{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:KHIZVWP3AGHOTKORN2QDTTBL7W","short_pith_number":"pith:KHIZVWP3","schema_version":"1.0","canonical_sha256":"51d19ad9fb018ee9a9d16ea039cc2bfda7a6886c7540fcc896fbfa75e617ab80","source":{"kind":"arxiv","id":"hep-th/0512101","version":2},"attestation_state":"computed","paper":{"title":"Half-BPS Geometries and Thermodynamics of Free Fermions","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Diego Trancanelli, Manuela Kulaxizi, Riccardo Ricci, Simone Giombi","submitted_at":"2005-12-08T20:36:08Z","abstract_excerpt":"Solutions of type IIB supergravity which preserve half of the supersymmetries have a dual description in terms of free fermions, as elucidated by the \"bubbling AdS\" construction of Lin, Lunin and Maldacena. In this paper we study the half-BPS geometry associated with a gas of free fermions in thermodynamic equilibrium obeying the Fermi-Dirac distribution. We consider both regimes of low and high temperature. In the former case, we present a detailed computation of the ADM mass of the supergravity solution and find agreement with the thermal energy of the fermions. The solution has a naked null"},"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/0512101","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2005-12-08T20:36:08Z","cross_cats_sorted":[],"title_canon_sha256":"194c0bc8c39a6a1528ed20ccc8b6aba565bd11af48adc287312eac3e8056731e","abstract_canon_sha256":"917c97ea38483f5b2072b85357876a23437c5591cea31b6c86dd81f995e75f14"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:20:49.926634Z","signature_b64":"wMrhgs3YzWaAFvQwZyAkHpe6ax617zdM1EjIDhwnm5IVNK9DKc/gcm20rO0MxQtOcMz2KYk5zibhd4U0hVe0DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"51d19ad9fb018ee9a9d16ea039cc2bfda7a6886c7540fcc896fbfa75e617ab80","last_reissued_at":"2026-07-04T17:20:49.926276Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:20:49.926276Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Half-BPS Geometries and Thermodynamics of Free Fermions","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Diego Trancanelli, Manuela Kulaxizi, Riccardo Ricci, Simone Giombi","submitted_at":"2005-12-08T20:36:08Z","abstract_excerpt":"Solutions of type IIB supergravity which preserve half of the supersymmetries have a dual description in terms of free fermions, as elucidated by the \"bubbling AdS\" construction of Lin, Lunin and Maldacena. In this paper we study the half-BPS geometry associated with a gas of free fermions in thermodynamic equilibrium obeying the Fermi-Dirac distribution. We consider both regimes of low and high temperature. In the former case, we present a detailed computation of the ADM mass of the supergravity solution and find agreement with the thermal energy of the fermions. The solution has a naked null"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0512101","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/0512101/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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/0512101","created_at":"2026-07-04T17:20:49.926334+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0512101v2","created_at":"2026-07-04T17:20:49.926334+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0512101","created_at":"2026-07-04T17:20:49.926334+00:00"},{"alias_kind":"pith_short_12","alias_value":"KHIZVWP3AGHO","created_at":"2026-07-04T17:20:49.926334+00:00"},{"alias_kind":"pith_short_16","alias_value":"KHIZVWP3AGHOTKOR","created_at":"2026-07-04T17:20:49.926334+00:00"},{"alias_kind":"pith_short_8","alias_value":"KHIZVWP3","created_at":"2026-07-04T17:20:49.926334+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/KHIZVWP3AGHOTKORN2QDTTBL7W","json":"https://pith.science/pith/KHIZVWP3AGHOTKORN2QDTTBL7W.json","graph_json":"https://pith.science/api/pith-number/KHIZVWP3AGHOTKORN2QDTTBL7W/graph.json","events_json":"https://pith.science/api/pith-number/KHIZVWP3AGHOTKORN2QDTTBL7W/events.json","paper":"https://pith.science/paper/KHIZVWP3"},"agent_actions":{"view_html":"https://pith.science/pith/KHIZVWP3AGHOTKORN2QDTTBL7W","download_json":"https://pith.science/pith/KHIZVWP3AGHOTKORN2QDTTBL7W.json","view_paper":"https://pith.science/paper/KHIZVWP3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0512101&json=true","fetch_graph":"https://pith.science/api/pith-number/KHIZVWP3AGHOTKORN2QDTTBL7W/graph.json","fetch_events":"https://pith.science/api/pith-number/KHIZVWP3AGHOTKORN2QDTTBL7W/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KHIZVWP3AGHOTKORN2QDTTBL7W/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KHIZVWP3AGHOTKORN2QDTTBL7W/action/storage_attestation","attest_author":"https://pith.science/pith/KHIZVWP3AGHOTKORN2QDTTBL7W/action/author_attestation","sign_citation":"https://pith.science/pith/KHIZVWP3AGHOTKORN2QDTTBL7W/action/citation_signature","submit_replication":"https://pith.science/pith/KHIZVWP3AGHOTKORN2QDTTBL7W/action/replication_record"}},"created_at":"2026-07-04T17:20:49.926334+00:00","updated_at":"2026-07-04T17:20:49.926334+00:00"}