{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2008:JCY4GGJBSVSQDKAG7TWYXSHIHD","short_pith_number":"pith:JCY4GGJB","schema_version":"1.0","canonical_sha256":"48b1c31921956501a806fced8bc8e838fe7d93e0f348ae8ac8582d90b6bc1695","source":{"kind":"arxiv","id":"0803.2128","version":1},"attestation_state":"computed","paper":{"title":"The deconfining phase transition in D=2+1 SU(N) gauge theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Jack Liddle, Michael Teper","submitted_at":"2008-03-14T10:37:06Z","abstract_excerpt":"We study the deconfining transition of SU(N) gauge theories in 2+1 dimensions for N ranging between N=2 and N=8. We confirm that the transition is second order for N<4 and first order for N>4. For the more delicate case of SU(4) all our evidence points to the transition being weakly first order. After extrapolating to the continuum limit, we obtain a deconfining temperature that can be well fitted by Tc/sqrt(sigma) = 0.9026(23) + 0.880(43)/N^2 for all N."},"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":"0803.2128","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2008-03-14T10:37:06Z","cross_cats_sorted":[],"title_canon_sha256":"77e3526212843aa2df075d6cc3685c1133947c5fc93e49690d2ee617f44cc6d5","abstract_canon_sha256":"2c174ab64aa23a6a40da7eb202cc3a3744e8f73d21fa723ee6ae1f4eae2d8a00"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:10:14.507801Z","signature_b64":"46OfyIHUp8se983zQENnSpS7QnNFXewWVNJC4kD39NLiZO6eCroMFbJc+74g5E7YFCpgHbuLx+Lm9eMqdgoqBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"48b1c31921956501a806fced8bc8e838fe7d93e0f348ae8ac8582d90b6bc1695","last_reissued_at":"2026-07-04T15:10:14.507391Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:10:14.507391Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The deconfining phase transition in D=2+1 SU(N) gauge theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Jack Liddle, Michael Teper","submitted_at":"2008-03-14T10:37:06Z","abstract_excerpt":"We study the deconfining transition of SU(N) gauge theories in 2+1 dimensions for N ranging between N=2 and N=8. We confirm that the transition is second order for N<4 and first order for N>4. For the more delicate case of SU(4) all our evidence points to the transition being weakly first order. After extrapolating to the continuum limit, we obtain a deconfining temperature that can be well fitted by Tc/sqrt(sigma) = 0.9026(23) + 0.880(43)/N^2 for all N."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0803.2128","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/0803.2128/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":"0803.2128","created_at":"2026-07-04T15:10:14.507453+00:00"},{"alias_kind":"arxiv_version","alias_value":"0803.2128v1","created_at":"2026-07-04T15:10:14.507453+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0803.2128","created_at":"2026-07-04T15:10:14.507453+00:00"},{"alias_kind":"pith_short_12","alias_value":"JCY4GGJBSVSQ","created_at":"2026-07-04T15:10:14.507453+00:00"},{"alias_kind":"pith_short_16","alias_value":"JCY4GGJBSVSQDKAG","created_at":"2026-07-04T15:10:14.507453+00:00"},{"alias_kind":"pith_short_8","alias_value":"JCY4GGJB","created_at":"2026-07-04T15:10:14.507453+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.01740","citing_title":"Intrinsic width of the flux tube in 2+1 dimensional Yang-Mills therories","ref_index":22,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JCY4GGJBSVSQDKAG7TWYXSHIHD","json":"https://pith.science/pith/JCY4GGJBSVSQDKAG7TWYXSHIHD.json","graph_json":"https://pith.science/api/pith-number/JCY4GGJBSVSQDKAG7TWYXSHIHD/graph.json","events_json":"https://pith.science/api/pith-number/JCY4GGJBSVSQDKAG7TWYXSHIHD/events.json","paper":"https://pith.science/paper/JCY4GGJB"},"agent_actions":{"view_html":"https://pith.science/pith/JCY4GGJBSVSQDKAG7TWYXSHIHD","download_json":"https://pith.science/pith/JCY4GGJBSVSQDKAG7TWYXSHIHD.json","view_paper":"https://pith.science/paper/JCY4GGJB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0803.2128&json=true","fetch_graph":"https://pith.science/api/pith-number/JCY4GGJBSVSQDKAG7TWYXSHIHD/graph.json","fetch_events":"https://pith.science/api/pith-number/JCY4GGJBSVSQDKAG7TWYXSHIHD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JCY4GGJBSVSQDKAG7TWYXSHIHD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JCY4GGJBSVSQDKAG7TWYXSHIHD/action/storage_attestation","attest_author":"https://pith.science/pith/JCY4GGJBSVSQDKAG7TWYXSHIHD/action/author_attestation","sign_citation":"https://pith.science/pith/JCY4GGJBSVSQDKAG7TWYXSHIHD/action/citation_signature","submit_replication":"https://pith.science/pith/JCY4GGJBSVSQDKAG7TWYXSHIHD/action/replication_record"}},"created_at":"2026-07-04T15:10:14.507453+00:00","updated_at":"2026-07-04T15:10:14.507453+00:00"}