{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:M5VUJSZBIGYRCSXPDVQWDOWTRS","short_pith_number":"pith:M5VUJSZB","schema_version":"1.0","canonical_sha256":"676b44cb2141b1114aef1d6161bad38ca88f0a7658953538f0df60a8be29b169","source":{"kind":"arxiv","id":"0907.5518","version":2},"attestation_state":"computed","paper":{"title":"On Relation Between the Quark Gluon Bag Surface Tension and the Colour Tube String Tension","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"G. M. Zinovjev, K. A. Bugaev","submitted_at":"2009-07-31T12:01:16Z","abstract_excerpt":"Here we revisit the bag phenomenology of the deconfining phase transition to replenish it by introducing systematically the bag surface tension. Comparing the free energy of such bags and that one of  the strings confining the static quark-antiquark pair, we express the string tension in terms of the bag surface tension and thermal pressure in order to estimate the bag characteristics using the lattice QCD data. Our analysis of the bag entropy density demonstrates that the surface tension coefficient is   amazingly negative at the cross-over (continuous transition). This approach allows us to "},"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":"0907.5518","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-07-31T12:01:16Z","cross_cats_sorted":[],"title_canon_sha256":"712b47c5426e63acacc473b7558d96e6b9c3d1f0efc47e92406bc5bf8ccf1f78","abstract_canon_sha256":"727fb881e272ff73cf205fdb46abe93fe833312d44fd8c2c6994edbe38a9eb4d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:35:05.318895Z","signature_b64":"NMCt1gQq2NFl1SQ4EFkq7QqXyZcaWkB1DJ9IYVIpFNhXEF3xHN8rASCyRhkZxD0IcIX0+4DYnaUuH5yuWd23Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"676b44cb2141b1114aef1d6161bad38ca88f0a7658953538f0df60a8be29b169","last_reissued_at":"2026-05-18T04:35:05.318450Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:35:05.318450Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On Relation Between the Quark Gluon Bag Surface Tension and the Colour Tube String Tension","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"G. M. Zinovjev, K. A. Bugaev","submitted_at":"2009-07-31T12:01:16Z","abstract_excerpt":"Here we revisit the bag phenomenology of the deconfining phase transition to replenish it by introducing systematically the bag surface tension. Comparing the free energy of such bags and that one of  the strings confining the static quark-antiquark pair, we express the string tension in terms of the bag surface tension and thermal pressure in order to estimate the bag characteristics using the lattice QCD data. Our analysis of the bag entropy density demonstrates that the surface tension coefficient is   amazingly negative at the cross-over (continuous transition). This approach allows us to "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0907.5518","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"0907.5518","created_at":"2026-05-18T04:35:05.318522+00:00"},{"alias_kind":"arxiv_version","alias_value":"0907.5518v2","created_at":"2026-05-18T04:35:05.318522+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0907.5518","created_at":"2026-05-18T04:35:05.318522+00:00"},{"alias_kind":"pith_short_12","alias_value":"M5VUJSZBIGYR","created_at":"2026-05-18T12:26:00.592388+00:00"},{"alias_kind":"pith_short_16","alias_value":"M5VUJSZBIGYRCSXP","created_at":"2026-05-18T12:26:00.592388+00:00"},{"alias_kind":"pith_short_8","alias_value":"M5VUJSZB","created_at":"2026-05-18T12:26:00.592388+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/M5VUJSZBIGYRCSXPDVQWDOWTRS","json":"https://pith.science/pith/M5VUJSZBIGYRCSXPDVQWDOWTRS.json","graph_json":"https://pith.science/api/pith-number/M5VUJSZBIGYRCSXPDVQWDOWTRS/graph.json","events_json":"https://pith.science/api/pith-number/M5VUJSZBIGYRCSXPDVQWDOWTRS/events.json","paper":"https://pith.science/paper/M5VUJSZB"},"agent_actions":{"view_html":"https://pith.science/pith/M5VUJSZBIGYRCSXPDVQWDOWTRS","download_json":"https://pith.science/pith/M5VUJSZBIGYRCSXPDVQWDOWTRS.json","view_paper":"https://pith.science/paper/M5VUJSZB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0907.5518&json=true","fetch_graph":"https://pith.science/api/pith-number/M5VUJSZBIGYRCSXPDVQWDOWTRS/graph.json","fetch_events":"https://pith.science/api/pith-number/M5VUJSZBIGYRCSXPDVQWDOWTRS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/M5VUJSZBIGYRCSXPDVQWDOWTRS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/M5VUJSZBIGYRCSXPDVQWDOWTRS/action/storage_attestation","attest_author":"https://pith.science/pith/M5VUJSZBIGYRCSXPDVQWDOWTRS/action/author_attestation","sign_citation":"https://pith.science/pith/M5VUJSZBIGYRCSXPDVQWDOWTRS/action/citation_signature","submit_replication":"https://pith.science/pith/M5VUJSZBIGYRCSXPDVQWDOWTRS/action/replication_record"}},"created_at":"2026-05-18T04:35:05.318522+00:00","updated_at":"2026-05-18T04:35:05.318522+00:00"}