{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1996:4DLXUWOIE6XTXGFX42ABEWNRCO","short_pith_number":"pith:4DLXUWOI","canonical_record":{"source":{"id":"hep-th/9610045","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1996-10-08T05:44:08Z","cross_cats_sorted":[],"title_canon_sha256":"2557c9c10806bda481ff5bf7b7a4fffa13037f2767fac72b74d70925d362604a","abstract_canon_sha256":"aafa1f800c0789fa852f35daacc4db2b647e770a59ec2d67aed86fa5b294a264"},"schema_version":"1.0"},"canonical_sha256":"e0d77a59c827af3b98b7e6801259b113b0f729099420d4b3e93f9c0b7486d240","source":{"kind":"arxiv","id":"hep-th/9610045","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9610045","created_at":"2026-07-04T17:25:41Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9610045v2","created_at":"2026-07-04T17:25:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9610045","created_at":"2026-07-04T17:25:41Z"},{"alias_kind":"pith_short_12","alias_value":"4DLXUWOIE6XT","created_at":"2026-07-04T17:25:41Z"},{"alias_kind":"pith_short_16","alias_value":"4DLXUWOIE6XTXGFX","created_at":"2026-07-04T17:25:41Z"},{"alias_kind":"pith_short_8","alias_value":"4DLXUWOI","created_at":"2026-07-04T17:25:41Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1996:4DLXUWOIE6XTXGFX42ABEWNRCO","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/9610045","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1996-10-08T05:44:08Z","cross_cats_sorted":[],"title_canon_sha256":"2557c9c10806bda481ff5bf7b7a4fffa13037f2767fac72b74d70925d362604a","abstract_canon_sha256":"aafa1f800c0789fa852f35daacc4db2b647e770a59ec2d67aed86fa5b294a264"},"schema_version":"1.0"},"canonical_sha256":"e0d77a59c827af3b98b7e6801259b113b0f729099420d4b3e93f9c0b7486d240","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:25:41.858457Z","signature_b64":"NKQVX0d5KNdfWILn3xUmNvSuxAcZ4cqqJN8EpPT0ubUMl4Lu/OXEoC6QUD7EEHjF/+8RZr7Ga2oL0N0ECWjlCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e0d77a59c827af3b98b7e6801259b113b0f729099420d4b3e93f9c0b7486d240","last_reissued_at":"2026-07-04T17:25:41.858039Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:25:41.858039Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/9610045","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T17:25:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Mcd70yH07pHCI9QCv2aKDsquV0NgXSlLfPraHZtl5jXLOYohthpYLjKFDCYPk7enOC2m0ahawhM5T+EFkRuMDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T19:14:27.919387Z"},"content_sha256":"530ed21fa39554f891d6d3d105bc4f0b3db84271d3aa3899a2533d9140118263","schema_version":"1.0","event_id":"sha256:530ed21fa39554f891d6d3d105bc4f0b3db84271d3aa3899a2533d9140118263"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1996:4DLXUWOIE6XTXGFX42ABEWNRCO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Microcanonical D-branes and Back Reaction","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Esko Keski-Vakkuri, Per Kraus (Cal Tech)","submitted_at":"1996-10-08T05:44:08Z","abstract_excerpt":"We compare the emission rates from excited D-branes in the microcanonical ensemble with back reaction corrected emission rates from black holes in field theory. In both cases, the rates in the high energy tail of the spectrum differ markedly from what a canonical ensemble or free field theory approach would yield. Instead of being proportional to a Bose-Einstein distribution function, the rates in the high energy tail are proportional to $\\exp (-\\Delta S_{BH})$ where $\\Delta S_{BH}$ is the difference in black hole entropies before and after emission. After including the new effects, we find ag"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9610045","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/9610045/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T17:25:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4PsXa8u685d7VwRpxBL2eqQGT1KrZ5kS3FUVpMMyf3PcC6JpYm++T1IlfQmEN8UtTWtwZlo5hlxu4ydtAwV7Aw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T19:14:27.919872Z"},"content_sha256":"7c6fe0a4578ade3deea208057156d752cf6d0d174d1f6b1a4e047c23aeae824f","schema_version":"1.0","event_id":"sha256:7c6fe0a4578ade3deea208057156d752cf6d0d174d1f6b1a4e047c23aeae824f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4DLXUWOIE6XTXGFX42ABEWNRCO/bundle.json","state_url":"https://pith.science/pith/4DLXUWOIE6XTXGFX42ABEWNRCO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4DLXUWOIE6XTXGFX42ABEWNRCO/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-03T19:14:27Z","links":{"resolver":"https://pith.science/pith/4DLXUWOIE6XTXGFX42ABEWNRCO","bundle":"https://pith.science/pith/4DLXUWOIE6XTXGFX42ABEWNRCO/bundle.json","state":"https://pith.science/pith/4DLXUWOIE6XTXGFX42ABEWNRCO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4DLXUWOIE6XTXGFX42ABEWNRCO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1996:4DLXUWOIE6XTXGFX42ABEWNRCO","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"aafa1f800c0789fa852f35daacc4db2b647e770a59ec2d67aed86fa5b294a264","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1996-10-08T05:44:08Z","title_canon_sha256":"2557c9c10806bda481ff5bf7b7a4fffa13037f2767fac72b74d70925d362604a"},"schema_version":"1.0","source":{"id":"hep-th/9610045","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9610045","created_at":"2026-07-04T17:25:41Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9610045v2","created_at":"2026-07-04T17:25:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9610045","created_at":"2026-07-04T17:25:41Z"},{"alias_kind":"pith_short_12","alias_value":"4DLXUWOIE6XT","created_at":"2026-07-04T17:25:41Z"},{"alias_kind":"pith_short_16","alias_value":"4DLXUWOIE6XTXGFX","created_at":"2026-07-04T17:25:41Z"},{"alias_kind":"pith_short_8","alias_value":"4DLXUWOI","created_at":"2026-07-04T17:25:41Z"}],"graph_snapshots":[{"event_id":"sha256:7c6fe0a4578ade3deea208057156d752cf6d0d174d1f6b1a4e047c23aeae824f","target":"graph","created_at":"2026-07-04T17:25:41Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-th/9610045/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We compare the emission rates from excited D-branes in the microcanonical ensemble with back reaction corrected emission rates from black holes in field theory. In both cases, the rates in the high energy tail of the spectrum differ markedly from what a canonical ensemble or free field theory approach would yield. Instead of being proportional to a Bose-Einstein distribution function, the rates in the high energy tail are proportional to $\\exp (-\\Delta S_{BH})$ where $\\Delta S_{BH}$ is the difference in black hole entropies before and after emission. After including the new effects, we find ag","authors_text":"Esko Keski-Vakkuri, Per Kraus (Cal Tech)","cross_cats":[],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"1996-10-08T05:44:08Z","title":"Microcanonical D-branes and Back Reaction"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9610045","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:530ed21fa39554f891d6d3d105bc4f0b3db84271d3aa3899a2533d9140118263","target":"record","created_at":"2026-07-04T17:25:41Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"aafa1f800c0789fa852f35daacc4db2b647e770a59ec2d67aed86fa5b294a264","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1996-10-08T05:44:08Z","title_canon_sha256":"2557c9c10806bda481ff5bf7b7a4fffa13037f2767fac72b74d70925d362604a"},"schema_version":"1.0","source":{"id":"hep-th/9610045","kind":"arxiv","version":2}},"canonical_sha256":"e0d77a59c827af3b98b7e6801259b113b0f729099420d4b3e93f9c0b7486d240","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e0d77a59c827af3b98b7e6801259b113b0f729099420d4b3e93f9c0b7486d240","first_computed_at":"2026-07-04T17:25:41.858039Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T17:25:41.858039Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"NKQVX0d5KNdfWILn3xUmNvSuxAcZ4cqqJN8EpPT0ubUMl4Lu/OXEoC6QUD7EEHjF/+8RZr7Ga2oL0N0ECWjlCw==","signature_status":"signed_v1","signed_at":"2026-07-04T17:25:41.858457Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/9610045","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:530ed21fa39554f891d6d3d105bc4f0b3db84271d3aa3899a2533d9140118263","sha256:7c6fe0a4578ade3deea208057156d752cf6d0d174d1f6b1a4e047c23aeae824f"],"state_sha256":"4b4f4589fc4937b9d186832f66b87e3bc7423410bc2995baae9d9e14d3c6f607"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7K6H2cPkzZOyCVCG1TjbjLPSvcNPDW5yxMuFw7wKP0jHRoI0fGfxX7sVdL3bL95UjeiP8Wzg+FO+qfAoV79pCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-03T19:14:27.928570Z","bundle_sha256":"823ab898872dcb8c091195d134db6d041ac36a50024c872616c0c7886212e868"}}