{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:R6D5ELWMOWDUSW6H2QHW23T5O4","short_pith_number":"pith:R6D5ELWM","canonical_record":{"source":{"id":"1111.0961","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2011-11-03T19:53:13Z","cross_cats_sorted":[],"title_canon_sha256":"2e8d6bf97680ca1a20d5f03d538de570fc4d46afcb7c582106e906048c142eab","abstract_canon_sha256":"0f8a1ce9276f19349cebe5165cbac94ed7b7d4bda66d30a212bf1b669e38eada"},"schema_version":"1.0"},"canonical_sha256":"8f87d22ecc7587495bc7d40f6d6e7d7736f51826d36bce14ff16a280b90b021e","source":{"kind":"arxiv","id":"1111.0961","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1111.0961","created_at":"2026-05-18T01:59:45Z"},{"alias_kind":"arxiv_version","alias_value":"1111.0961v2","created_at":"2026-05-18T01:59:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1111.0961","created_at":"2026-05-18T01:59:45Z"},{"alias_kind":"pith_short_12","alias_value":"R6D5ELWMOWDU","created_at":"2026-05-18T12:26:41Z"},{"alias_kind":"pith_short_16","alias_value":"R6D5ELWMOWDUSW6H","created_at":"2026-05-18T12:26:41Z"},{"alias_kind":"pith_short_8","alias_value":"R6D5ELWM","created_at":"2026-05-18T12:26:41Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:R6D5ELWMOWDUSW6H2QHW23T5O4","target":"record","payload":{"canonical_record":{"source":{"id":"1111.0961","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2011-11-03T19:53:13Z","cross_cats_sorted":[],"title_canon_sha256":"2e8d6bf97680ca1a20d5f03d538de570fc4d46afcb7c582106e906048c142eab","abstract_canon_sha256":"0f8a1ce9276f19349cebe5165cbac94ed7b7d4bda66d30a212bf1b669e38eada"},"schema_version":"1.0"},"canonical_sha256":"8f87d22ecc7587495bc7d40f6d6e7d7736f51826d36bce14ff16a280b90b021e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:59:45.828025Z","signature_b64":"u+W2ym0BCEJGV8LkTmdIrSxNt1UP/0BqtWBQZTuaIf0Fq6wk9oXHzr5Acz/TiJJ2Q5TrFAPRgVO2PcLiH7asDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8f87d22ecc7587495bc7d40f6d6e7d7736f51826d36bce14ff16a280b90b021e","last_reissued_at":"2026-05-18T01:59:45.827280Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:59:45.827280Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1111.0961","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":"2026-05-18T01:59:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"olaHSRmJAH5q6/3oHE8NpwBzCwz5y/+k1jjTAivaM0SiHVgf7qZ+mwoTwv69EWOJsi4p8xDzXVAkvFAvUMtmDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T19:19:50.211764Z"},"content_sha256":"ef04eef1c76229ef18d0d833c8b5b629c7bac15ef888b014a17f69e75598b03b","schema_version":"1.0","event_id":"sha256:ef04eef1c76229ef18d0d833c8b5b629c7bac15ef888b014a17f69e75598b03b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:R6D5ELWMOWDUSW6H2QHW23T5O4","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Immirzi parameter and Noether charges in first order gravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"R. Durka","submitted_at":"2011-11-03T19:53:13Z","abstract_excerpt":"The framework of SO(3,2) constrained BF theory applied to gravity makes it possible to generalize formulas for gravitational diffeomorphic Noether charges (mass, angular momentum, and entropy). It extends Wald's approach to the case of first order gravity with a negative cosmological constant, the Holst modification and the topological terms (Nieh-Yan, Euler, and Pontryagin). Topological invariants play essential role contributing to the boundary terms in the regularization scheme for the asymptotically AdS spacetimes, so that the differentiability of the action is automatically secured. Intri"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1111.0961","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":"2026-05-18T01:59:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JqjMvGysdh/OptWnvLly4q1uz5eHVx8izH1Uvt1P9FGnhh6XdEt4+LIv9AuRFlu5kqWrDNyCnEPiieGpNxbeBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T19:19:50.212165Z"},"content_sha256":"6c122218f7fc68c5f285d3dc34c8769ba84c7469e96e58d40a42935f49e5c7db","schema_version":"1.0","event_id":"sha256:6c122218f7fc68c5f285d3dc34c8769ba84c7469e96e58d40a42935f49e5c7db"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/R6D5ELWMOWDUSW6H2QHW23T5O4/bundle.json","state_url":"https://pith.science/pith/R