{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:I4GW2FQTUQDXXUOPSJ7JKN5U3V","short_pith_number":"pith:I4GW2FQT","canonical_record":{"source":{"id":"1409.5548","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2014-09-19T08:37:25Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"ab263acd5967d380e7004f9b4163c3e0097be4aa383c0d3a9def77549b36a4a9","abstract_canon_sha256":"c24f9be2f104002854fb7a2e675de5f5b1be0580de488bf2a8aabdaa454862ab"},"schema_version":"1.0"},"canonical_sha256":"470d6d1613a4077bd1cf927e9537b4dd796ca80e25af1bab5ad70fa0a109cdd6","source":{"kind":"arxiv","id":"1409.5548","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.5548","created_at":"2026-05-18T02:25:41Z"},{"alias_kind":"arxiv_version","alias_value":"1409.5548v2","created_at":"2026-05-18T02:25:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.5548","created_at":"2026-05-18T02:25:41Z"},{"alias_kind":"pith_short_12","alias_value":"I4GW2FQTUQDX","created_at":"2026-05-18T12:28:33Z"},{"alias_kind":"pith_short_16","alias_value":"I4GW2FQTUQDXXUOP","created_at":"2026-05-18T12:28:33Z"},{"alias_kind":"pith_short_8","alias_value":"I4GW2FQT","created_at":"2026-05-18T12:28:33Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:I4GW2FQTUQDXXUOPSJ7JKN5U3V","target":"record","payload":{"canonical_record":{"source":{"id":"1409.5548","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2014-09-19T08:37:25Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"ab263acd5967d380e7004f9b4163c3e0097be4aa383c0d3a9def77549b36a4a9","abstract_canon_sha256":"c24f9be2f104002854fb7a2e675de5f5b1be0580de488bf2a8aabdaa454862ab"},"schema_version":"1.0"},"canonical_sha256":"470d6d1613a4077bd1cf927e9537b4dd796ca80e25af1bab5ad70fa0a109cdd6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:25:41.895550Z","signature_b64":"EiZ1piBnDL89uYhMXENuZ1uhZTbBdtSCcX/HLyfXIqNPQfyGihhh0MEYGN3E+3l2/zpQXOufGkvvmT4K8k84Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"470d6d1613a4077bd1cf927e9537b4dd796ca80e25af1bab5ad70fa0a109cdd6","last_reissued_at":"2026-05-18T02:25:41.895055Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:25:41.895055Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1409.5548","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":"2026-05-18T02:25:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vgs8QiTHqjXOFbh2lMHu7WQKP1Lql4UE8J3amLFxgfJ2S3Eu8sFT2f8BCstt37TlwCRJgRzki1IyQ0jQ4IkFCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T23:59:27.932266Z"},"content_sha256":"3bfcd2c4005c3e796787530b57e7f9153d193519bcfce924abe0c006970d36c1","schema_version":"1.0","event_id":"sha256:3bfcd2c4005c3e796787530b57e7f9153d193519bcfce924abe0c006970d36c1"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:I4GW2FQTUQDXXUOPSJ7JKN5U3V","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Thermodynamic phase transition based on the non-singular temperature","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"Myungseok Eune, Wontae Kim, Yongwan Gim","submitted_at":"2014-09-19T08:37:25Z","abstract_excerpt":"The Hawking temperature for the Schwarzschild black hole is divergent when the mass of the black hole vanishes; however the corresponding geometry becomes the Minkowski spacetime whose intrinsic temperature is zero. In connection with this issue, we construct a non-singular temperature which follows the Hawking temperature for the large black hole while it vanishes when the black hole completely evaporated. In order for thermodynamic significances of this modified temperature, we calculate thermodynamic quantities and study phase transitions. It turns out that even the small black hole can be "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.5548","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":""},"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":"2026-05-18T02:25:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"div1ScF93QXy9+9fIwHlEQa6PRqltOdTzh0RyVyKO00fKRT0fwAk7MOo7FfpebFw0MypoWlHSZMR1HJXkiSJDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T23:59:27.932935Z"},"content_sha256":"66bce5638dd61eed5f216be8d9930fda36ecb1e6c9b7d0b9c79d910300dbd9a6","schema_version":"1.0","event_id":"sha256:66bce5638dd61eed5f216be8d9930fda36ecb1e6c9b7d0b9c79d910300dbd9a6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/I4GW2FQTUQDXXUOPSJ7JKN5U3V/bundle.json","state_url":"https://pith