{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:VJO6EVC46RNDYUCYT624PQQ23X","short_pith_number":"pith:VJO6EVC4","canonical_record":{"source":{"id":"1111.4716","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-11-21T02:20:50Z","cross_cats_sorted":[],"title_canon_sha256":"aeb8a4343144eeeaad9fe3d8831168d2b359b45dbae41fd547bac2efe55c996b","abstract_canon_sha256":"ecc1530d508f920994f14d06313f889d6574ba067ef363e0775bd75a7f8d3385"},"schema_version":"1.0"},"canonical_sha256":"aa5de2545cf45a3c50589fb5c7c21addf454f1eb885e96824552f0c63b4388f5","source":{"kind":"arxiv","id":"1111.4716","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1111.4716","created_at":"2026-05-18T01:59:28Z"},{"alias_kind":"arxiv_version","alias_value":"1111.4716v1","created_at":"2026-05-18T01:59:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1111.4716","created_at":"2026-05-18T01:59:28Z"},{"alias_kind":"pith_short_12","alias_value":"VJO6EVC46RND","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_16","alias_value":"VJO6EVC46RNDYUCY","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_8","alias_value":"VJO6EVC4","created_at":"2026-05-18T12:26:44Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:VJO6EVC46RNDYUCYT624PQQ23X","target":"record","payload":{"canonical_record":{"source":{"id":"1111.4716","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-11-21T02:20:50Z","cross_cats_sorted":[],"title_canon_sha256":"aeb8a4343144eeeaad9fe3d8831168d2b359b45dbae41fd547bac2efe55c996b","abstract_canon_sha256":"ecc1530d508f920994f14d06313f889d6574ba067ef363e0775bd75a7f8d3385"},"schema_version":"1.0"},"canonical_sha256":"aa5de2545cf45a3c50589fb5c7c21addf454f1eb885e96824552f0c63b4388f5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:59:28.773407Z","signature_b64":"wjgtdFPIbcFvVcAcaTT/YuagZ7Xs9L5YdcqUfUNk8rhetVEFwFr4uJEXn0THZiJPpVS+Lrv1YO8pTWyQNoyRDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aa5de2545cf45a3c50589fb5c7c21addf454f1eb885e96824552f0c63b4388f5","last_reissued_at":"2026-05-18T01:59:28.772940Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:59:28.772940Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1111.4716","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":"2026-05-18T01:59:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"t7SnqfJDx3s5whSklysaV+olJJ+CPiDup6LvfwGxuiHJpWqO9yafZb8L1ph/Uv1Pu6OBFPH6rtDS428eB9cEDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T00:35:23.108532Z"},"content_sha256":"028f8184643783845204ac5298a6130a40de238e426da8cce43de3f31b93e03f","schema_version":"1.0","event_id":"sha256:028f8184643783845204ac5298a6130a40de238e426da8cce43de3f31b93e03f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:VJO6EVC46RNDYUCYT624PQQ23X","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Parity nonconservation in hyperfine transitions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"V. A. Dzuba, V. V. Flambaum","submitted_at":"2011-11-21T02:20:50Z","abstract_excerpt":"We use relativistic Hartree-Fock and correlation potential methods to calculate nuclear spin-dependent parity non-conserving amplitudes (dominated by the nuclear anapole moment) between hyperfine structure components of the ground state of odd isotopes of K, Rb, Cs, Ba+, Yb+, Tl, Fr, and Ra+. The results are to be used for interpretation of current and future measurements."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1111.4716","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":""},"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":"2026-05-18T01:59:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7LFPR/k26IJ14zcqRvh9WEB/S5RBiIGpEvXixfevB9Uvb9PCAlFj+fHdZrqXIRi3HPETpHddpBsc2FRzPeKiCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T00:35:23.109073Z"},"content_sha256":"a980517112d279354b0b6459d3c8929eba28294e058604e6cb3a64d4177040e0","schema_version":"1.0","event_id":"sha256:a980517112d279354b0b6459d3c8929eba28294e058604e6cb3a64d4177040e0"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VJO6EVC46RNDYUCYT624PQQ23X/bundle.json","state