{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:3OB7AIFFU6QZ4SEJ6VKVY6JRLO","short_pith_number":"pith:3OB7AIFF","canonical_record":{"source":{"id":"1512.03330","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.HE","submitted_at":"2015-12-10T17:22:55Z","cross_cats_sorted":["gr-qc","hep-th"],"title_canon_sha256":"725bc8a4ece6ce8d16b48140e13e5e152c7711a9667b1b9bb9b358441495dbc6","abstract_canon_sha256":"1535a19e5a290de8e33aaf6befa12b4c6dde4c02bb020b3ea21b862d47794f73"},"schema_version":"1.0"},"canonical_sha256":"db83f020a5a7a19e4889f5555c79315b943349428a9e71ddb812c94213a707ac","source":{"kind":"arxiv","id":"1512.03330","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1512.03330","created_at":"2026-05-18T01:17:30Z"},{"alias_kind":"arxiv_version","alias_value":"1512.03330v1","created_at":"2026-05-18T01:17:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.03330","created_at":"2026-05-18T01:17:30Z"},{"alias_kind":"pith_short_12","alias_value":"3OB7AIFFU6QZ","created_at":"2026-05-18T12:29:02Z"},{"alias_kind":"pith_short_16","alias_value":"3OB7AIFFU6QZ4SEJ","created_at":"2026-05-18T12:29:02Z"},{"alias_kind":"pith_short_8","alias_value":"3OB7AIFF","created_at":"2026-05-18T12:29:02Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:3OB7AIFFU6QZ4SEJ6VKVY6JRLO","target":"record","payload":{"canonical_record":{"source":{"id":"1512.03330","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.HE","submitted_at":"2015-12-10T17:22:55Z","cross_cats_sorted":["gr-qc","hep-th"],"title_canon_sha256":"725bc8a4ece6ce8d16b48140e13e5e152c7711a9667b1b9bb9b358441495dbc6","abstract_canon_sha256":"1535a19e5a290de8e33aaf6befa12b4c6dde4c02bb020b3ea21b862d47794f73"},"schema_version":"1.0"},"canonical_sha256":"db83f020a5a7a19e4889f5555c79315b943349428a9e71ddb812c94213a707ac","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:17:30.356411Z","signature_b64":"uS8Zz/LCYLo49nmXU3fdUN6UFuNp1XcldfD9qu6emJJAbFD0wk2BNiqLP6gHdZCR2c0UYvxGY3Myn9jLy148Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"db83f020a5a7a19e4889f5555c79315b943349428a9e71ddb812c94213a707ac","last_reissued_at":"2026-05-18T01:17:30.355507Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:17:30.355507Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1512.03330","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:17:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MS3qsVfozP0iybR7ABzKA36lO1VjdBOAqRF+GLdA0f5Ry+b3lcNBp2kU3xSy6qBBs6691huPEwB9RvuEvndCAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-12T10:18:41.876088Z"},"content_sha256":"6e56dcc8bc717534d8138ae22a730b38edb3219e53105780433029dfd80a09b3","schema_version":"1.0","event_id":"sha256:6e56dcc8bc717534d8138ae22a730b38edb3219e53105780433029dfd80a09b3"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:3OB7AIFFU6QZ4SEJ6VKVY6JRLO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Relativistic rotating Boltzmann gas using the tetrad formalism","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-th"],"primary_cat":"astro-ph.HE","authors_text":"Robert Blaga, Victor E. Ambrus","submitted_at":"2015-12-10T17:22:55Z","abstract_excerpt":"We consider an application of the tetrad formalism introduced by Cardall et al. [Phys. Rev. D 88 (2013) 023011] to the problem of a rigidly rotating relativistic gas in thermal equilibrium and discuss the possible applications of this formalism to relativistic lattice Boltzmann simulations. We present in detail the transformation to the comoving frame, the choice of tetrad, as well as the explicit calculation and analysis of the components of the equilibrium particle flow four-vector and of the equilibrium stress-energy tensor."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.03330","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:17:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hwbNbctWVTEaYdxWuJkcGtwnAS5W8vz/JhGVObKy4SY7xCDpvl0ZUSwRKwOF9puOo+1LTeGf/mxDqcLrLRI5DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-12T10:18:41.876451Z"},"content_sha256":"674e6570be56a040bb768d54f22d0b47c8c5789969fbcd32b967f76e822ed20c","schema_version":"1.0","event_id":"sha256:674e6570be56a040bb768d54f22d0b47c8c5789969fbcd32b967f76e822ed20c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3OB7AIFFU6QZ4SEJ6VKVY6JRLO/bundle.json","state_url":"https://pith.science/pith/3OB7AIFFU6QZ4SEJ6VKVY6JRLO