.science/pith/I4GW2FQTUQDXXUOPSJ7JKN5U3V/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/I4GW2FQTUQDXXUOPSJ7JKN5U3V/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":"2026-06-11T23:59:27Z","links":{"resolver":"https://pith.science/pith/I4GW2FQTUQDXXUOPSJ7JKN5U3V","bundle":"https://pith.science/pith/I4GW2FQTUQDXXUOPSJ7JKN5U3V/bundle.json","state":"https://pith.science/pith/I4GW2FQTUQDXXUOPSJ7JKN5U3V/state.json","well_known_bundle":"https://pith.science/.well-known/pith/I4GW2FQTUQDXXUOPSJ7JKN5U3V/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:I4GW2FQTUQDXXUOPSJ7JKN5U3V","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":"c24f9be2f104002854fb7a2e675de5f5b1be0580de488bf2a8aabdaa454862ab","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2014-09-19T08:37:25Z","title_canon_sha256":"ab263acd5967d380e7004f9b4163c3e0097be4aa383c0d3a9def77549b36a4a9"},"schema_version":"1.0","source":{"id":"1409.5548","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.5548","created_at":"2026-05-18T02:25:41Z"},{"alias_kind":"arxiv_version","alias_value":"1409.5548v2","created_at":"2026-05-18T02:25:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.5548","created_at":"2026-05-18T02:25:41Z"},{"alias_kind":"pith_short_12","alias_value":"I4GW2FQTUQDX","created_at":"2026-05-18T12:28:33Z"},{"alias_kind":"pith_short_16","alias_value":"I4GW2FQTUQDXXUOP","created_at":"2026-05-18T12:28:33Z"},{"alias_kind":"pith_short_8","alias_value":"I4GW2FQT","created_at":"2026-05-18T12:28:33Z"}],"graph_snapshots":[{"event_id":"sha256:66bce5638dd61eed5f216be8d9930fda36ecb1e6c9b7d0b9c79d910300dbd9a6","target":"graph","created_at":"2026-05-18T02:25:41Z","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"},"paper":{"abstract_excerpt":"The Hawking temperature for the Schwarzschild black hole is divergent when the mass of the black hole vanishes; however the corresponding geometry becomes the Minkowski spacetime whose intrinsic temperature is zero. In connection with this issue, we construct a non-singular temperature which follows the Hawking temperature for the large black hole while it vanishes when the black hole completely evaporated. In order for thermodynamic significances of this modified temperature, we calculate thermodynamic quantities and study phase transitions. It turns out that even the small black hole can be ","authors_text":"Myungseok Eune, Wontae Kim, Yongwan Gim","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2014-09-19T08:37:25Z","title":"Thermodynamic phase transition based on the non-singular temperature"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.5548","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":"sha256:3bfcd2c4005c3e796787530b57e7f9153d193519bcfce924abe0c006970d36c1","target":"record","created_at":"2026-05-18T02:25:41Z","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":"c24f9be2f104002854fb7a2e675de5f5b1be0580de488bf2a8aabdaa454862ab","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2014-09-19T08:37:25Z","title_canon_sha256":"ab263acd5967d380e7004f9b4163c3e0097be4aa383c0d3a9def77549b36a4a9"},"schema_version":"1.0","source":{"id":"1409.5548","kind":"arxiv","version":2}},"canonical_sha256":"470d6d1613a4077bd1cf927e9537b4dd796ca80e25af1bab5ad70fa0a109cdd6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"470d6d1613a4077bd1cf927e9537b4dd796ca80e25af1bab5ad70fa0a109cdd6","first_computed_at":"2026-05-18T02:25:41.895055Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:25:41.895055Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"EiZ1piBnDL89uYhMXENuZ1uhZTbBdtSCcX/HLyfXIqNPQfyGihhh0MEYGN3E+3l2/zpQXOufGkvvmT4K8k84Bg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:25:41.895550Z","signed_message":"canonical_sha256_bytes"},"source_id":"1409.5548","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3bfcd2c4005c3e796787530b57e7f9153d193519bcfce924abe0c006970d36c1","sha256:66bce5638dd61eed5f216be8d9930fda36ecb1e6c9b7d0b9c79d910300dbd9a6"],"state_sha256":"fa9b39d9102f2023d37f718d8917be0cb1dbcaeb185a090d709f06cc8b8da8e2"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3ci0vcN37DOvXhFNHH3uR8EYDgJOocrreh+ZvjNPaXXY02OMOi3XegEPk8DOU+cDXYOxEDJFrgnpesRrilcQDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-11T23:59:27.936999Z","bundle_sha256":"8c257c888df32e0f63726742bae386ee3e2bdecc9f952cb177ad621837a4e7dd"}}