{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:VD2RA46LG436ZI4PPENUMPJ6DJ","short_pith_number":"pith:VD2RA46L","canonical_record":{"source":{"id":"1004.3574","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2010-04-20T20:59:24Z","cross_cats_sorted":["astro-ph.SR","hep-th"],"title_canon_sha256":"ffbe2332ad8e8a22df2e3b28f41101b3081c2636a25ee7b4e50db918c42d5a6a","abstract_canon_sha256":"b55e7d3ec01b5c1c759ba6c5583aecf6e6234f25ef2ca2929245ca4a7f0a4455"},"schema_version":"1.0"},"canonical_sha256":"a8f51073cb3737eca38f791b463d3e1a41a67e6f31c2d8bfb827ffb9e98c61ce","source":{"kind":"arxiv","id":"1004.3574","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1004.3574","created_at":"2026-05-18T02:24:16Z"},{"alias_kind":"arxiv_version","alias_value":"1004.3574v2","created_at":"2026-05-18T02:24:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1004.3574","created_at":"2026-05-18T02:24:16Z"},{"alias_kind":"pith_short_12","alias_value":"VD2RA46LG436","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_16","alias_value":"VD2RA46LG436ZI4P","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_8","alias_value":"VD2RA46L","created_at":"2026-05-18T12:26:15Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:VD2RA46LG436ZI4PPENUMPJ6DJ","target":"record","payload":{"canonical_record":{"source":{"id":"1004.3574","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2010-04-20T20:59:24Z","cross_cats_sorted":["astro-ph.SR","hep-th"],"title_canon_sha256":"ffbe2332ad8e8a22df2e3b28f41101b3081c2636a25ee7b4e50db918c42d5a6a","abstract_canon_sha256":"b55e7d3ec01b5c1c759ba6c5583aecf6e6234f25ef2ca2929245ca4a7f0a4455"},"schema_version":"1.0"},"canonical_sha256":"a8f51073cb3737eca38f791b463d3e1a41a67e6f31c2d8bfb827ffb9e98c61ce","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:24:16.382874Z","signature_b64":"4qaKhZdfdANDeMH+8reP5q1/IfMTB/VoALx6GpPGLtrDePs/c8qjyi4g8yjTwE8EC7kITt9JMk+yy0Mcd19pAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a8f51073cb3737eca38f791b463d3e1a41a67e6f31c2d8bfb827ffb9e98c61ce","last_reissued_at":"2026-05-18T02:24:16.382124Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:24:16.382124Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1004.3574","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":"2026-05-18T02:24:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HzjMU8GFxeiSZzw/YRenYiHLhUWEIQPcCw1aBEo4dnop+ADrvLaySVA1zpWuq0kefmT0u0QjEiscFmhkQEdLDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T20:23:22.102926Z"},"content_sha256":"5f559f04e5bd75d7ca9126e0b7a529c21c8edca3252b260ad3d0b858aef4e88f","schema_version":"1.0","event_id":"sha256:5f559f04e5bd75d7ca9126e0b7a529c21c8edca3252b260ad3d0b858aef4e88f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:VD2RA46LG436ZI4PPENUMPJ6DJ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quasiblack holes with pressure: relativistic charged spheres as the frozen stars","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.SR","hep-th"],"primary_cat":"gr-qc","authors_text":"Jos\\'e P. S. Lemos, Vilson T. Zanchin","submitted_at":"2010-04-20T20:59:24Z","abstract_excerpt":"In general relativity coupled to Maxwell's electromagnetism and charged matter, when the gravitational potential $W^2$ and the electric potential field $\\phi$ obey a relation of the form $W^{2}= a\\left(-\\epsilon\\, \\phi+ b\\right)^2 +c$, where $a$, $b$ and $c$ are arbitrary constants, and $\\epsilon=\\pm1$ (the speed of light $c$ and Newton's constant $G$ are put to one), a class of very interesting electrically charged systems with pressure arises. We call the relation above between $W$ and $\\phi$, the Weyl-Guilfoyle relation, and it generalizes the usual Weyl relation, for which $a=1$. For both,"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1004.3574","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":"2026-05-18T02:24:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"k/nI9rsANms0/tVFgoL4ofrJtiS60uHao+lDlGxMwedhJ9J0t3y7ofhNOVnA+NjBaBjHjVqaPpyu/CCmnMFuCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T20:23:22.103300Z"},"content_sha256":"23c3e57289e640b5c08061db8aed8ec50ed47b79356d262a82c545e00a942016","schema_version":"1.0","event_id":"sha256:23c3e57289e640b5c08061db8aed8ec50ed47b79356d262a82c545e00a942016"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VD2RA46LG436ZI4PPENUMPJ6DJ/bundle.json","state_url":"https://pith.science/pith/VD2RA46LG436ZI4PPENUMPJ6DJ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VD2RA46LG436ZI4PPENUMPJ6DJ/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":"2026-05-25T20:23:22Z","links":{"resolver":"https://pith.science/pith/VD2RA46LG436ZI4PPENUMPJ6DJ","bundle":"https://pith.science/pith/VD2RA46LG436ZI4PPENUMPJ6DJ/bundle.json","state":"https://pith.science/pith/VD2RA46LG436ZI4PPENUMPJ6DJ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VD2RA46LG436ZI4PPENUMPJ6DJ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:VD2RA46LG436ZI4PPENUMPJ6DJ","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":"b55e7d3ec01b5c1c759ba6c5583aecf6e6234f25ef2ca2929245ca4a7f0a4455","cross_cats_sorted":["astro-ph.SR","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2010-04-20T20:59:24Z","title_canon_sha256":"ffbe2332ad8e8a22df2e3b28f41101b3081c2636a25ee7b4e50db918c42d5a6a"},"schema_version":"1.0","source":{"id":"1004.3574","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1004.3574","created_at":"2026-05-18T02:24:16Z"},{"alias_kind":"arxiv_version","alias_value":"1004.3574v2","created_at":"2026-05-18T02:24:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1004.3574","created_at":"2026-05-18T02:24:16Z"},{"alias_kind":"pith_short_12","alias_value":"VD2RA46LG436","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_16","alias_value":"VD2RA46LG436ZI4P","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_8","alias_value":"VD2RA46L","created_at":"2026-05-18T12:26:15Z"}],"graph_snapshots":[{"event_id":"sha256:23c3e57289e640b5c08061db8aed8ec50ed47b79356d262a82c545e00a942016","target":"graph","created_at":"2026-05-18T02:24:16Z","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":"In general relativity coupled to Maxwell's electromagnetism and charged matter, when the gravitational potential $W^2$ and the electric potential field $\\phi$ obey a relation of the form $W^{2}= a\\left(-\\epsilon\\, \\phi+ b\\right)^2 +c$, where $a$, $b$ and $c$ are arbitrary constants, and $\\epsilon=\\pm1$ (the speed of light $c$ and Newton's constant $G$ are put to one), a class of very interesting electrically charged systems with pressure arises. We call the relation above between $W$ and $\\phi$, the Weyl-Guilfoyle relation, and it generalizes the usual Weyl relation, for which $a=1$. For both,","authors_text":"Jos\\'e P. S. Lemos, Vilson T. Zanchin","cross_cats":["astro-ph.SR","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2010-04-20T20:59:24Z","title":"Quasiblack holes with pressure: relativistic charged spheres as the frozen stars"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1004.3574","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":"sha256:5f559f04e5bd75d7ca9126e0b7a529c21c8edca3252b260ad3d0b858aef4e88f","target":"record","created_at":"2026-05-18T02:24:16Z","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":"b55e7d3ec01b5c1c759ba6c5583aecf6e6234f25ef2ca2929245ca4a7f0a4455","cross_cats_sorted":["astro-ph.SR","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2010-04-20T20:59:24Z","title_canon_sha256":"ffbe2332ad8e8a22df2e3b28f41101b3081c2636a25ee7b4e50db918c42d5a6a"},"schema_version":"1.0","source":{"id":"1004.3574","kind":"arxiv","version":2}},"canonical_sha256":"a8f51073cb3737eca38f791b463d3e1a41a67e6f31c2d8bfb827ffb9e98c61ce","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a8f51073cb3737eca38f791b463d3e1a41a67e6f31c2d8bfb827ffb9e98c61ce","first_computed_at":"2026-05-18T02:24:16.382124Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:24:16.382124Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4qaKhZdfdANDeMH+8reP5q1/IfMTB/VoALx6GpPGLtrDePs/c8qjyi4g8yjTwE8EC7kITt9JMk+yy0Mcd19pAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:24:16.382874Z","signed_message":"canonical_sha256_bytes"},"source_id":"1004.3574","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5f559f04e5bd75d7ca9126e0b7a529c21c8edca3252b260ad3d0b858aef4e88f","sha256:23c3e57289e640b5c08061db8aed8ec50ed47b79356d262a82c545e00a942016"],"state_sha256":"a7fffb878ce9de760f891c0516246be1ef0b2b70e8451493cd037e00b44e3cd5"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FGhf06MAChEj06ml/369+UREX4EKMugFQn1E/Q9MWTF3vQvaba6GbVFwf7YGb3oeOnz37efJKa2gnjAUhFkzDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T20:23:22.106226Z","bundle_sha256":"c03193e42a8a21fa3d28bb0f8afb9736deb775120914aed8e9004fce1d5ddfe7"}}