{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:A3HMYW7NTXO5E5GNPJDFRCDAQ2","short_pith_number":"pith:A3HMYW7N","schema_version":"1.0","canonical_sha256":"06cecc5bed9dddd274cd7a46588860869b854e736c4a84f4f059b03ce50fce8b","source":{"kind":"arxiv","id":"hep-th/0106201","version":2},"attestation_state":"computed","paper":{"title":"Brane-Antibrane Systems at Finite Temperature and the Entropy of Black Branes","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alberto Guijosa, Martin Kruczenski, Ulf H. Danielsson","submitted_at":"2001-06-22T16:52:41Z","abstract_excerpt":"We consider D-brane/anti-D-brane systems at T>0. Starting at the closed string vacuum, we argue that a finite temperature leads to the reappearance of open string degrees of freedom. We also show that, at a sufficiently large temperature, the open string vacuum becomes stable. Building upon this observation and previous work by Horowitz, Maldacena and Strominger, we formulate a microscopic brane-antibrane model for the non-extremal black three-brane in ten dimensions (as well as for the black two- and five-branes in eleven dimensions). Under reasonable assumptions, and using known results from"},"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/0106201","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2001-06-22T16:52:41Z","cross_cats_sorted":[],"title_canon_sha256":"58a7fb4027acbeecc80e2e9018a96dc4875f47311043df82e7471f29afdbc427","abstract_canon_sha256":"b15c3db38fdd979d2a220a7ae61a72dd772ae4e7cb8cdd877b932671407fc20b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:21:05.864425Z","signature_b64":"sreKCG4/PnmoeDvs3ZQzC7nwNW1a6qqF1hQrcliyjxAIDMSChPKuZXnwyDumTajbeIpwZIBcXMN0HFEeveZZCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"06cecc5bed9dddd274cd7a46588860869b854e736c4a84f4f059b03ce50fce8b","last_reissued_at":"2026-07-04T17:21:05.863957Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:21:05.863957Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Brane-Antibrane Systems at Finite Temperature and the Entropy of Black Branes","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alberto Guijosa, Martin Kruczenski, Ulf H. Danielsson","submitted_at":"2001-06-22T16:52:41Z","abstract_excerpt":"We consider D-brane/anti-D-brane systems at T>0. Starting at the closed string vacuum, we argue that a finite temperature leads to the reappearance of open string degrees of freedom. We also show that, at a sufficiently large temperature, the open string vacuum becomes stable. Building upon this observation and previous work by Horowitz, Maldacena and Strominger, we formulate a microscopic brane-antibrane model for the non-extremal black three-brane in ten dimensions (as well as for the black two- and five-branes in eleven dimensions). Under reasonable assumptions, and using known results from"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0106201","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/0106201/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/0106201","created_at":"2026-07-04T17:21:05.864017+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0106201v2","created_at":"2026-07-04T17:21:05.864017+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0106201","created_at":"2026-07-04T17:21:05.864017+00:00"},{"alias_kind":"pith_short_12","alias_value":"A3HMYW7NTXO5","created_at":"2026-07-04T17:21:05.864017+00:00"},{"alias_kind":"pith_short_16","alias_value":"A3HMYW7NTXO5E5GN","created_at":"2026-07-04T17:21:05.864017+00:00"},{"alias_kind":"pith_short_8","alias_value":"A3HMYW7N","created_at":"2026-07-04T17:21:05.864017+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.11096","citing_title":"An extremal black hole with a unique ground state","ref_index":31,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/A3HMYW7NTXO5E5GNPJDFRCDAQ2","json":"https://pith.science/pith/A3HMYW7NTXO5E5GNPJDFRCDAQ2.json","graph_json":"https://pith.science/api/pith-number/A3HMYW7NTXO5E5GNPJDFRCDAQ2/graph.json","events_json":"https://pith.science/api/pith-number/A3HMYW7NTXO5E5GNPJDFRCDAQ2/events.json","paper":"https://pith.science/paper/A3HMYW7N"},"agent_actions":{"view_html":"https://pith.science/pith/A3HMYW7NTXO5E5GNPJDFRCDAQ2","download_json":"https://pith.science/pith/A3HMYW7NTXO5E5GNPJDFRCDAQ2.json","view_paper":"https://pith.science/paper/A3HMYW7N","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0106201&json=true","fetch_graph":"https://pith.science/api/pith-number/A3HMYW7NTXO5E5GNPJDFRCDAQ2/graph.json","fetch_events":"https://pith.science/api/pith-number/A3HMYW7NTXO5E5GNPJDFRCDAQ2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/A3HMYW7NTXO5E5GNPJDFRCDAQ2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/A3HMYW7NTXO5E5GNPJDFRCDAQ2/action/storage_attestation","attest_author":"https://pith.science/pith/A3HMYW7NTXO5E5GNPJDFRCDAQ2/action/author_attestation","sign_citation":"https://pith.science/pith/A3HMYW7NTXO5E5GNPJDFRCDAQ2/action/citation_signature","submit_replication":"https://pith.science/pith/A3HMYW7NTXO5E5GNPJDFRCDAQ2/action/replication_record"}},"created_at":"2026-07-04T17:21:05.864017+00:00","updated_at":"2026-07-04T17:21:05.864017+00:00"}