{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2020:HX4LVRJYMIMNJUNAVKEPUVME3W","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":"ca343fb434a2c7f1a7fc492867a2554f855391e7ecbcaae4d2e38f49f2e0f8cc","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"astro-ph.HE","submitted_at":"2020-12-14T07:34:27Z","title_canon_sha256":"716f4abab74eb9b5eba0a19c014c27f815c00c587b5579ded9ae6d925a9d493c"},"schema_version":"1.0","source":{"id":"2012.07303","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2012.07303","created_at":"2026-07-05T01:59:19Z"},{"alias_kind":"arxiv_version","alias_value":"2012.07303v1","created_at":"2026-07-05T01:59:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2012.07303","created_at":"2026-07-05T01:59:19Z"},{"alias_kind":"pith_short_12","alias_value":"HX4LVRJYMIMN","created_at":"2026-07-05T01:59:19Z"},{"alias_kind":"pith_short_16","alias_value":"HX4LVRJYMIMNJUNA","created_at":"2026-07-05T01:59:19Z"},{"alias_kind":"pith_short_8","alias_value":"HX4LVRJY","created_at":"2026-07-05T01:59:19Z"}],"graph_snapshots":[{"event_id":"sha256:34a086bce7481be1022f07244de79925e33dafccd485954febffb33c8a4ba955","target":"graph","created_at":"2026-07-05T01:59:19Z","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/2012.07303/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"There are some similarities between bursts of repeating fast radio bursts (FRBs) and giant pulses (GPs) of pulsars. To explore possible relations between them, we study the cumulative energy distributions of these two phenomena using the observations of repeating FRB 121102 and the GPs of Crab pulsar. We find that the power-law slope of GPs (with fluence $\\geq$130 Jy ms) is $2.85\\pm0.10$. The energy distribution of FRB 121102 can be well fitted by a smooth broken power-law function. For the bursts of FRB 121102 above the break energy (1.22 $\\times 10^{37}$ erg), the best-fitting slope is $2.90","authors_text":"Can-Min Deng, Fen Lyu, Jin-Jun Geng, Jun-Jie Wei, Lin Lin, Xue-Feng Wu, Yan-Zhi Meng, Ye Li, Zhen-Fan Tang","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"astro-ph.HE","submitted_at":"2020-12-14T07:34:27Z","title":"A comparison between repeating bursts of FRB 121102 and giant pulses from Crab pulsar and its applications"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2012.07303","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":"sha256:3794c3ef0abf3bea8949254ede08a25664e8681a2c7a09aa28e4aee236c76ad3","target":"record","created_at":"2026-07-05T01:59:19Z","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":"ca343fb434a2c7f1a7fc492867a2554f855391e7ecbcaae4d2e38f49f2e0f8cc","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"astro-ph.HE","submitted_at":"2020-12-14T07:34:27Z","title_canon_sha256":"716f4abab74eb9b5eba0a19c014c27f815c00c587b5579ded9ae6d925a9d493c"},"schema_version":"1.0","source":{"id":"2012.07303","kind":"arxiv","version":1}},"canonical_sha256":"3df8bac5386218d4d1a0aa88fa5584dd83f8c344a0c84bdbdf0068a6287b5af8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3df8bac5386218d4d1a0aa88fa5584dd83f8c344a0c84bdbdf0068a6287b5af8","first_computed_at":"2026-07-05T01:59:19.209822Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T01:59:19.209822Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"mP8Rn63f2hZgQcgsDlmEdfzboihOPcGI7KqlsrodUSm800kXEIqJFp029EWSHscLXK991X9qHyEJYYT3KzTiBQ==","signature_status":"signed_v1","signed_at":"2026-07-05T01:59:19.210159Z","signed_message":"canonical_sha256_bytes"},"source_id":"2012.07303","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3794c3ef0abf3bea8949254ede08a25664e8681a2c7a09aa28e4aee236c76ad3","sha256:34a086bce7481be1022f07244de79925e33dafccd485954febffb33c8a4ba955"],"state_sha256":"88bd397ecc238ebf28b931da1c032893abef612e5bcc6493ad491c9e70e8505d"}