{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2004:3HRFB6C2BYWMOSF4SZSINFRVBU","short_pith_number":"pith:3HRFB6C2","schema_version":"1.0","canonical_sha256":"d9e250f85a0e2cc748bc96648696350d0c95e67d49c15c470f3fd41e8817e52e","source":{"kind":"arxiv","id":"gr-qc/0410089","version":1},"attestation_state":"computed","paper":{"title":"Spinning Up Asymptotically Flat Spacetimes","license":"","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"E.N. Glass, J.P. Krisch","submitted_at":"2004-10-19T03:13:49Z","abstract_excerpt":"We present a method for constructing stationary, asymptotically flat, rotating solutions of Einstein's field equations. One of the spun-up solutions has quasilocal mass but no global mass. It has an ergosphere but no event horizon. The angular momentum is constant everywhere beyond the ergosphere. The energy-momentum content of this solution can be interpreted as a rotating string-fluid."},"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":"gr-qc/0410089","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"gr-qc","submitted_at":"2004-10-19T03:13:49Z","cross_cats_sorted":[],"title_canon_sha256":"12c2f35018f246bb687ec0b402bce3dd0966a29adff2cf45b76ee73b1c92e117","abstract_canon_sha256":"2537fc32e3c2164ac5fede70f68888a16a0aa6926b4c41e9de85a29fc833e8bb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:35:34.573137Z","signature_b64":"A1PPCBKh6AeTbrBzbGmDTLmKaArk05PQugpFGLpdsNKpCZv4VUvaryPyB9EyanM57y5Ehenm0soaOI9Wl2eACg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d9e250f85a0e2cc748bc96648696350d0c95e67d49c15c470f3fd41e8817e52e","last_reissued_at":"2026-05-18T04:35:34.572503Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:35:34.572503Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Spinning Up Asymptotically Flat Spacetimes","license":"","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"E.N. Glass, J.P. Krisch","submitted_at":"2004-10-19T03:13:49Z","abstract_excerpt":"We present a method for constructing stationary, asymptotically flat, rotating solutions of Einstein's field equations. One of the spun-up solutions has quasilocal mass but no global mass. It has an ergosphere but no event horizon. The angular momentum is constant everywhere beyond the ergosphere. The energy-momentum content of this solution can be interpreted as a rotating string-fluid."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"gr-qc/0410089","kind":"arxiv","version":1},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"gr-qc/0410089","created_at":"2026-05-18T04:35:34.572589+00:00"},{"alias_kind":"arxiv_version","alias_value":"gr-qc/0410089v1","created_at":"2026-05-18T04:35:34.572589+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.gr-qc/0410089","created_at":"2026-05-18T04:35:34.572589+00:00"},{"alias_kind":"pith_short_12","alias_value":"3HRFB6C2BYWM","created_at":"2026-05-18T12:25:52.051335+00:00"},{"alias_kind":"pith_short_16","alias_value":"3HRFB6C2BYWMOSF4","created_at":"2026-05-18T12:25:52.051335+00:00"},{"alias_kind":"pith_short_8","alias_value":"3HRFB6C2","created_at":"2026-05-18T12:25:52.051335+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3HRFB6C2BYWMOSF4SZSINFRVBU","json":"https://pith.science/pith/3HRFB6C2BYWMOSF4SZSINFRVBU.json","graph_json":"https://pith.science/api/pith-number/3HRFB6C2BYWMOSF4SZSINFRVBU/graph.json","events_json":"https://pith.science/api/pith-number/3HRFB6C2BYWMOSF4SZSINFRVBU/events.json","paper":"https://pith.science/paper/3HRFB6C2"},"agent_actions":{"view_html":"https://pith.science/pith/3HRFB6C2BYWMOSF4SZSINFRVBU","download_json":"https://pith.science/pith/3HRFB6C2BYWMOSF4SZSINFRVBU.json","view_paper":"https://pith.science/paper/3HRFB6C2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=gr-qc/0410089&json=true","fetch_graph":"https://pith.science/api/pith-number/3HRFB6C2BYWMOSF4SZSINFRVBU/graph.json","fetch_events":"https://pith.science/api/pith-number/3HRFB6C2BYWMOSF4SZSINFRVBU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3HRFB6C2BYWMOSF4SZSINFRVBU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3HRFB6C2BYWMOSF4SZSINFRVBU/action/storage_attestation","attest_author":"https://pith.science/pith/3HRFB6C2BYWMOSF4SZSINFRVBU/action/author_attestation","sign_citation":"https://pith.science/pith/3HRFB6C2BYWMOSF4SZSINFRVBU/action/citation_signature","submit_replication":"https://pith.science/pith/3HRFB6C2BYWMOSF4SZSINFRVBU/action/replication_record"}},"created_at":"2026-05-18T04:35:34.572589+00:00","updated_at":"2026-05-18T04:35:34.572589+00:00"}