{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:WRQNPA2GBQC2YIPNUOEPHHHKUD","short_pith_number":"pith:WRQNPA2G","schema_version":"1.0","canonical_sha256":"b460d783460c05ac21eda388f39ceaa0dd033a88e40cbcaef648f22af57c7856","source":{"kind":"arxiv","id":"1103.2315","version":3},"attestation_state":"computed","paper":{"title":"Holographic Roberge-Weiss Transitions II: Defect Theories and the Sakai-Sugimoto Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-th","authors_text":"James Rafferty","submitted_at":"2011-03-11T17:08:01Z","abstract_excerpt":"We extend the work of Aarts et al., including an imaginary chemical potential for quark number into the Sakai-Sugimoto model and codimension k defect theories. The phase diagram of these models are a function of three parameters, the temperature, chemical potential and the asymptotic separation of the flavour branes, related to a mass for the quarks in the boundary theories. We compute the phase diagrams and the pressure due to the flavours of the theories as a function of these parameters and show that there are Roberge-Weiss transitions in the high temperature phases, chiral symmetry restore"},"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":"1103.2315","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-03-11T17:08:01Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"97ecc704e767cacf79167e9c161d862195ebaa1cbcba93c4efec5d928ba2e657","abstract_canon_sha256":"9179c0aae90ab4d568bc204aa28445e68d4598a8561c193f40ed41082377f499"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:22:19.917897Z","signature_b64":"PAC9X9vH69eNm+MAjBgi2y6fOO0sJBLNY7f4qSgAVD+0BHkcCaPmOWRkC3D4lKf7rs1TAG1yiz7PCPi5MJswCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b460d783460c05ac21eda388f39ceaa0dd033a88e40cbcaef648f22af57c7856","last_reissued_at":"2026-05-18T02:22:19.917277Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:22:19.917277Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Holographic Roberge-Weiss Transitions II: Defect Theories and the Sakai-Sugimoto Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-th","authors_text":"James Rafferty","submitted_at":"2011-03-11T17:08:01Z","abstract_excerpt":"We extend the work of Aarts et al., including an imaginary chemical potential for quark number into the Sakai-Sugimoto model and codimension k defect theories. The phase diagram of these models are a function of three parameters, the temperature, chemical potential and the asymptotic separation of the flavour branes, related to a mass for the quarks in the boundary theories. We compute the phase diagrams and the pressure due to the flavours of the theories as a function of these parameters and show that there are Roberge-Weiss transitions in the high temperature phases, chiral symmetry restore"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1103.2315","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":"1103.2315","created_at":"2026-05-18T02:22:19.917396+00:00"},{"alias_kind":"arxiv_version","alias_value":"1103.2315v3","created_at":"2026-05-18T02:22:19.917396+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1103.2315","created_at":"2026-05-18T02:22:19.917396+00:00"},{"alias_kind":"pith_short_12","alias_value":"WRQNPA2GBQC2","created_at":"2026-05-18T12:26:44.992195+00:00"},{"alias_kind":"pith_short_16","alias_value":"WRQNPA2GBQC2YIPN","created_at":"2026-05-18T12:26:44.992195+00:00"},{"alias_kind":"pith_short_8","alias_value":"WRQNPA2G","created_at":"2026-05-18T12:26:44.992195+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.07284","citing_title":"The Roberge-Weiss transition as a probe for conformality in many-flavor QCD","ref_index":97,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WRQNPA2GBQC2YIPNUOEPHHHKUD","json":"https://pith.science/pith/WRQNPA2GBQC2YIPNUOEPHHHKUD.json","graph_json":"https://pith.science/api/pith-number/WRQNPA2GBQC2YIPNUOEPHHHKUD/graph.json","events_json":"https://pith.science/api/pith-number/WRQNPA2GBQC2YIPNUOEPHHHKUD/events.json","paper":"https://pith.science/paper/WRQNPA2G"},"agent_actions":{"view_html":"https://pith.science/pith/WRQNPA2GBQC2YIPNUOEPHHHKUD","download_json":"https://pith.science/pith/WRQNPA2GBQC2YIPNUOEPHHHKUD.json","view_paper":"https://pith.science/paper/WRQNPA2G","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1103.2315&json=true","fetch_graph":"https://pith.science/api/pith-number/WRQNPA2GBQC2YIPNUOEPHHHKUD/graph.json","fetch_events":"https://pith.science/api/pith-number/WRQNPA2GBQC2YIPNUOEPHHHKUD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WRQNPA2GBQC2YIPNUOEPHHHKUD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WRQNPA2GBQC2YIPNUOEPHHHKUD/action/storage_attestation","attest_author":"https://pith.science/pith/WRQNPA2GBQC2YIPNUOEPHHHKUD/action/author_attestation","sign_citation":"https://pith.science/pith/WRQNPA2GBQC2YIPNUOEPHHHKUD/action/citation_signature","submit_replication":"https://pith.science/pith/WRQNPA2GBQC2YIPNUOEPHHHKUD/action/replication_record"}},"created_at":"2026-05-18T02:22:19.917396+00:00","updated_at":"2026-05-18T02:22:19.917396+00:00"}