{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:ITE37LQS7H7XC3AJGPOU4DBD4Z","short_pith_number":"pith:ITE37LQS","schema_version":"1.0","canonical_sha256":"44c9bfae12f9ff716c0933dd4e0c23e65ef775a7be1ce9a8fc822e09f1f23194","source":{"kind":"arxiv","id":"1811.08646","version":1},"attestation_state":"computed","paper":{"title":"Comments on deconfinement in AdS/CFT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Joonho Kim, June Nahmgoong, Seok Kim, Sunjin Choi","submitted_at":"2018-11-21T09:21:14Z","abstract_excerpt":"We study the index of $\\mathcal{N}=4$ Yang-Mills theory on $S^3\\times\\mathbb{R}$. We argue that the index should undergo a large $N$ deconfinement phase transition, by computing an upper bound of its `temperature.' We compute this bound by optimizing the phases of fugacities. The bound we find has some features analogous to the Hagedorn temperature. We briefly discuss a possible mechanism of the actual deconfinement transition below our bound. Our upper bound is lower than the Hawking-Page transition `temperature' of known BPS black holes in the AdS$_5$ dual. We thus expect the existence of ne"},"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":"1811.08646","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-11-21T09:21:14Z","cross_cats_sorted":[],"title_canon_sha256":"406880031c900c6a6f75cfe5c77a32686794c1ec43f41faed7ea8a8ba3752c70","abstract_canon_sha256":"552e7e40fddc99a786ac023fcd8373f2f4885ea2680303114844db0dcc1ea648"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:00:11.985926Z","signature_b64":"apc/5BFrbAJPLKHwLvKdHkmFuvkstzE/jVqqMoG8oPthLOJC0eCEcS66pHnCem+nCotX5twHp7npWhUfVr+iAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"44c9bfae12f9ff716c0933dd4e0c23e65ef775a7be1ce9a8fc822e09f1f23194","last_reissued_at":"2026-05-18T00:00:11.985449Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:00:11.985449Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Comments on deconfinement in AdS/CFT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Joonho Kim, June Nahmgoong, Seok Kim, Sunjin Choi","submitted_at":"2018-11-21T09:21:14Z","abstract_excerpt":"We study the index of $\\mathcal{N}=4$ Yang-Mills theory on $S^3\\times\\mathbb{R}$. We argue that the index should undergo a large $N$ deconfinement phase transition, by computing an upper bound of its `temperature.' We compute this bound by optimizing the phases of fugacities. The bound we find has some features analogous to the Hagedorn temperature. We briefly discuss a possible mechanism of the actual deconfinement transition below our bound. Our upper bound is lower than the Hawking-Page transition `temperature' of known BPS black holes in the AdS$_5$ dual. We thus expect the existence of ne"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.08646","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":"1811.08646","created_at":"2026-05-18T00:00:11.985518+00:00"},{"alias_kind":"arxiv_version","alias_value":"1811.08646v1","created_at":"2026-05-18T00:00:11.985518+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.08646","created_at":"2026-05-18T00:00:11.985518+00:00"},{"alias_kind":"pith_short_12","alias_value":"ITE37LQS7H7X","created_at":"2026-05-18T12:32:31.084164+00:00"},{"alias_kind":"pith_short_16","alias_value":"ITE37LQS7H7XC3AJ","created_at":"2026-05-18T12:32:31.084164+00:00"},{"alias_kind":"pith_short_8","alias_value":"ITE37LQS","created_at":"2026-05-18T12:32:31.084164+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2508.05322","citing_title":"Explorations of Universality in the Entropy and Hawking Radiation of Non-Extremal Kerr AdS$_4$ Black Holes","ref_index":13,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ITE37LQS7H7XC3AJGPOU4DBD4Z","json":"https://pith.science/pith/ITE37LQS7H7XC3AJGPOU4DBD4Z.json","graph_json":"https://pith.science/api/pith-number/ITE37LQS7H7XC3AJGPOU4DBD4Z/graph.json","events_json":"https://pith.science/api/pith-number/ITE37LQS7H7XC3AJGPOU4DBD4Z/events.json","paper":"https://pith.science/paper/ITE37LQS"},"agent_actions":{"view_html":"https://pith.science/pith/ITE37LQS7H7XC3AJGPOU4DBD4Z","download_json":"https://pith.science/pith/ITE37LQS7H7XC3AJGPOU4DBD4Z.json","view_paper":"https://pith.science/paper/ITE37LQS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1811.08646&json=true","fetch_graph":"https://pith.science/api/pith-number/ITE37LQS7H7XC3AJGPOU4DBD4Z/graph.json","fetch_events":"https://pith.science/api/pith-number/ITE37LQS7H7XC3AJGPOU4DBD4Z/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ITE37LQS7H7XC3AJGPOU4DBD4Z/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ITE37LQS7H7XC3AJGPOU4DBD4Z/action/storage_attestation","attest_author":"https://pith.science/pith/ITE37LQS7H7XC3AJGPOU4DBD4Z/action/author_attestation","sign_citation":"https://pith.science/pith/ITE37LQS7H7XC3AJGPOU4DBD4Z/action/citation_signature","submit_replication":"https://pith.science/pith/ITE37LQS7H7XC3AJGPOU4DBD4Z/action/replication_record"}},"created_at":"2026-05-18T00:00:11.985518+00:00","updated_at":"2026-05-18T00:00:11.985518+00:00"}