{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:AOEMDPOH4WZR4M4ENJETFH45FN","short_pith_number":"pith:AOEMDPOH","canonical_record":{"source":{"id":"1508.07704","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-08-31T06:52:55Z","cross_cats_sorted":[],"title_canon_sha256":"bb709e0ae60114de5c422d68bf998740f4b44cbb58cbac59a5f6b4f21f2ed599","abstract_canon_sha256":"49f2c4a0346ef6de7ba13a533456bb0913cd4f3339f7058e1a257cb9d4c8cee9"},"schema_version":"1.0"},"canonical_sha256":"0388c1bdc7e5b31e33846a49329f9d2b50083d1721763faf99828870d2e0a523","source":{"kind":"arxiv","id":"1508.07704","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1508.07704","created_at":"2026-05-18T01:27:22Z"},{"alias_kind":"arxiv_version","alias_value":"1508.07704v2","created_at":"2026-05-18T01:27:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.07704","created_at":"2026-05-18T01:27:22Z"},{"alias_kind":"pith_short_12","alias_value":"AOEMDPOH4WZR","created_at":"2026-05-18T12:29:10Z"},{"alias_kind":"pith_short_16","alias_value":"AOEMDPOH4WZR4M4E","created_at":"2026-05-18T12:29:10Z"},{"alias_kind":"pith_short_8","alias_value":"AOEMDPOH","created_at":"2026-05-18T12:29:10Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:AOEMDPOH4WZR4M4ENJETFH45FN","target":"record","payload":{"canonical_record":{"source":{"id":"1508.07704","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-08-31T06:52:55Z","cross_cats_sorted":[],"title_canon_sha256":"bb709e0ae60114de5c422d68bf998740f4b44cbb58cbac59a5f6b4f21f2ed599","abstract_canon_sha256":"49f2c4a0346ef6de7ba13a533456bb0913cd4f3339f7058e1a257cb9d4c8cee9"},"schema_version":"1.0"},"canonical_sha256":"0388c1bdc7e5b31e33846a49329f9d2b50083d1721763faf99828870d2e0a523","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:27:22.722277Z","signature_b64":"pLhYVpvsA5DbdCTvSmpGKmDupMd9TKz5dQpIPZONkamG2DJ353LpHFz5YBMNCl9OgklaH1uWvRv4Ab2+jcnQBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0388c1bdc7e5b31e33846a49329f9d2b50083d1721763faf99828870d2e0a523","last_reissued_at":"2026-05-18T01:27:22.721883Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:27:22.721883Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1508.07704","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:27:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5MCZaO4Pv9/opoungzThMjrbFv6EMY5s0uVnvvtBcNmTqa8R0Btt6ItQSZYkRoYh1iaAKFaLeI4LRwlpSViVAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T08:45:34.246106Z"},"content_sha256":"28de534b03c88eaf55c0e23502b96ebee929bcdb5255df4fa2cc2a75a75ec4bd","schema_version":"1.0","event_id":"sha256:28de534b03c88eaf55c0e23502b96ebee929bcdb5255df4fa2cc2a75a75ec4bd"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:AOEMDPOH4WZR4M4ENJETFH45FN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Topological susceptibility near $T_{c}$ in SU(3) gauge theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Chuan Liu, Guang-Yi Xiong, Jian-Bo Zhang, Jian-Ping Ma, Ying Chen, Yu-Bin Liu","submitted_at":"2015-08-31T06:52:55Z","abstract_excerpt":"Topological charge susceptibility $\\chi_{t}$ for pure gauge SU(3) theory at finite temperature is studied using anisotropic lattices. The over-improved stout-link smoothing method is utilized to calculate the topological charge. Near the phase transition point we find a rapid declining behavior for $\\chi_{t}$ with values decreasing from $(188(1)\\mathrm{MeV})^{4}$ to $(67(3)\\mathrm{MeV})^{4}$ as the temperature increased from zero temperature to $1.9T_{c}$ which demonstrates the existence of topological excitations far above $T_{c}$. The 4th order cumulant $c_4$ of topological charge, as well a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.07704","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:27:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RUHmLzKgQaNdjssSeKUwWpa/1evcV+Imqq8ITdLRAJtgH83CbZ7GOrlsR8jLa+IvfVVyRa+1mo0TaW2U5x4WCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T08:45:34.246479Z"},"content_sha256":"b83b7e50d440dd430f91d48662282f26420ac739ec0ea69eb6d41a27cfe52e52","schema_version":"1.0","event_id":"sha256:b83b7e50d440dd430f91d48662282f26420ac739ec0ea69eb6d41a27cfe52e52"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/AOEMDPOH4WZR4M4ENJETFH45FN/bundle.json","state_url":"https://pith.science/pith/AOEMDPOH4WZR4M4ENJETFH45FN