{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:65TBPERX6VMU3PJZUHFZHCFXJ6","short_pith_number":"pith:65TBPERX","canonical_record":{"source":{"id":"1803.08421","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-03-22T15:55:24Z","cross_cats_sorted":[],"title_canon_sha256":"f5c02d4c9cb1eb8e7b1c32e62f4170571555787043e042e52861a518db46f1e2","abstract_canon_sha256":"6da976f6d3e8c5ad0f66f33b8c114e50029e68a0d2530ff9b128604d7b047784"},"schema_version":"1.0"},"canonical_sha256":"f766179237f5594dbd39a1cb9388b74fa4c6e8e66dcd42b251693df4a5150ae3","source":{"kind":"arxiv","id":"1803.08421","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1803.08421","created_at":"2026-05-18T00:14:21Z"},{"alias_kind":"arxiv_version","alias_value":"1803.08421v2","created_at":"2026-05-18T00:14:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.08421","created_at":"2026-05-18T00:14:21Z"},{"alias_kind":"pith_short_12","alias_value":"65TBPERX6VMU","created_at":"2026-05-18T12:32:08Z"},{"alias_kind":"pith_short_16","alias_value":"65TBPERX6VMU3PJZ","created_at":"2026-05-18T12:32:08Z"},{"alias_kind":"pith_short_8","alias_value":"65TBPERX","created_at":"2026-05-18T12:32:08Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:65TBPERX6VMU3PJZUHFZHCFXJ6","target":"record","payload":{"canonical_record":{"source":{"id":"1803.08421","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-03-22T15:55:24Z","cross_cats_sorted":[],"title_canon_sha256":"f5c02d4c9cb1eb8e7b1c32e62f4170571555787043e042e52861a518db46f1e2","abstract_canon_sha256":"6da976f6d3e8c5ad0f66f33b8c114e50029e68a0d2530ff9b128604d7b047784"},"schema_version":"1.0"},"canonical_sha256":"f766179237f5594dbd39a1cb9388b74fa4c6e8e66dcd42b251693df4a5150ae3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:14:21.557375Z","signature_b64":"vbAjkfsEzWd0IAet6xeR64nxh8TD6KoSnnE4Ul1YbxSdjeyRgE5qdCq2ThQ38Ha7CzhORC+T4DwgnnDyK/QgCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f766179237f5594dbd39a1cb9388b74fa4c6e8e66dcd42b251693df4a5150ae3","last_reissued_at":"2026-05-18T00:14:21.556766Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:14:21.556766Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1803.08421","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":"2026-05-18T00:14:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"r3yS5FsFmpEP2Avb9E3RDe8TlCye7cEAG2BUr2PBq1HKY2uaZlA9UPJbBR21bNlkmThFCz/L9xSmN4duj3VKBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T01:13:30.873479Z"},"content_sha256":"2159fe2c5fb3dc885ea275b0308eeb1c26b010ff9952e029951371e75fe37ccf","schema_version":"1.0","event_id":"sha256:2159fe2c5fb3dc885ea275b0308eeb1c26b010ff9952e029951371e75fe37ccf"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:65TBPERX6VMU3PJZUHFZHCFXJ6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"BRST-BV approach to continuous-spin field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"R.R. Metsaev","submitted_at":"2018-03-22T15:55:24Z","abstract_excerpt":"Using BRST-BV approach, massless and massive continuous-spin fields propagating in the flat space are studied. For such fields, BRST-BV gauge invariant Lagrangian is obtained. The Lagrangian and gauge transformations are constructed out of traceless gauge fields and traceless gauge transformation parameters. Interrelation between the BRST-BV Lagrangian and the Lagrangian for the continuous-spin fields in metric-like approach is demonstrated. Considering the BRST-BV Lagrangian in the Siegel gauge, we get gauge-fixed Lagrangian which is invariant under global BRST and antiBRST transformations."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.08421","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":"2026-05-18T00:14:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YqsZrQA7TviK2iTz5ae3M87GdvP8r/cZ8CjY9beJDwXSl+Ba/0GvpaBmWAvVzuJHNuxnk1F7ClbaUslq5QWnCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T01:13:30.874094Z"},"content_sha256":"c8655b5783ef27d9e3950cbef86584b45d5dd310ddb475686bf6cf0f75c1613e","schema_version":"1.0","event_id":"sha256:c8655b5783ef27d9e3950cbef86584b45d5dd310ddb475686bf6cf0f75c1613e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/65TBPERX6VMU3PJZUHFZHCFXJ6/bundle.json","state_url":"https://pith.science