{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:3DDROBDAL7SPU3TB25ZB25JL4D","short_pith_number":"pith:3DDROBDA","canonical_record":{"source":{"id":"1812.11231","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-12-28T21:58:07Z","cross_cats_sorted":[],"title_canon_sha256":"ca0a3776ae16c8d6bb4017006bf3de72b3d501050c4bb555713a33d86dbfc7e8","abstract_canon_sha256":"0b1fa07c194e65a5013f84cf3d019ad2b3cf404bef82fc1a9c9fc76a164772c5"},"schema_version":"1.0"},"canonical_sha256":"d8c71704605fe4fa6e61d7721d752be0dfc93b1e1303154f6e81c785d4e4dfee","source":{"kind":"arxiv","id":"1812.11231","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1812.11231","created_at":"2026-05-17T23:44:02Z"},{"alias_kind":"arxiv_version","alias_value":"1812.11231v3","created_at":"2026-05-17T23:44:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.11231","created_at":"2026-05-17T23:44:02Z"},{"alias_kind":"pith_short_12","alias_value":"3DDROBDAL7SP","created_at":"2026-05-18T12:32:02Z"},{"alias_kind":"pith_short_16","alias_value":"3DDROBDAL7SPU3TB","created_at":"2026-05-18T12:32:02Z"},{"alias_kind":"pith_short_8","alias_value":"3DDROBDA","created_at":"2026-05-18T12:32:02Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:3DDROBDAL7SPU3TB25ZB25JL4D","target":"record","payload":{"canonical_record":{"source":{"id":"1812.11231","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-12-28T21:58:07Z","cross_cats_sorted":[],"title_canon_sha256":"ca0a3776ae16c8d6bb4017006bf3de72b3d501050c4bb555713a33d86dbfc7e8","abstract_canon_sha256":"0b1fa07c194e65a5013f84cf3d019ad2b3cf404bef82fc1a9c9fc76a164772c5"},"schema_version":"1.0"},"canonical_sha256":"d8c71704605fe4fa6e61d7721d752be0dfc93b1e1303154f6e81c785d4e4dfee","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:44:02.566245Z","signature_b64":"qVmCzPabp59JuC4nkAxUk/zEaG9ErhbpYGCgUIoShH4jMCMp2u1nh0mXVS/fiDbocTfXCiuEfaSmiTcuKJ6FAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d8c71704605fe4fa6e61d7721d752be0dfc93b1e1303154f6e81c785d4e4dfee","last_reissued_at":"2026-05-17T23:44:02.565853Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:44:02.565853Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1812.11231","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:44:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7Trp2mLEDyQy8Nr/uSrzZhA6Q1GHiGzOmdVE3TgxqJNrpsitzueP33KuYOl5uRmBjlDKXbdJ9KXALOpf2qUgAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T10:41:44.140765Z"},"content_sha256":"23e8e8c22b56a96cc845267fbcb7af23176176a7130078de9e78bf1b25922416","schema_version":"1.0","event_id":"sha256:23e8e8c22b56a96cc845267fbcb7af23176176a7130078de9e78bf1b25922416"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:3DDROBDAL7SPU3TB25ZB25JL4D","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Meronic Einstein-Yang-Mills black hole in 5D and gravitational spin from isospin effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Andr\\'es Gomberoff, Fabrizio Canfora, Francisco Rojas, Patricio Salgado-Rebolledo, Seung Hun Oh","submitted_at":"2018-12-28T21:58:07Z","abstract_excerpt":"We construct an analytic black hole solution in $SU(2)$ Einstein-Yang-Mills theory in five dimensions supporting a Meron field. The gauge field is proportional to a pure gauge and has a non-trivial topological charge. The would-be singularity at the Meron core gets shielded from the exterior by the black hole horizon. The metric has only one integration constant, namely, its ADM mass, which is shown to be finite once an appropriate boundary term is added to the action. The thermodynamics is also worked out, and a first-order phase transition, similar to the one occurring in the Reissner-Nordst"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.11231","kind":"arxiv","version":3},"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":"2026-05-17T23:44:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SLZg5j7n/8hudOfje9cv2z+1PpiPX4aTGSlEy4gav7K060DQHjSwYpFUCu+rDY6izDBsVhWSO+dy8OrNXvN7Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T10:41:44.141559Z"},"content_sha256":"39f05778776e08e9f2293fe475625dbf99430de77361fd8d4cda0deeabba180b","schema_version":"1.0","event_id":"sha256:39f05778776e08e9f2293fe475625dbf99430de77361fd8d4cda0deeabba180b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3DDROBDAL7SPU3TB25ZB25JL4D/bundle.json","state_url":"https://pith.science/pith/3DDROBDAL7SPU3TB25ZB25JL4D/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3DDROBDAL7SPU3TB25ZB25JL4D/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":"2026-08-11T10:41:44Z","links":{"resolver":"https://pith.science/pith/3DDROBDAL7SPU3TB25ZB25JL4D","bundle":"https://pith.science/pith/3DDROBDAL7SPU3TB25ZB25JL4D/bundle.json","state":"https://pith.science/pith/3DDROBDAL7SPU3TB25ZB25JL4D/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3DDROBDAL7SPU3TB25ZB25JL4D/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:3DDROBDAL7SPU3TB25ZB25JL4D","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":"0b1fa07c194e65a5013f84cf3d019ad2b3cf404bef82fc1a9c9fc76a164772c5","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-12-28T21:58:07Z","title_canon_sha256":"ca0a3776ae16c8d6bb4017006bf3de72b3d501050c4bb555713a33d86dbfc7e8"},"schema_version":"1.0","source":{"id":"1812.11231","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1812.11231","created_at":"2026-05-17T23:44:02Z"},{"alias_kind":"arxiv_version","alias_value":"1812.11231v3","created_at":"2026-05-17T23:44:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.11231","created_at":"2026-05-17T23:44:02Z"},{"alias_kind":"pith_short_12","alias_value":"3DDROBDAL7SP","created_at":"2026-05-18T12:32:02Z"},{"alias_kind":"pith_short_16","alias_value":"3DDROBDAL7SPU3TB","created_at":"2026-05-18T12:32:02Z"},{"alias_kind":"pith_short_8","alias_value":"3DDROBDA","created_at":"2026-05-18T12:32:02Z"}],"graph_snapshots":[{"event_id":"sha256:39f05778776e08e9f2293fe475625dbf99430de77361fd8d4cda0deeabba180b","target":"graph","created_at":"2026-05-17T23:44:02Z","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":"We construct an analytic black hole solution in $SU(2)$ Einstein-Yang-Mills theory in five dimensions supporting a Meron field. The gauge field is proportional to a pure gauge and has a non-trivial topological charge. The would-be singularity at the Meron core gets shielded from the exterior by the black hole horizon. The metric has only one integration constant, namely, its ADM mass, which is shown to be finite once an appropriate boundary term is added to the action. The thermodynamics is also worked out, and a first-order phase transition, similar to the one occurring in the Reissner-Nordst","authors_text":"Andr\\'es Gomberoff, Fabrizio Canfora, Francisco Rojas, Patricio Salgado-Rebolledo, Seung Hun Oh","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-12-28T21:58:07Z","title":"Meronic Einstein-Yang-Mills black hole in 5D and gravitational spin from isospin effect"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.11231","kind":"arxiv","version":3},"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":"sha256:23e8e8c22b56a96cc845267fbcb7af23176176a7130078de9e78bf1b25922416","target":"record","created_at":"2026-05-17T23:44:02Z","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":"0b1fa07c194e65a5013f84cf3d019ad2b3cf404bef82fc1a9c9fc76a164772c5","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-12-28T21:58:07Z","title_canon_sha256":"ca0a3776ae16c8d6bb4017006bf3de72b3d501050c4bb555713a33d86dbfc7e8"},"schema_version":"1.0","source":{"id":"1812.11231","kind":"arxiv","version":3}},"canonical_sha256":"d8c71704605fe4fa6e61d7721d752be0dfc93b1e1303154f6e81c785d4e4dfee","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d8c71704605fe4fa6e61d7721d752be0dfc93b1e1303154f6e81c785d4e4dfee","first_computed_at":"2026-05-17T23:44:02.565853Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:44:02.565853Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"qVmCzPabp59JuC4nkAxUk/zEaG9ErhbpYGCgUIoShH4jMCMp2u1nh0mXVS/fiDbocTfXCiuEfaSmiTcuKJ6FAQ==","signature_status":"signed_v1","signed_at":"2026-05-17T23:44:02.566245Z","signed_message":"canonical_sha256_bytes"},"source_id":"1812.11231","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:23e8e8c22b56a96cc845267fbcb7af23176176a7130078de9e78bf1b25922416","sha256:39f05778776e08e9f2293fe475625dbf99430de77361fd8d4cda0deeabba180b"],"state_sha256":"b81d082b6b1587d9f672659ca288ae2374c04e79d1dcd4a2d68ae9cf085e7ca0"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zbo0GE67H02TMMRw9ZBDydhqdEiV1ZS/b4wv+AfGVulRA9WNdUlUdfchXqIoVfU8DfbAc7tIQwSLfAwv48JLCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-11T10:41:44.147926Z","bundle_sha256":"e324cb922e4da9b56fc1beffbf4f17b22550767b1e7826f3d4d49f58e14d5cf2"}}