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/AOEMDPOH4WZR4M4ENJETFH45FN/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":"2026-05-30T08:45:34Z","links":{"resolver":"https://pith.science/pith/AOEMDPOH4WZR4M4ENJETFH45FN","bundle":"https://pith.science/pith/AOEMDPOH4WZR4M4ENJETFH45FN/bundle.json","state":"https://pith.science/pith/AOEMDPOH4WZR4M4ENJETFH45FN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/AOEMDPOH4WZR4M4ENJETFH45FN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:AOEMDPOH4WZR4M4ENJETFH45FN","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":"49f2c4a0346ef6de7ba13a533456bb0913cd4f3339f7058e1a257cb9d4c8cee9","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-08-31T06:52:55Z","title_canon_sha256":"bb709e0ae60114de5c422d68bf998740f4b44cbb58cbac59a5f6b4f21f2ed599"},"schema_version":"1.0","source":{"id":"1508.07704","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1508.07704","created_at":"2026-05-18T01:27:22Z"},{"alias_kind":"arxiv_version","alias_value":"1508.07704v2","created_at":"2026-05-18T01:27:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.07704","created_at":"2026-05-18T01:27:22Z"},{"alias_kind":"pith_short_12","alias_value":"AOEMDPOH4WZR","created_at":"2026-05-18T12:29:10Z"},{"alias_kind":"pith_short_16","alias_value":"AOEMDPOH4WZR4M4E","created_at":"2026-05-18T12:29:10Z"},{"alias_kind":"pith_short_8","alias_value":"AOEMDPOH","created_at":"2026-05-18T12:29:10Z"}],"graph_snapshots":[{"event_id":"sha256:b83b7e50d440dd430f91d48662282f26420ac739ec0ea69eb6d41a27cfe52e52","target":"graph","created_at":"2026-05-18T01:27:22Z","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":"Topological charge susceptibility $\\chi_{t}$ for pure gauge SU(3) theory at finite temperature is studied using anisotropic lattices. The over-improved stout-link smoothing method is utilized to calculate the topological charge. Near the phase transition point we find a rapid declining behavior for $\\chi_{t}$ with values decreasing from $(188(1)\\mathrm{MeV})^{4}$ to $(67(3)\\mathrm{MeV})^{4}$ as the temperature increased from zero temperature to $1.9T_{c}$ which demonstrates the existence of topological excitations far above $T_{c}$. The 4th order cumulant $c_4$ of topological charge, as well a","authors_text":"Chuan Liu, Guang-Yi Xiong, Jian-Bo Zhang, Jian-Ping Ma, Ying Chen, Yu-Bin Liu","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-08-31T06:52:55Z","title":"Topological susceptibility near $T_{c}$ in SU(3) gauge theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.07704","kind":"arxiv","version":2},"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":"sha256:28de534b03c88eaf55c0e23502b96ebee929bcdb5255df4fa2cc2a75a75ec4bd","target":"record","created_at":"2026-05-18T01:27:22Z","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":"49f2c4a0346ef6de7ba13a533456bb0913cd4f3339f7058e1a257cb9d4c8cee9","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-08-31T06:52:55Z","title_canon_sha256":"bb709e0ae60114de5c422d68bf998740f4b44cbb58cbac59a5f6b4f21f2ed599"},"schema_version":"1.0","source":{"id":"1508.07704","kind":"arxiv","version":2}},"canonical_sha256":"0388c1bdc7e5b31e33846a49329f9d2b50083d1721763faf99828870d2e0a523","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0388c1bdc7e5b31e33846a49329f9d2b50083d1721763faf99828870d2e0a523","first_computed_at":"2026-05-18T01:27:22.721883Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:27:22.721883Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"pLhYVpvsA5DbdCTvSmpGKmDupMd9TKz5dQpIPZONkamG2DJ353LpHFz5YBMNCl9OgklaH1uWvRv4Ab2+jcnQBg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:27:22.722277Z","signed_message":"canonical_sha256_bytes"},"source_id":"1508.07704","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:28de534b03c88eaf55c0e23502b96ebee929bcdb5255df4fa2cc2a75a75ec4bd","sha256:b83b7e50d440dd430f91d48662282f26420ac739ec0ea69eb6d41a27cfe52e52"],"state_sha256":"58b3779866bd5b2b85b00f99b46aa820e8f37b27b857f3ff3cd7dd1c9c8794df"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CzN22Tg6FEqpDapuQK4e4viOucF76aLbLVFSB4SquPXZZmcg3Oyem+LE+Er+/GS1GUkkSOZTaFX6bAG5v9BdDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T08:45:34.248419Z","bundle_sha256":"8ec2a0d5ab7866e831efb09cfba3cc16f659e4609dd4fc018a856ba86ff500ef"}}