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3OB7AIFFU6QZ4SEJ6VKVY6JRLO/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":"2026-06-12T10:18:41Z","links":{"resolver":"https://pith.science/pith/3OB7AIFFU6QZ4SEJ6VKVY6JRLO","bundle":"https://pith.science/pith/3OB7AIFFU6QZ4SEJ6VKVY6JRLO/bundle.json","state":"https://pith.science/pith/3OB7AIFFU6QZ4SEJ6VKVY6JRLO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3OB7AIFFU6QZ4SEJ6VKVY6JRLO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:3OB7AIFFU6QZ4SEJ6VKVY6JRLO","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":"1535a19e5a290de8e33aaf6befa12b4c6dde4c02bb020b3ea21b862d47794f73","cross_cats_sorted":["gr-qc","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.HE","submitted_at":"2015-12-10T17:22:55Z","title_canon_sha256":"725bc8a4ece6ce8d16b48140e13e5e152c7711a9667b1b9bb9b358441495dbc6"},"schema_version":"1.0","source":{"id":"1512.03330","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1512.03330","created_at":"2026-05-18T01:17:30Z"},{"alias_kind":"arxiv_version","alias_value":"1512.03330v1","created_at":"2026-05-18T01:17:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.03330","created_at":"2026-05-18T01:17:30Z"},{"alias_kind":"pith_short_12","alias_value":"3OB7AIFFU6QZ","created_at":"2026-05-18T12:29:02Z"},{"alias_kind":"pith_short_16","alias_value":"3OB7AIFFU6QZ4SEJ","created_at":"2026-05-18T12:29:02Z"},{"alias_kind":"pith_short_8","alias_value":"3OB7AIFF","created_at":"2026-05-18T12:29:02Z"}],"graph_snapshots":[{"event_id":"sha256:674e6570be56a040bb768d54f22d0b47c8c5789969fbcd32b967f76e822ed20c","target":"graph","created_at":"2026-05-18T01:17:30Z","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 consider an application of the tetrad formalism introduced by Cardall et al. [Phys. Rev. D 88 (2013) 023011] to the problem of a rigidly rotating relativistic gas in thermal equilibrium and discuss the possible applications of this formalism to relativistic lattice Boltzmann simulations. We present in detail the transformation to the comoving frame, the choice of tetrad, as well as the explicit calculation and analysis of the components of the equilibrium particle flow four-vector and of the equilibrium stress-energy tensor.","authors_text":"Robert Blaga, Victor E. Ambrus","cross_cats":["gr-qc","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.HE","submitted_at":"2015-12-10T17:22:55Z","title":"Relativistic rotating Boltzmann gas using the tetrad formalism"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.03330","kind":"arxiv","version":1},"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":"sha256:6e56dcc8bc717534d8138ae22a730b38edb3219e53105780433029dfd80a09b3","target":"record","created_at":"2026-05-18T01:17:30Z","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":"1535a19e5a290de8e33aaf6befa12b4c6dde4c02bb020b3ea21b862d47794f73","cross_cats_sorted":["gr-qc","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.HE","submitted_at":"2015-12-10T17:22:55Z","title_canon_sha256":"725bc8a4ece6ce8d16b48140e13e5e152c7711a9667b1b9bb9b358441495dbc6"},"schema_version":"1.0","source":{"id":"1512.03330","kind":"arxiv","version":1}},"canonical_sha256":"db83f020a5a7a19e4889f5555c79315b943349428a9e71ddb812c94213a707ac","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"db83f020a5a7a19e4889f5555c79315b943349428a9e71ddb812c94213a707ac","first_computed_at":"2026-05-18T01:17:30.355507Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:17:30.355507Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"uS8Zz/LCYLo49nmXU3fdUN6UFuNp1XcldfD9qu6emJJAbFD0wk2BNiqLP6gHdZCR2c0UYvxGY3Myn9jLy148Cw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:17:30.356411Z","signed_message":"canonical_sha256_bytes"},"source_id":"1512.03330","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6e56dcc8bc717534d8138ae22a730b38edb3219e53105780433029dfd80a09b3","sha256:674e6570be56a040bb768d54f22d0b47c8c5789969fbcd32b967f76e822ed20c"],"state_sha256":"8083722cd5ed7302afcf1b6b3293f480ccc192860e66436a4879dd97396e8d61"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rQQa5NYBSpXODwtvTv5TKvlAnAGX9s8TMibyNx/UzXFPWVPiZXr0+7Qb5yU7dSWTL7GG02QZHRPySrB3IlGHCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-12T10:18:41.878471Z","bundle_sha256":"66c969357828140a9e9834572e5755c550ec0de8f6f8bf362b5d05bd845bcc0f"}}