{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:2PD75DYZFR6G5CSJMEN4KVPTAD","short_pith_number":"pith:2PD75DYZ","canonical_record":{"source":{"id":"1010.3457","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2010-10-17T22:42:19Z","cross_cats_sorted":[],"title_canon_sha256":"958ef955a0b7ca899d6e7ca208754dc063237104f47f7174f2d4f6a70069c430","abstract_canon_sha256":"beee800d90847028f45688ef567650008fe3ca627be08aa55a2c6e267738449e"},"schema_version":"1.0"},"canonical_sha256":"d3c7fe8f192c7c6e8a49611bc555f300c3944d0dad89518164edc37564fe1f52","source":{"kind":"arxiv","id":"1010.3457","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1010.3457","created_at":"2026-05-18T04:30:13Z"},{"alias_kind":"arxiv_version","alias_value":"1010.3457v2","created_at":"2026-05-18T04:30:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.3457","created_at":"2026-05-18T04:30:13Z"},{"alias_kind":"pith_short_12","alias_value":"2PD75DYZFR6G","created_at":"2026-05-18T12:26:03Z"},{"alias_kind":"pith_short_16","alias_value":"2PD75DYZFR6G5CSJ","created_at":"2026-05-18T12:26:03Z"},{"alias_kind":"pith_short_8","alias_value":"2PD75DYZ","created_at":"2026-05-18T12:26:03Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:2PD75DYZFR6G5CSJMEN4KVPTAD","target":"record","payload":{"canonical_record":{"source":{"id":"1010.3457","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2010-10-17T22:42:19Z","cross_cats_sorted":[],"title_canon_sha256":"958ef955a0b7ca899d6e7ca208754dc063237104f47f7174f2d4f6a70069c430","abstract_canon_sha256":"beee800d90847028f45688ef567650008fe3ca627be08aa55a2c6e267738449e"},"schema_version":"1.0"},"canonical_sha256":"d3c7fe8f192c7c6e8a49611bc555f300c3944d0dad89518164edc37564fe1f52","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:30:13.769073Z","signature_b64":"ezYdlhAcYq3nUipc8/Vo5Ijq/MoYN7b8rpCgFS2ButSF7tjzOy7j4gcV5OlE3VmRSbLUtzlD/5wDbcY5Md1VCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d3c7fe8f192c7c6e8a49611bc555f300c3944d0dad89518164edc37564fe1f52","last_reissued_at":"2026-05-18T04:30:13.768575Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:30:13.768575Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1010.3457","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":"2026-05-18T04:30:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5oAbABAcLjdWTwWmoKFid2blRMWv4zOah9gedFxquzYJ55WjiBYugdhZr9qpMXw80dZRrEUdAiLquB31VvPtCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T02:09:12.952489Z"},"content_sha256":"c447a27c1104b87f73c045a9170569fab91d20248ef9aaa914fbe205ccb80b97","schema_version":"1.0","event_id":"sha256:c447a27c1104b87f73c045a9170569fab91d20248ef9aaa914fbe205ccb80b97"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:2PD75DYZFR6G5CSJMEN4KVPTAD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dynamical Polarizabilities of SU(3) Octet of Baryons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"A. Aleksejevs, S. Barkanova","submitted_at":"2010-10-17T22:42:19Z","abstract_excerpt":"We present calculations and an analysis of the spin-independent dipole electric and magnetic dynamical polarizabilities for the lowest in mass SU(3) octet of baryons. These extensive calculations are made possible by the recent implementation of semi-automatized calculations in Chiral Perturbation Theory which allows evaluating dynamical spin-independent electromagnetic polarizabilities from Compton scattering up to next-to-the-leading order. Our results are in good agreement with calculations performed for nucleons found in the literature. The dependencies for the range of photon energies up "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.3457","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":"2026-05-18T04:30:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kAdBPAwbBc2IJztqAdk8U7AuJSihOL1jGhIOW9X8dnqI/EWNjO+DoLF0SNZRik3Evb3aarGEuJaj/OY//tRKDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T02:09:12.953220Z"},"content_sha256":"2e105b07d72c62988cf6c28bd72b814c65ffa211295c0a340cbfd00e49b9a5d2","schema_version":"1.0","event_id":"sha256:2e105b07d72c62988cf6c28bd72b814c65ffa211295c0a340cbfd00e49b9a5d2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2PD75DYZFR6G5CSJMEN4KVPTAD/bundle.json","state_url":"https://pith