/pith/65TBPERX6VMU3PJZUHFZHCFXJ6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/65TBPERX6VMU3PJZUHFZHCFXJ6/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":"2026-06-09T01:13:30Z","links":{"resolver":"https://pith.science/pith/65TBPERX6VMU3PJZUHFZHCFXJ6","bundle":"https://pith.science/pith/65TBPERX6VMU3PJZUHFZHCFXJ6/bundle.json","state":"https://pith.science/pith/65TBPERX6VMU3PJZUHFZHCFXJ6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/65TBPERX6VMU3PJZUHFZHCFXJ6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:65TBPERX6VMU3PJZUHFZHCFXJ6","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":"6da976f6d3e8c5ad0f66f33b8c114e50029e68a0d2530ff9b128604d7b047784","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-03-22T15:55:24Z","title_canon_sha256":"f5c02d4c9cb1eb8e7b1c32e62f4170571555787043e042e52861a518db46f1e2"},"schema_version":"1.0","source":{"id":"1803.08421","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1803.08421","created_at":"2026-05-18T00:14:21Z"},{"alias_kind":"arxiv_version","alias_value":"1803.08421v2","created_at":"2026-05-18T00:14:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.08421","created_at":"2026-05-18T00:14:21Z"},{"alias_kind":"pith_short_12","alias_value":"65TBPERX6VMU","created_at":"2026-05-18T12:32:08Z"},{"alias_kind":"pith_short_16","alias_value":"65TBPERX6VMU3PJZ","created_at":"2026-05-18T12:32:08Z"},{"alias_kind":"pith_short_8","alias_value":"65TBPERX","created_at":"2026-05-18T12:32:08Z"}],"graph_snapshots":[{"event_id":"sha256:c8655b5783ef27d9e3950cbef86584b45d5dd310ddb475686bf6cf0f75c1613e","target":"graph","created_at":"2026-05-18T00:14:21Z","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":"Using BRST-BV approach, massless and massive continuous-spin fields propagating in the flat space are studied. For such fields, BRST-BV gauge invariant Lagrangian is obtained. The Lagrangian and gauge transformations are constructed out of traceless gauge fields and traceless gauge transformation parameters. Interrelation between the BRST-BV Lagrangian and the Lagrangian for the continuous-spin fields in metric-like approach is demonstrated. Considering the BRST-BV Lagrangian in the Siegel gauge, we get gauge-fixed Lagrangian which is invariant under global BRST and antiBRST transformations.","authors_text":"R.R. Metsaev","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-03-22T15:55:24Z","title":"BRST-BV approach to continuous-spin field"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.08421","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":"sha256:2159fe2c5fb3dc885ea275b0308eeb1c26b010ff9952e029951371e75fe37ccf","target":"record","created_at":"2026-05-18T00:14:21Z","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":"6da976f6d3e8c5ad0f66f33b8c114e50029e68a0d2530ff9b128604d7b047784","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-03-22T15:55:24Z","title_canon_sha256":"f5c02d4c9cb1eb8e7b1c32e62f4170571555787043e042e52861a518db46f1e2"},"schema_version":"1.0","source":{"id":"1803.08421","kind":"arxiv","version":2}},"canonical_sha256":"f766179237f5594dbd39a1cb9388b74fa4c6e8e66dcd42b251693df4a5150ae3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f766179237f5594dbd39a1cb9388b74fa4c6e8e66dcd42b251693df4a5150ae3","first_computed_at":"2026-05-18T00:14:21.556766Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:14:21.556766Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vbAjkfsEzWd0IAet6xeR64nxh8TD6KoSnnE4Ul1YbxSdjeyRgE5qdCq2ThQ38Ha7CzhORC+T4DwgnnDyK/QgCg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:14:21.557375Z","signed_message":"canonical_sha256_bytes"},"source_id":"1803.08421","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2159fe2c5fb3dc885ea275b0308eeb1c26b010ff9952e029951371e75fe37ccf","sha256:c8655b5783ef27d9e3950cbef86584b45d5dd310ddb475686bf6cf0f75c1613e"],"state_sha256":"6773ffff08a8e06f44164a485339281bf40dae2f4cf0585a0bb3541439712646"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QPzKtm/s6W6lXN5ZKmMFv2GAD8YIUVarQAkEGoFKQOd9TB/hyX13PcsiQ5oUTdyVZiaoGg/8+epYOvqLzP7uCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T01:13:30.877220Z","bundle_sha256":"f7f588a33483846a1e28f7ec61398b998389e0dc088898faa083ca193faef753"}}