{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:6HQHOFEKCI3O6TXJAIY44PCA6M","short_pith_number":"pith:6HQHOFEK","schema_version":"1.0","canonical_sha256":"f1e077148a1236ef4ee90231ce3c40f33d755d8a0502599d156ecf7b1509cf10","source":{"kind":"arxiv","id":"hep-th/0608198","version":3},"attestation_state":"computed","paper":{"title":"Holographic chiral phase transition with chemical potential","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"N. Horigome, Y. Tanii","submitted_at":"2006-08-28T09:50:29Z","abstract_excerpt":"We discuss the Sakai-Sugimoto model at finite temperature and finite chemical potential. It is a holographic model of large N_c QCD with N_f massless quarks based on a D4/D8-\\bar{D8} brane system. The near horizon limit of the D4-branes and the probe approximation of the D8-\\bar{D8} pairs allow us to treat the D4-branes as a gravitational background and the D8-\\bar{D8} pairs as a probe which does not affect the background. We propose that the asymptotic value of a U(1) gauge field on the D8-\\bar{D8}-branes is identified with the chemical potential for the baryon number. Using this chemical pot"},"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":"hep-th/0608198","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2006-08-28T09:50:29Z","cross_cats_sorted":[],"title_canon_sha256":"45a96453c553cb2bfa748a4ab2fdc785c4072cd90c90f4905fcd544dc396b5eb","abstract_canon_sha256":"de35dae95f90d8580aba09661b6a37740cb740c09d8b65ae2e61c94647284e24"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:38:26.590211Z","signature_b64":"DY7bM4ndBYtZsNqOAbJrWLG2g7OHVYg+CmbkbcfbwD1pBd5L3Ybt1H+34+r+Gxr72goawvpzt3tuSCZGBaPlBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f1e077148a1236ef4ee90231ce3c40f33d755d8a0502599d156ecf7b1509cf10","last_reissued_at":"2026-05-18T04:38:26.589701Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:38:26.589701Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Holographic chiral phase transition with chemical potential","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"N. Horigome, Y. Tanii","submitted_at":"2006-08-28T09:50:29Z","abstract_excerpt":"We discuss the Sakai-Sugimoto model at finite temperature and finite chemical potential. It is a holographic model of large N_c QCD with N_f massless quarks based on a D4/D8-\\bar{D8} brane system. The near horizon limit of the D4-branes and the probe approximation of the D8-\\bar{D8} pairs allow us to treat the D4-branes as a gravitational background and the D8-\\bar{D8} pairs as a probe which does not affect the background. We propose that the asymptotic value of a U(1) gauge field on the D8-\\bar{D8}-branes is identified with the chemical potential for the baryon number. Using this chemical pot"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0608198","kind":"arxiv","version":3},"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":"hep-th/0608198","created_at":"2026-05-18T04:38:26.589769+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0608198v3","created_at":"2026-05-18T04:38:26.589769+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0608198","created_at":"2026-05-18T04:38:26.589769+00:00"},{"alias_kind":"pith_short_12","alias_value":"6HQHOFEKCI3O","created_at":"2026-05-18T12:25:53.939244+00:00"},{"alias_kind":"pith_short_16","alias_value":"6HQHOFEKCI3O6TXJ","created_at":"2026-05-18T12:25:53.939244+00:00"},{"alias_kind":"pith_short_8","alias_value":"6HQHOFEK","created_at":"2026-05-18T12:25:53.939244+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.04586","citing_title":"Bound states and deconfinement from Romans supergravity with magnetic flux","ref_index":52,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6HQHOFEKCI3O6TXJAIY44PCA6M","json":"https://pith.science/pith/6HQHOFEKCI3O6TXJAIY44PCA6M.json","graph_json":"https://pith.science/api/pith-number/6HQHOFEKCI3O6TXJAIY44PCA6M/graph.json","events_json":"https://pith.science/api/pith-number/6HQHOFEKCI3O6TXJAIY44PCA6M/events.json","paper":"https://pith.science/paper/6HQHOFEK"},"agent_actions":{"view_html":"https://pith.science/pith/6HQHOFEKCI3O6TXJAIY44PCA6M","download_json":"https://pith.science/pith/6HQHOFEKCI3O6TXJAIY44PCA6M.json","view_paper":"https://pith.science/paper/6HQHOFEK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0608198&json=true","fetch_graph":"https://pith.science/api/pith-number/6HQHOFEKCI3O6TXJAIY44PCA6M/graph.json","fetch_events":"https://pith.science/api/pith-number/6HQHOFEKCI3O6TXJAIY44PCA6M/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6HQHOFEKCI3O6TXJAIY44PCA6M/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6HQHOFEKCI3O6TXJAIY44PCA6M/action/storage_attestation","attest_author":"https://pith.science/pith/6HQHOFEKCI3O6TXJAIY44PCA6M/action/author_attestation","sign_citation":"https://pith.science/pith/6HQHOFEKCI3O6TXJAIY44PCA6M/action/citation_signature","submit_replication":"https://pith.science/pith/6HQHOFEKCI3O6TXJAIY44PCA6M/action/replication_record"}},"created_at":"2026-05-18T04:38:26.589769+00:00","updated_at":"2026-05-18T04:38:26.589769+00:00"}