_url":"https://pith.science/pith/VJO6EVC46RNDYUCYT624PQQ23X/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VJO6EVC46RNDYUCYT624PQQ23X/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":"2026-05-27T00:35:23Z","links":{"resolver":"https://pith.science/pith/VJO6EVC46RNDYUCYT624PQQ23X","bundle":"https://pith.science/pith/VJO6EVC46RNDYUCYT624PQQ23X/bundle.json","state":"https://pith.science/pith/VJO6EVC46RNDYUCYT624PQQ23X/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VJO6EVC46RNDYUCYT624PQQ23X/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:VJO6EVC46RNDYUCYT624PQQ23X","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":"ecc1530d508f920994f14d06313f889d6574ba067ef363e0775bd75a7f8d3385","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-11-21T02:20:50Z","title_canon_sha256":"aeb8a4343144eeeaad9fe3d8831168d2b359b45dbae41fd547bac2efe55c996b"},"schema_version":"1.0","source":{"id":"1111.4716","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1111.4716","created_at":"2026-05-18T01:59:28Z"},{"alias_kind":"arxiv_version","alias_value":"1111.4716v1","created_at":"2026-05-18T01:59:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1111.4716","created_at":"2026-05-18T01:59:28Z"},{"alias_kind":"pith_short_12","alias_value":"VJO6EVC46RND","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_16","alias_value":"VJO6EVC46RNDYUCY","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_8","alias_value":"VJO6EVC4","created_at":"2026-05-18T12:26:44Z"}],"graph_snapshots":[{"event_id":"sha256:a980517112d279354b0b6459d3c8929eba28294e058604e6cb3a64d4177040e0","target":"graph","created_at":"2026-05-18T01:59:28Z","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 use relativistic Hartree-Fock and correlation potential methods to calculate nuclear spin-dependent parity non-conserving amplitudes (dominated by the nuclear anapole moment) between hyperfine structure components of the ground state of odd isotopes of K, Rb, Cs, Ba+, Yb+, Tl, Fr, and Ra+. The results are to be used for interpretation of current and future measurements.","authors_text":"V. A. Dzuba, V. V. Flambaum","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-11-21T02:20:50Z","title":"Parity nonconservation in hyperfine transitions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1111.4716","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":"sha256:028f8184643783845204ac5298a6130a40de238e426da8cce43de3f31b93e03f","target":"record","created_at":"2026-05-18T01:59:28Z","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":"ecc1530d508f920994f14d06313f889d6574ba067ef363e0775bd75a7f8d3385","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-11-21T02:20:50Z","title_canon_sha256":"aeb8a4343144eeeaad9fe3d8831168d2b359b45dbae41fd547bac2efe55c996b"},"schema_version":"1.0","source":{"id":"1111.4716","kind":"arxiv","version":1}},"canonical_sha256":"aa5de2545cf45a3c50589fb5c7c21addf454f1eb885e96824552f0c63b4388f5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"aa5de2545cf45a3c50589fb5c7c21addf454f1eb885e96824552f0c63b4388f5","first_computed_at":"2026-05-18T01:59:28.772940Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:59:28.772940Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"wjgtdFPIbcFvVcAcaTT/YuagZ7Xs9L5YdcqUfUNk8rhetVEFwFr4uJEXn0THZiJPpVS+Lrv1YO8pTWyQNoyRDA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:59:28.773407Z","signed_message":"canonical_sha256_bytes"},"source_id":"1111.4716","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:028f8184643783845204ac5298a6130a40de238e426da8cce43de3f31b93e03f","sha256:a980517112d279354b0b6459d3c8929eba28294e058604e6cb3a64d4177040e0"],"state_sha256":"c45ef18287faab1750597f62260bcb4ee11e4745acc54bc79e712333b2ac7bd1"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"H8Tgm4sOP8w5RqKb3DpQaaUFkwGk7HwflAmUKeCpumeI8C3BXWoA3rV4DRN8/qR9xGL+M4ih2fZ+pizsdT9dDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T00:35:23.112073Z","bundle_sha256":"06b831063e6117a2db7ee6d68c41844b04575d91ce4fab4076bd0f4b9b8d91e7"}}