{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:VO4O7W234SVOANEX4DPLC3XOER","short_pith_number":"pith:VO4O7W23","canonical_record":{"source":{"id":"2506.10437","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2025-06-12T07:39:41Z","cross_cats_sorted":[],"title_canon_sha256":"faa72ba0e92e9a2315da390fac3abbf1b1ffacac0cd32a34a14ab0a7b0b3ec5d","abstract_canon_sha256":"e55dc89399183645dfa2ce126b9b39700a8c56939c39e8c8b34fbf14156d9caf"},"schema_version":"1.0"},"canonical_sha256":"abb8efdb5be4aae03497e0deb16eee2456b09cb669f571b149836beb49e14e4b","source":{"kind":"arxiv","id":"2506.10437","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2506.10437","created_at":"2026-07-05T11:20:23Z"},{"alias_kind":"arxiv_version","alias_value":"2506.10437v1","created_at":"2026-07-05T11:20:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.10437","created_at":"2026-07-05T11:20:23Z"},{"alias_kind":"pith_short_12","alias_value":"VO4O7W234SVO","created_at":"2026-07-05T11:20:23Z"},{"alias_kind":"pith_short_16","alias_value":"VO4O7W234SVOANEX","created_at":"2026-07-05T11:20:23Z"},{"alias_kind":"pith_short_8","alias_value":"VO4O7W23","created_at":"2026-07-05T11:20:23Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:VO4O7W234SVOANEX4DPLC3XOER","target":"record","payload":{"canonical_record":{"source":{"id":"2506.10437","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2025-06-12T07:39:41Z","cross_cats_sorted":[],"title_canon_sha256":"faa72ba0e92e9a2315da390fac3abbf1b1ffacac0cd32a34a14ab0a7b0b3ec5d","abstract_canon_sha256":"e55dc89399183645dfa2ce126b9b39700a8c56939c39e8c8b34fbf14156d9caf"},"schema_version":"1.0"},"canonical_sha256":"abb8efdb5be4aae03497e0deb16eee2456b09cb669f571b149836beb49e14e4b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:20:23.659514Z","signature_b64":"PP1o6eIeX6sf5CByUm8Fs7TNFrH4SAvuhWYTCDvr+/l9Czk6FXc8pfHa71uXryFpO0r9/wzA22zPhRjo9jldBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"abb8efdb5be4aae03497e0deb16eee2456b09cb669f571b149836beb49e14e4b","last_reissued_at":"2026-07-05T11:20:23.658998Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:20:23.658998Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2506.10437","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":"2026-07-05T11:20:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6CHjJM84cFB+z9/62tqO8wKgZohOAkfYr0JDepPVvUhmcC4HBWvwwKLT18ZTy4QgJzzfwvHGSHxNn/71rke4BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-07T16:02:05.052670Z"},"content_sha256":"41ffd78023e775440b79e7c19553abee633bcc11f3ff9927135771a850d21789","schema_version":"1.0","event_id":"sha256:41ffd78023e775440b79e7c19553abee633bcc11f3ff9927135771a850d21789"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:VO4O7W234SVOANEX4DPLC3XOER","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Constraining quadrupole deformations with relativistic effects","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Ainur Urazalina, Anuar Idrissov, Daniya Utepova, Gulzada Baimbetova, Hernando Quevedo, Kuantay Boshkayev, Serzhan Momynov","submitted_at":"2025-06-12T07:39:41Z","abstract_excerpt":"We investigate two general relativistic effects - namely, the Shirokov and Shapiro effects - within the framework of the Zipoy-Voorhees spacetime ($q$-metric), which generalizes the Schwarzschild solution by incorporating a quadrupole moment. By analyzing the geodesic deviation equations, we explore the oscillatory motion of test particles and demonstrate how the source's quadrupole parameter influences the Shirokov effect. Furthermore, we derive an expression for the Shapiro time delay in this deformed spacetime and examine the quadrupole moment's impact on the gravitational time delay experi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.10437","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2506.10437/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T11:20:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9/oeQtlvc0mq20KBim3IRavr3gJigkR8iFoXkiac6QOX45ribQ9ykYR6/ISQi3lqnl8pq7SRhkd5JiDn7lsYCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-07T16:02:05.053319Z"},"content_sha256":"31e457e3f9acea8a08b7002f91e03879d0d5353483e127e5e85a2058dd30eab6","schema_version":"1.0","event_id":"sha256:31e457e3f9acea8a08b7002f91e03879d0d5353483e127e5e85a2058dd30eab6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VO4O7W234SVOANEX4DPLC3XOER/bundle.json","state_url":"https://pith.science/pith/VO4O7W234SVOANEX4DPLC3XOER/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VO4O7W234SVOANEX4DPLC3XOER/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":"2026-08-07T16:02:05Z","links":{"resolver":"https://pith.science/pith/VO4O7W234SVOANEX4DPLC3XOER","bundle":"https://pith.science/pith/VO4O7W234SVOANEX4DPLC3XOER/bundle.json","state":"https://pith.science/pith/VO4O7W234SVOANEX4DPLC3XOER/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VO4O7W234SVOANEX4DPLC3XOER/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:VO4O7W234SVOANEX4DPLC3XOER","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":"e55dc89399183645dfa2ce126b9b39700a8c56939c39e8c8b34fbf14156d9caf","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2025-06-12T07:39:41Z","title_canon_sha256":"faa72ba0e92e9a2315da390fac3abbf1b1ffacac0cd32a34a14ab0a7b0b3ec5d"},"schema_version":"1.0","source":{"id":"2506.10437","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2506.10437","created_at":"2026-07-05T11:20:23Z"},{"alias_kind":"arxiv_version","alias_value":"2506.10437v1","created_at":"2026-07-05T11:20:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.10437","created_at":"2026-07-05T11:20:23Z"},{"alias_kind":"pith_short_12","alias_value":"VO4O7W234SVO","created_at":"2026-07-05T11:20:23Z"},{"alias_kind":"pith_short_16","alias_value":"VO4O7W234SVOANEX","created_at":"2026-07-05T11:20:23Z"},{"alias_kind":"pith_short_8","alias_value":"VO4O7W23","created_at":"2026-07-05T11:20:23Z"}],"graph_snapshots":[{"event_id":"sha256:31e457e3f9acea8a08b7002f91e03879d0d5353483e127e5e85a2058dd30eab6","target":"graph","created_at":"2026-07-05T11:20:23Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2506.10437/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We investigate two general relativistic effects - namely, the Shirokov and Shapiro effects - within the framework of the Zipoy-Voorhees spacetime ($q$-metric), which generalizes the Schwarzschild solution by incorporating a quadrupole moment. By analyzing the geodesic deviation equations, we explore the oscillatory motion of test particles and demonstrate how the source's quadrupole parameter influences the Shirokov effect. Furthermore, we derive an expression for the Shapiro time delay in this deformed spacetime and examine the quadrupole moment's impact on the gravitational time delay experi","authors_text":"Ainur Urazalina, Anuar Idrissov, Daniya Utepova, Gulzada Baimbetova, Hernando Quevedo, Kuantay Boshkayev, Serzhan Momynov","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2025-06-12T07:39:41Z","title":"Constraining quadrupole deformations with relativistic effects"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.10437","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":"sha256:41ffd78023e775440b79e7c19553abee633bcc11f3ff9927135771a850d21789","target":"record","created_at":"2026-07-05T11:20:23Z","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":"e55dc89399183645dfa2ce126b9b39700a8c56939c39e8c8b34fbf14156d9caf","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2025-06-12T07:39:41Z","title_canon_sha256":"faa72ba0e92e9a2315da390fac3abbf1b1ffacac0cd32a34a14ab0a7b0b3ec5d"},"schema_version":"1.0","source":{"id":"2506.10437","kind":"arxiv","version":1}},"canonical_sha256":"abb8efdb5be4aae03497e0deb16eee2456b09cb669f571b149836beb49e14e4b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"abb8efdb5be4aae03497e0deb16eee2456b09cb669f571b149836beb49e14e4b","first_computed_at":"2026-07-05T11:20:23.658998Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:20:23.658998Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"PP1o6eIeX6sf5CByUm8Fs7TNFrH4SAvuhWYTCDvr+/l9Czk6FXc8pfHa71uXryFpO0r9/wzA22zPhRjo9jldBw==","signature_status":"signed_v1","signed_at":"2026-07-05T11:20:23.659514Z","signed_message":"canonical_sha256_bytes"},"source_id":"2506.10437","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:41ffd78023e775440b79e7c19553abee633bcc11f3ff9927135771a850d21789","sha256:31e457e3f9acea8a08b7002f91e03879d0d5353483e127e5e85a2058dd30eab6"],"state_sha256":"2225a0f5c249d2de73891614f34f30147a10d23bb42c61a0f6c19a1539828308"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5GaOl89f0D1vzE1Z2s1VrLioWbk38hbjQghYzAktYNNAi2VHOCZZ9XOLqEnUHw/T/0uNi6lDoOTlnIAJJs52Ag==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-07T16:02:05.060221Z","bundle_sha256":"ba6acf5cf28b46bb78ce96fc0792a7e60fd3a10bb25173987fc3a28e432e03d8"}}