.science/pith/2PD75DYZFR6G5CSJMEN4KVPTAD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2PD75DYZFR6G5CSJMEN4KVPTAD/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":"2026-05-31T02:09:12Z","links":{"resolver":"https://pith.science/pith/2PD75DYZFR6G5CSJMEN4KVPTAD","bundle":"https://pith.science/pith/2PD75DYZFR6G5CSJMEN4KVPTAD/bundle.json","state":"https://pith.science/pith/2PD75DYZFR6G5CSJMEN4KVPTAD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2PD75DYZFR6G5CSJMEN4KVPTAD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:2PD75DYZFR6G5CSJMEN4KVPTAD","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":"beee800d90847028f45688ef567650008fe3ca627be08aa55a2c6e267738449e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2010-10-17T22:42:19Z","title_canon_sha256":"958ef955a0b7ca899d6e7ca208754dc063237104f47f7174f2d4f6a70069c430"},"schema_version":"1.0","source":{"id":"1010.3457","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1010.3457","created_at":"2026-05-18T04:30:13Z"},{"alias_kind":"arxiv_version","alias_value":"1010.3457v2","created_at":"2026-05-18T04:30:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.3457","created_at":"2026-05-18T04:30:13Z"},{"alias_kind":"pith_short_12","alias_value":"2PD75DYZFR6G","created_at":"2026-05-18T12:26:03Z"},{"alias_kind":"pith_short_16","alias_value":"2PD75DYZFR6G5CSJ","created_at":"2026-05-18T12:26:03Z"},{"alias_kind":"pith_short_8","alias_value":"2PD75DYZ","created_at":"2026-05-18T12:26:03Z"}],"graph_snapshots":[{"event_id":"sha256:2e105b07d72c62988cf6c28bd72b814c65ffa211295c0a340cbfd00e49b9a5d2","target":"graph","created_at":"2026-05-18T04:30:13Z","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 present calculations and an analysis of the spin-independent dipole electric and magnetic dynamical polarizabilities for the lowest in mass SU(3) octet of baryons. These extensive calculations are made possible by the recent implementation of semi-automatized calculations in Chiral Perturbation Theory which allows evaluating dynamical spin-independent electromagnetic polarizabilities from Compton scattering up to next-to-the-leading order. Our results are in good agreement with calculations performed for nucleons found in the literature. The dependencies for the range of photon energies up ","authors_text":"A. Aleksejevs, S. Barkanova","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2010-10-17T22:42:19Z","title":"Dynamical Polarizabilities of SU(3) Octet of Baryons"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.3457","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:c447a27c1104b87f73c045a9170569fab91d20248ef9aaa914fbe205ccb80b97","target":"record","created_at":"2026-05-18T04:30:13Z","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":"beee800d90847028f45688ef567650008fe3ca627be08aa55a2c6e267738449e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2010-10-17T22:42:19Z","title_canon_sha256":"958ef955a0b7ca899d6e7ca208754dc063237104f47f7174f2d4f6a70069c430"},"schema_version":"1.0","source":{"id":"1010.3457","kind":"arxiv","version":2}},"canonical_sha256":"d3c7fe8f192c7c6e8a49611bc555f300c3944d0dad89518164edc37564fe1f52","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d3c7fe8f192c7c6e8a49611bc555f300c3944d0dad89518164edc37564fe1f52","first_computed_at":"2026-05-18T04:30:13.768575Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:30:13.768575Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ezYdlhAcYq3nUipc8/Vo5Ijq/MoYN7b8rpCgFS2ButSF7tjzOy7j4gcV5OlE3VmRSbLUtzlD/5wDbcY5Md1VCA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:30:13.769073Z","signed_message":"canonical_sha256_bytes"},"source_id":"1010.3457","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c447a27c1104b87f73c045a9170569fab91d20248ef9aaa914fbe205ccb80b97","sha256:2e105b07d72c62988cf6c28bd72b814c65ffa211295c0a340cbfd00e49b9a5d2"],"state_sha256":"f62527181965b565f845e582e28f4adb4c13f36b479610764e1d6f80facb8c3f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Hl8V39cGCMG0XZuYnBvbYGYzZfYr6u3dC6PwE6r3rRR4aQyD3GBeluQ1DBS2WzLCWqXshqETs27aTM68/xucDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T02:09:12.957242Z","bundle_sha256":"f4fbce442275c4453fed938def19f35287fef4b66a253f4dffc1f66c2024cc87"}}