27:54.188330+00:00","updated_at":"2026-05-18T03:27:54.188330+00:00"}