{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:STIQR3SEHYOXD5BKKRGO7W4QIB","short_pith_number":"pith:STIQR3SE","canonical_record":{"source":{"id":"1307.6339","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-07-24T09:11:55Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"f2bc9e5b9036e76741d218fb9ad021fe08cdaec334ad6bca1ccc6ebbbed5c51b","abstract_canon_sha256":"795a590267782b688cfc201a9f6f2cf355df498f08fe05f3cfe98823c59d163d"},"schema_version":"1.0"},"canonical_sha256":"94d108ee443e1d71f42a544cefdb9040654a0221a5e106c07102a98d3446b036","source":{"kind":"arxiv","id":"1307.6339","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1307.6339","created_at":"2026-05-18T03:08:04Z"},{"alias_kind":"arxiv_version","alias_value":"1307.6339v1","created_at":"2026-05-18T03:08:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1307.6339","created_at":"2026-05-18T03:08:04Z"},{"alias_kind":"pith_short_12","alias_value":"STIQR3SEHYOX","created_at":"2026-05-18T12:27:59Z"},{"alias_kind":"pith_short_16","alias_value":"STIQR3SEHYOXD5BK","created_at":"2026-05-18T12:27:59Z"},{"alias_kind":"pith_short_8","alias_value":"STIQR3SE","created_at":"2026-05-18T12:27:59Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:STIQR3SEHYOXD5BKKRGO7W4QIB","target":"record","payload":{"canonical_record":{"source":{"id":"1307.6339","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-07-24T09:11:55Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"f2bc9e5b9036e76741d218fb9ad021fe08cdaec334ad6bca1ccc6ebbbed5c51b","abstract_canon_sha256":"795a590267782b688cfc201a9f6f2cf355df498f08fe05f3cfe98823c59d163d"},"schema_version":"1.0"},"canonical_sha256":"94d108ee443e1d71f42a544cefdb9040654a0221a5e106c07102a98d3446b036","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:08:04.009798Z","signature_b64":"/70MkviChn6g73J5jDAvuSSBfzxShqLdylzUowPhSbaE9O2cPuSJO5wQd4v4TyXw5lgrOOsSbvwG24ovxJ00CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"94d108ee443e1d71f42a544cefdb9040654a0221a5e106c07102a98d3446b036","last_reissued_at":"2026-05-18T03:08:04.009074Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:08:04.009074Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1307.6339","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:08:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UQeIqn3CgjjwOLqgHoy0bko7aFOGmUE4OY7ulUn92VxIs4qdN0gNP0iqLOCS6jqL3IQDlehl8pGdjuZ4lWIlBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T06:58:57.841171Z"},"content_sha256":"00192c6a8c71d57e08deada804a6e717b6ca2ddc16f6b05aaa137bb95e8605f2","schema_version":"1.0","event_id":"sha256:00192c6a8c71d57e08deada804a6e717b6ca2ddc16f6b05aaa137bb95e8605f2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:STIQR3SEHYOXD5BKKRGO7W4QIB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Effective potential for SU(2) Polyakov loops and Wilson loop eigenvalues","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Adrian Dumitru, Dominik Smith, Lorenz von Smekal, Robert Pisarski","submitted_at":"2013-07-24T09:11:55Z","abstract_excerpt":"We simulate SU(2) gauge theory at temperatures ranging from slightly below $T_c$ to roughly $2T_c$ for two different values of the gauge coupling. Using a histogram method, we extract the effective potential for the Polyakov loop and for the phases of the eigenvalues of the thermal Wilson loop, in both the fundamental and adjoint representations. We show that the classical potential of the fundamental loop can be parametrized within a simple model which includes a Vandermonde potential and terms linear and quadratic in the Polyakov loop. We discuss how parametrizations for the other cases can "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1307.6339","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:08:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uwVVe9hJ21mv/cZDOgJUiKD8jYPbA+wxFmmb4KsffuIpgpcvV4DV1bt0B5348SFCT1FoqU1dojHgxiSM2gREAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T06:58:57.841875Z"},"content_sha256":"48594fc26575c38ba310a023b6a9a3078c7fdbbdc3a46d1e795c8b648d462b04","schema_version":"1.0","event_id":"sha256:48594fc26575c38ba310a023b6a9a3078c7fdbbdc3a46d1e795c8b648d462b04"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/STIQR3SEHYOXD5BKKRGO7W4QIB/bundle.json","state_url":"https://pith.science/pith/STIQR3SEHYOXD5BKKRGO7W4QIB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/STIQR3SEHYOXD5BKKRGO7W4QIB/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-30T06:58:57Z","links":{"resolver":"https://pith.science/pith/STIQR3SEHYOXD5BKKRGO7W4QIB","bundle":"https://pith.science/pith/STIQR3SEHYOXD5BKKRGO7W4QIB/bundle.json","state":"https://pith.science/pith/STIQR3SEHYOXD5BKKRGO7W4QIB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/STIQR3SEHYOXD5BKKRGO7W4QIB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:STIQR3SEHYOXD5BKKRGO7W4QIB","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"795a590267782b688cfc201a9f6f2cf355df498f08fe05f3cfe98823c59d163d","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-07-24T09:11:55Z","title_canon_sha256":"f2bc9e5b9036e76741d218fb9ad021fe08cdaec334ad6bca1ccc6ebbbed5c51b"},"schema_version":"1.0","source":{"id":"1307.6339","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1307.6339","created_at":"2026-05-18T03:08:04Z"},{"alias_kind":"arxiv_version","alias_value":"1307.6339v1","created_at":"2026-05-18T03:08:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1307.6339","created_at":"2026-05-18T03:08:04Z"},{"alias_kind":"pith_short_12","alias_value":"STIQR3SEHYOX","created_at":"2026-05-18T12:27:59Z"},{"alias_kind":"pith_short_16","alias_value":"STIQR3SEHYOXD5BK","created_at":"2026-05-18T12:27:59Z"},{"alias_kind":"pith_short_8","alias_value":"STIQR3SE","created_at":"2026-05-18T12:27:59Z"}],"graph_snapshots":[{"event_id":"sha256:48594fc26575c38ba310a023b6a9a3078c7fdbbdc3a46d1e795c8b648d462b04","target":"graph","created_at":"2026-05-18T03:08:04Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We simulate SU(2) gauge theory at temperatures ranging from slightly below $T_c$ to roughly $2T_c$ for two different values of the gauge coupling. Using a histogram method, we extract the effective potential for the Polyakov loop and for the phases of the eigenvalues of the thermal Wilson loop, in both the fundamental and adjoint representations. We show that the classical potential of the fundamental loop can be parametrized within a simple model which includes a Vandermonde potential and terms linear and quadratic in the Polyakov loop. We discuss how parametrizations for the other cases can ","authors_text":"Adrian Dumitru, Dominik Smith, Lorenz von Smekal, Robert Pisarski","cross_cats":["hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-07-24T09:11:55Z","title":"Effective potential for SU(2) Polyakov loops and Wilson loop eigenvalues"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1307.6339","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:00192c6a8c71d57e08deada804a6e717b6ca2ddc16f6b05aaa137bb95e8605f2","target":"record","created_at":"2026-05-18T03:08:04Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"795a590267782b688cfc201a9f6f2cf355df498f08fe05f3cfe98823c59d163d","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-07-24T09:11:55Z","title_canon_sha256":"f2bc9e5b9036e76741d218fb9ad021fe08cdaec334ad6bca1ccc6ebbbed5c51b"},"schema_version":"1.0","source":{"id":"1307.6339","kind":"arxiv","version":1}},"canonical_sha256":"94d108ee443e1d71f42a544cefdb9040654a0221a5e106c07102a98d3446b036","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"94d108ee443e1d71f42a544cefdb9040654a0221a5e106c07102a98d3446b036","first_computed_at":"2026-05-18T03:08:04.009074Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:08:04.009074Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"/70MkviChn6g73J5jDAvuSSBfzxShqLdylzUowPhSbaE9O2cPuSJO5wQd4v4TyXw5lgrOOsSbvwG24ovxJ00CQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:08:04.009798Z","signed_message":"canonical_sha256_bytes"},"source_id":"1307.6339","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:00192c6a8c71d57e08deada804a6e717b6ca2ddc16f6b05aaa137bb95e8605f2","sha256:48594fc26575c38ba310a023b6a9a3078c7fdbbdc3a46d1e795c8b648d462b04"],"state_sha256":"6575fd12ceaba5d9e04e4da47f432c96d837b32102d0c110b728351b1072f0bc"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0Pa5NfYjR1ECsRxpjxWTb1UaOXCQLpnzvcC6mhfIxxVuJUC6FFh4oCXm355RIQQVzHDGPoqrhr6AyFOO07DxCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T06:58:57.844517Z","bundle_sha256":"05b11a167c56ab9b57baf93b16eef22af40c9cac38fba8b638a7047c6b660095"}}