6D5ELWMOWDUSW6H2QHW23T5O4/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/R6D5ELWMOWDUSW6H2QHW23T5O4/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":"2026-06-06T19:19:50Z","links":{"resolver":"https://pith.science/pith/R6D5ELWMOWDUSW6H2QHW23T5O4","bundle":"https://pith.science/pith/R6D5ELWMOWDUSW6H2QHW23T5O4/bundle.json","state":"https://pith.science/pith/R6D5ELWMOWDUSW6H2QHW23T5O4/state.json","well_known_bundle":"https://pith.science/.well-known/pith/R6D5ELWMOWDUSW6H2QHW23T5O4/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:R6D5ELWMOWDUSW6H2QHW23T5O4","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":"0f8a1ce9276f19349cebe5165cbac94ed7b7d4bda66d30a212bf1b669e38eada","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2011-11-03T19:53:13Z","title_canon_sha256":"2e8d6bf97680ca1a20d5f03d538de570fc4d46afcb7c582106e906048c142eab"},"schema_version":"1.0","source":{"id":"1111.0961","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1111.0961","created_at":"2026-05-18T01:59:45Z"},{"alias_kind":"arxiv_version","alias_value":"1111.0961v2","created_at":"2026-05-18T01:59:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1111.0961","created_at":"2026-05-18T01:59:45Z"},{"alias_kind":"pith_short_12","alias_value":"R6D5ELWMOWDU","created_at":"2026-05-18T12:26:41Z"},{"alias_kind":"pith_short_16","alias_value":"R6D5ELWMOWDUSW6H","created_at":"2026-05-18T12:26:41Z"},{"alias_kind":"pith_short_8","alias_value":"R6D5ELWM","created_at":"2026-05-18T12:26:41Z"}],"graph_snapshots":[{"event_id":"sha256:6c122218f7fc68c5f285d3dc34c8769ba84c7469e96e58d40a42935f49e5c7db","target":"graph","created_at":"2026-05-18T01:59:45Z","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 framework of SO(3,2) constrained BF theory applied to gravity makes it possible to generalize formulas for gravitational diffeomorphic Noether charges (mass, angular momentum, and entropy). It extends Wald's approach to the case of first order gravity with a negative cosmological constant, the Holst modification and the topological terms (Nieh-Yan, Euler, and Pontryagin). Topological invariants play essential role contributing to the boundary terms in the regularization scheme for the asymptotically AdS spacetimes, so that the differentiability of the action is automatically secured. Intri","authors_text":"R. Durka","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2011-11-03T19:53:13Z","title":"Immirzi parameter and Noether charges in first order gravity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1111.0961","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:ef04eef1c76229ef18d0d833c8b5b629c7bac15ef888b014a17f69e75598b03b","target":"record","created_at":"2026-05-18T01:59:45Z","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":"0f8a1ce9276f19349cebe5165cbac94ed7b7d4bda66d30a212bf1b669e38eada","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2011-11-03T19:53:13Z","title_canon_sha256":"2e8d6bf97680ca1a20d5f03d538de570fc4d46afcb7c582106e906048c142eab"},"schema_version":"1.0","source":{"id":"1111.0961","kind":"arxiv","version":2}},"canonical_sha256":"8f87d22ecc7587495bc7d40f6d6e7d7736f51826d36bce14ff16a280b90b021e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8f87d22ecc7587495bc7d40f6d6e7d7736f51826d36bce14ff16a280b90b021e","first_computed_at":"2026-05-18T01:59:45.827280Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:59:45.827280Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"u+W2ym0BCEJGV8LkTmdIrSxNt1UP/0BqtWBQZTuaIf0Fq6wk9oXHzr5Acz/TiJJ2Q5TrFAPRgVO2PcLiH7asDg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:59:45.828025Z","signed_message":"canonical_sha256_bytes"},"source_id":"1111.0961","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ef04eef1c76229ef18d0d833c8b5b629c7bac15ef888b014a17f69e75598b03b","sha256:6c122218f7fc68c5f285d3dc34c8769ba84c7469e96e58d40a42935f49e5c7db"],"state_sha256":"d75f794b2b0b59033d51c738ac0dc0e876b0fad00827f18dff1523c6d63f3aed"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zC7hO9/ugWoQ0mGc+w/myFRNZVxJ+kSkRCvRJR/04Iou60RYQ9GLd18EB7MQ7imfyfDFKKcEjSNHJizW3orWAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-06T19:19:50.214875Z","bundle_sha256":"c8473225df07ae9b4ed6a866ca807dae1ff04d079b51ba1737c6c91e041660e7"}}