{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:2HACGY4UOXEBV5VZFRTPUKNYDL","short_pith_number":"pith:2HACGY4U","schema_version":"1.0","canonical_sha256":"d1c023639475c81af6b92c66fa29b81ad451a4a9026c0598b763146ad93d692b","source":{"kind":"arxiv","id":"1012.2308","version":1},"attestation_state":"computed","paper":{"title":"Yang-Mills streamlines and semi-classical confinement","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"hep-lat","authors_text":"Ernst-Michael Ilgenfritz, Kurt Langfeld","submitted_at":"2010-12-10T16:09:55Z","abstract_excerpt":"Semi-classical configurations in Yang-Mills theory have been derived from lattice Monte Carlo configurations using a recently proposed constrained cooling technique which is designed to preserve every Polyakov line (at any point in space-time in any direction). Consequently, confinement was found sustained by the ensemble of semi-classical configurations. The existence of gluonic and fermionic near-to-zero modes was demonstrated as a precondition for a possible semi-classical expansion around the cooled configurations as well as providing the gapless spectrum of the Dirac operator necessary fo"},"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":"1012.2308","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2010-12-10T16:09:55Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"923f87137fe3323c58edf3267735fbde59f1c2d54c49626d949a871570f1993c","abstract_canon_sha256":"a3b95bd96c13162d929ea016cfd2f3b68120eb1fea9418fea57f01bf79d4fcb6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:04:30.457625Z","signature_b64":"HsMwt3k2eJn8R9CvX4rnikQITxhSNcCWJWR2viFeIuBaULsPjHMl2OQE+YPl4Yg94oik7HkNMegpUL5b2eJgBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d1c023639475c81af6b92c66fa29b81ad451a4a9026c0598b763146ad93d692b","last_reissued_at":"2026-05-18T02:04:30.457014Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:04:30.457014Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Yang-Mills streamlines and semi-classical confinement","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"hep-lat","authors_text":"Ernst-Michael Ilgenfritz, Kurt Langfeld","submitted_at":"2010-12-10T16:09:55Z","abstract_excerpt":"Semi-classical configurations in Yang-Mills theory have been derived from lattice Monte Carlo configurations using a recently proposed constrained cooling technique which is designed to preserve every Polyakov line (at any point in space-time in any direction). Consequently, confinement was found sustained by the ensemble of semi-classical configurations. The existence of gluonic and fermionic near-to-zero modes was demonstrated as a precondition for a possible semi-classical expansion around the cooled configurations as well as providing the gapless spectrum of the Dirac operator necessary fo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1012.2308","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":"1012.2308","created_at":"2026-05-18T02:04:30.457127+00:00"},{"alias_kind":"arxiv_version","alias_value":"1012.2308v1","created_at":"2026-05-18T02:04:30.457127+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1012.2308","created_at":"2026-05-18T02:04:30.457127+00:00"},{"alias_kind":"pith_short_12","alias_value":"2HACGY4UOXEB","created_at":"2026-05-18T12:26:03.138858+00:00"},{"alias_kind":"pith_short_16","alias_value":"2HACGY4UOXEBV5VZ","created_at":"2026-05-18T12:26:03.138858+00:00"},{"alias_kind":"pith_short_8","alias_value":"2HACGY4U","created_at":"2026-05-18T12:26:03.138858+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/2HACGY4UOXEBV5VZFRTPUKNYDL","json":"https://pith.science/pith/2HACGY4UOXEBV5VZFRTPUKNYDL.json","graph_json":"https://pith.science/api/pith-number/2HACGY4UOXEBV5VZFRTPUKNYDL/graph.json","events_json":"https://pith.science/api/pith-number/2HACGY4UOXEBV5VZFRTPUKNYDL/events.json","paper":"https://pith.science/paper/2HACGY4U"},"agent_actions":{"view_html":"https://pith.science/pith/2HACGY4UOXEBV5VZFRTPUKNYDL","download_json":"https://pith.science/pith/2HACGY4UOXEBV5VZFRTPUKNYDL.json","view_paper":"https://pith.science/paper/2HACGY4U","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1012.2308&json=true","fetch_graph":"https://pith.science/api/pith-number/2HACGY4UOXEBV5VZFRTPUKNYDL/graph.json","fetch_events":"https://pith.science/api/pith-number/2HACGY4UOXEBV5VZFRTPUKNYDL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2HACGY4UOXEBV5VZFRTPUKNYDL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2HACGY4UOXEBV5VZFRTPUKNYDL/action/storage_attestation","attest_author":"https://pith.science/pith/2HACGY4UOXEBV5VZFRTPUKNYDL/action/author_attestation","sign_citation":"https://pith.science/pith/2HACGY4UOXEBV5VZFRTPUKNYDL/action/citation_signature","submit_replication":"https://pith.science/pith/2HACGY4UOXEBV5VZFRTPUKNYDL/action/replication_record"}},"created_at":"2026-05-18T02:04:30.457127+00:00","updated_at":"2026-05-18T02:04:30.457127+00:00"}