{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:WXISH7OSDY3OENUAS632UAEU4B","short_pith_number":"pith:WXISH7OS","schema_version":"1.0","canonical_sha256":"b5d123fdd21e36e2368097b7aa0094e055c300caa5c1ea6018589f2a6bfb2a8e","source":{"kind":"arxiv","id":"1309.6541","version":1},"attestation_state":"computed","paper":{"title":"Thermodynamics of the Quark-Gluon Plasma in Terms of Quasiparticles and Polyakov Line Condensates","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"Lucia Oliva, Marco Ruggieri, Paolo Castorina, Vincenzo Greco","submitted_at":"2013-09-25T15:14:02Z","abstract_excerpt":"We study a model of quark-gluon plasma of 2+1 flavors Quantum Chromodynamics in terms of quasiparticles propagating in a condensate of Polyakov loops. The Polyakov loop is coupled to quasiparticles by means of a gas-like effective potential. This study is useful to identify the effective degrees of freedom propagating in the medium above the critical temperature. Our finding is that a dominant part of the phase transition dynamics is accounted for by the Polyakov loop, hence the thermodynamics can be described without the need for rapidly increasing quasiparticle masses as $T \\rightarrow T_c$,"},"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":"1309.6541","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-09-25T15:14:02Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"00e9ef0c3bda4fede807a408d246bfcf9cbb14fff752e5b1d0c34f08791ed4e8","abstract_canon_sha256":"6c7c0be5729d22c99da68366ea058c875ff6316c0ccf11940cf1a46393a433ed"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:47:26.807517Z","signature_b64":"eooMIIpggfjJ8H8hDAUlzQ885vK8SUwHPX63Io6ernMT5fxsViC42Gi+jswybceooGuVspQBVf9zzsvQja74Dw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b5d123fdd21e36e2368097b7aa0094e055c300caa5c1ea6018589f2a6bfb2a8e","last_reissued_at":"2026-05-18T01:47:26.806882Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:47:26.806882Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermodynamics of the Quark-Gluon Plasma in Terms of Quasiparticles and Polyakov Line Condensates","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"Lucia Oliva, Marco Ruggieri, Paolo Castorina, Vincenzo Greco","submitted_at":"2013-09-25T15:14:02Z","abstract_excerpt":"We study a model of quark-gluon plasma of 2+1 flavors Quantum Chromodynamics in terms of quasiparticles propagating in a condensate of Polyakov loops. The Polyakov loop is coupled to quasiparticles by means of a gas-like effective potential. This study is useful to identify the effective degrees of freedom propagating in the medium above the critical temperature. Our finding is that a dominant part of the phase transition dynamics is accounted for by the Polyakov loop, hence the thermodynamics can be described without the need for rapidly increasing quasiparticle masses as $T \\rightarrow T_c$,"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1309.6541","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":"1309.6541","created_at":"2026-05-18T01:47:26.806992+00:00"},{"alias_kind":"arxiv_version","alias_value":"1309.6541v1","created_at":"2026-05-18T01:47:26.806992+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1309.6541","created_at":"2026-05-18T01:47:26.806992+00:00"},{"alias_kind":"pith_short_12","alias_value":"WXISH7OSDY3O","created_at":"2026-05-18T12:28:06.772260+00:00"},{"alias_kind":"pith_short_16","alias_value":"WXISH7OSDY3OENUA","created_at":"2026-05-18T12:28:06.772260+00:00"},{"alias_kind":"pith_short_8","alias_value":"WXISH7OS","created_at":"2026-05-18T12:28:06.772260+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/WXISH7OSDY3OENUAS632UAEU4B","json":"https://pith.science/pith/WXISH7OSDY3OENUAS632UAEU4B.json","graph_json":"https://pith.science/api/pith-number/WXISH7OSDY3OENUAS632UAEU4B/graph.json","events_json":"https://pith.science/api/pith-number/WXISH7OSDY3OENUAS632UAEU4B/events.json","paper":"https://pith.science/paper/WXISH7OS"},"agent_actions":{"view_html":"https://pith.science/pith/WXISH7OSDY3OENUAS632UAEU4B","download_json":"https://pith.science/pith/WXISH7OSDY3OENUAS632UAEU4B.json","view_paper":"https://pith.science/paper/WXISH7OS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1309.6541&json=true","fetch_graph":"https://pith.science/api/pith-number/WXISH7OSDY3OENUAS632UAEU4B/graph.json","fetch_events":"https://pith.science/api/pith-number/WXISH7OSDY3OENUAS632UAEU4B/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WXISH7OSDY3OENUAS632UAEU4B/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WXISH7OSDY3OENUAS632UAEU4B/action/storage_attestation","attest_author":"https://pith.science/pith/WXISH7OSDY3OENUAS632UAEU4B/action/author_attestation","sign_citation":"https://pith.science/pith/WXISH7OSDY3OENUAS632UAEU4B/action/citation_signature","submit_replication":"https://pith.science/pith/WXISH7OSDY3OENUAS632UAEU4B/action/replication_record"}},"created_at":"2026-05-18T01:47:26.806992+00:00","updated_at":"2026-05-18T01:47:26.806992+00:00"}