{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2008:QXAUF72X33DAKRC3PXRVA4R6R4","short_pith_number":"pith:QXAUF72X","schema_version":"1.0","canonical_sha256":"85c142ff57dec605445b7de350723e8f041576add9e201430a6a6e05689d85e4","source":{"kind":"arxiv","id":"0807.0855","version":2},"attestation_state":"computed","paper":{"title":"Thermodynamics of SU(3) Gauge Theory in 2 + 1 Dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Morel, B. Petersson, L. Daniel, P. Bialas","submitted_at":"2008-07-07T16:30:00Z","abstract_excerpt":"The pressure, and the energy and entropy densities are determined for the SU(3) gauge theory in $2 + 1$ dimensions from lattice Monte Carlo calculations in the interval $0.6 \\leq T/T_c \\leq 15$. The finite temperature lattices simulated have temporal extent $N_\\tau = 2, 4, 6$ and 8, and spatial volumes $N_S^2$ such that the aspect ratio is $N_S/N_\\tau = 8$. To obtain the thermodynamical quantities, we calculate the averages of the temporal plaquettes $P_\\tau$ and the spatial plaquettes $P_S$ on these lattices. We also need the zero temperature averages of the plaquettes $P_0$, calculated on sy"},"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":"0807.0855","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2008-07-07T16:30:00Z","cross_cats_sorted":[],"title_canon_sha256":"18035a0c35261fa612a0f5487601fecd6061f37255d7b536d50b4559c5ad94f7","abstract_canon_sha256":"ff1b6232bfdc47f39b531527f9df47b08115bbb40da5d853774909d4465c5bfc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:30:21.123476Z","signature_b64":"20zOfvKVEG5fJQEo6dvZZmMkCKul6GZafpmuofCD7oG32t2pYkxsllsGrVCsaY64SrWR04dWBIs20WyFwidSAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"85c142ff57dec605445b7de350723e8f041576add9e201430a6a6e05689d85e4","last_reissued_at":"2026-07-04T15:30:21.123142Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:30:21.123142Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermodynamics of SU(3) Gauge Theory in 2 + 1 Dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Morel, B. Petersson, L. Daniel, P. Bialas","submitted_at":"2008-07-07T16:30:00Z","abstract_excerpt":"The pressure, and the energy and entropy densities are determined for the SU(3) gauge theory in $2 + 1$ dimensions from lattice Monte Carlo calculations in the interval $0.6 \\leq T/T_c \\leq 15$. The finite temperature lattices simulated have temporal extent $N_\\tau = 2, 4, 6$ and 8, and spatial volumes $N_S^2$ such that the aspect ratio is $N_S/N_\\tau = 8$. To obtain the thermodynamical quantities, we calculate the averages of the temporal plaquettes $P_\\tau$ and the spatial plaquettes $P_S$ on these lattices. We also need the zero temperature averages of the plaquettes $P_0$, calculated on sy"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0807.0855","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/0807.0855/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"0807.0855","created_at":"2026-07-04T15:30:21.123197+00:00"},{"alias_kind":"arxiv_version","alias_value":"0807.0855v2","created_at":"2026-07-04T15:30:21.123197+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0807.0855","created_at":"2026-07-04T15:30:21.123197+00:00"},{"alias_kind":"pith_short_12","alias_value":"QXAUF72X33DA","created_at":"2026-07-04T15:30:21.123197+00:00"},{"alias_kind":"pith_short_16","alias_value":"QXAUF72X33DAKRC3","created_at":"2026-07-04T15:30:21.123197+00:00"},{"alias_kind":"pith_short_8","alias_value":"QXAUF72X","created_at":"2026-07-04T15:30:21.123197+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/QXAUF72X33DAKRC3PXRVA4R6R4","json":"https://pith.science/pith/QXAUF72X33DAKRC3PXRVA4R6R4.json","graph_json":"https://pith.science/api/pith-number/QXAUF72X33DAKRC3PXRVA4R6R4/graph.json","events_json":"https://pith.science/api/pith-number/QXAUF72X33DAKRC3PXRVA4R6R4/events.json","paper":"https://pith.science/paper/QXAUF72X"},"agent_actions":{"view_html":"https://pith.science/pith/QXAUF72X33DAKRC3PXRVA4R6R4","download_json":"https://pith.science/pith/QXAUF72X33DAKRC3PXRVA4R6R4.json","view_paper":"https://pith.science/paper/QXAUF72X","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0807.0855&json=true","fetch_graph":"https://pith.science/api/pith-number/QXAUF72X33DAKRC3PXRVA4R6R4/graph.json","fetch_events":"https://pith.science/api/pith-number/QXAUF72X33DAKRC3PXRVA4R6R4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QXAUF72X33DAKRC3PXRVA4R6R4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QXAUF72X33DAKRC3PXRVA4R6R4/action/storage_attestation","attest_author":"https://pith.science/pith/QXAUF72X33DAKRC3PXRVA4R6R4/action/author_attestation","sign_citation":"https://pith.science/pith/QXAUF72X33DAKRC3PXRVA4R6R4/action/citation_signature","submit_replication":"https://pith.science/pith/QXAUF72X33DAKRC3PXRVA4R6R4/action/replication_record"}},"created_at":"2026-07-04T15:30:21.123197+00:00","updated_at":"2026-07-04T15:30:21.123197+00:00"}