{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2009:Y2JG6QSCSIJWRWPBNRLPQYFSML","short_pith_number":"pith:Y2JG6QSC","canonical_record":{"source":{"id":"0903.2090","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2009-03-12T05:23:11Z","cross_cats_sorted":[],"title_canon_sha256":"cdd2fd11c341221234539bec23eb74125f3258f7e768705bf0ea6c9f43c4d466","abstract_canon_sha256":"e65096843dcfb875c92a01776bda233d2a0ae16499e9c4376e9eaa743c6aef71"},"schema_version":"1.0"},"canonical_sha256":"c6926f4242921368d9e16c56f860b262d64f57bc9a7ca6b681184f21504b7f7c","source":{"kind":"arxiv","id":"0903.2090","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0903.2090","created_at":"2026-05-18T04:37:34Z"},{"alias_kind":"arxiv_version","alias_value":"0903.2090v3","created_at":"2026-05-18T04:37:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0903.2090","created_at":"2026-05-18T04:37:34Z"},{"alias_kind":"pith_short_12","alias_value":"Y2JG6QSCSIJW","created_at":"2026-05-18T12:26:02Z"},{"alias_kind":"pith_short_16","alias_value":"Y2JG6QSCSIJWRWPB","created_at":"2026-05-18T12:26:02Z"},{"alias_kind":"pith_short_8","alias_value":"Y2JG6QSC","created_at":"2026-05-18T12:26:02Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2009:Y2JG6QSCSIJWRWPBNRLPQYFSML","target":"record","payload":{"canonical_record":{"source":{"id":"0903.2090","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2009-03-12T05:23:11Z","cross_cats_sorted":[],"title_canon_sha256":"cdd2fd11c341221234539bec23eb74125f3258f7e768705bf0ea6c9f43c4d466","abstract_canon_sha256":"e65096843dcfb875c92a01776bda233d2a0ae16499e9c4376e9eaa743c6aef71"},"schema_version":"1.0"},"canonical_sha256":"c6926f4242921368d9e16c56f860b262d64f57bc9a7ca6b681184f21504b7f7c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:37:34.359224Z","signature_b64":"o0hdcgX0wQ3r6B5qvWZefv4ykZEte5Q23nmLvvCmYcU0MhYch/A6/H9E+BVpn2EPE5y9oBnSmzZV/nfrVLvuDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c6926f4242921368d9e16c56f860b262d64f57bc9a7ca6b681184f21504b7f7c","last_reissued_at":"2026-05-18T04:37:34.358611Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:37:34.358611Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0903.2090","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:37:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nR0cKOuvdY9q3lNTFWyjZTRCdil+PFiejxzMPMaLdMZb0zWpK4TwfOSfZt6QPeroT20yLOImblTaXAtLn9EYBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T11:09:26.666609Z"},"content_sha256":"f927187b51994212d415d9ba544ba8f586f90b4c5d4f44349c4a92245e64d467","schema_version":"1.0","event_id":"sha256:f927187b51994212d415d9ba544ba8f586f90b4c5d4f44349c4a92245e64d467"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2009:Y2JG6QSCSIJWRWPBNRLPQYFSML","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The sensitivity of hyperfine structure to nuclear radius and quark mass variation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"A. Dunning, T. H. Dinh, V. A. Dzuba, V. V. Flambaum","submitted_at":"2009-03-12T05:23:11Z","abstract_excerpt":"To search for the temporal variation of the fundamental constants one needs to know dependence of atomic transition frequencies on these constants. We study the dependence of the hyperfine structure of atomic $s$-levels on nuclear radius and, via radius, on quark masses. An analytical formula has been derived and tested by the numerical relativistic Hartree-Fock calculations for Rb, Cd$^+$, Cs, Yb$^+$ and Hg$^+$. The results of this work allow the use of the results of past and future atomic clock experiments and quasar spectra measurements to put constrains on time variation of the quark mass"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0903.2090","kind":"arxiv","version":3},"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":"2026-05-18T04:37:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"W9T3/NT9Bpd3ikHypFjkXdAwvG7QQhHK4ebubqbosZRi1mqLVzGWFu71OJIMKPaZHYSvWB7m7R2oBoLAN5rRDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T11:09:26.666963Z"},"content_sha256":"56a07328713a913b0549bdee2819a59282313e2ab03758fc88de206c941d1f96","schema_version":"1.0","event_id":"sha256:56a07328713a913b0549bdee2819a59282313e2ab03758fc88de206c941d1f96"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/Y2JG6QSCSIJWRWPBNRLPQYFSML/bundle.json","state_url":"https://pith.science/pith/Y2JG6QSCSIJWRWPBNRLPQYFSML/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/Y2JG6QSCSIJWRWPBNRLPQYFSML/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":"2026-05-26T11:09:26Z","links":{"resolver":"https://pith.science/pith/Y2JG6QSCSIJWRWPBNRLPQYFSML","bundle":"https://pith.science/pith/Y2JG6QSCSIJWRWPBNRLPQYFSML/bundle.json","state":"https://pith.science/pith/Y2JG6QSCSIJWRWPBNRLPQYFSML/state.json","well_known_bundle":"https://pith.science/.well-known/pith/Y2JG6QSCSIJWRWPBNRLPQYFSML/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2009:Y2JG6QSCSIJWRWPBNRLPQYFSML","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":"e65096843dcfb875c92a01776bda233d2a0ae16499e9c4376e9eaa743c6aef71","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2009-03-12T05:23:11Z","title_canon_sha256":"cdd2fd11c341221234539bec23eb74125f3258f7e768705bf0ea6c9f43c4d466"},"schema_version":"1.0","source":{"id":"0903.2090","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0903.2090","created_at":"2026-05-18T04:37:34Z"},{"alias_kind":"arxiv_version","alias_value":"0903.2090v3","created_at":"2026-05-18T04:37:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0903.2090","created_at":"2026-05-18T04:37:34Z"},{"alias_kind":"pith_short_12","alias_value":"Y2JG6QSCSIJW","created_at":"2026-05-18T12:26:02Z"},{"alias_kind":"pith_short_16","alias_value":"Y2JG6QSCSIJWRWPB","created_at":"2026-05-18T12:26:02Z"},{"alias_kind":"pith_short_8","alias_value":"Y2JG6QSC","created_at":"2026-05-18T12:26:02Z"}],"graph_snapshots":[{"event_id":"sha256:56a07328713a913b0549bdee2819a59282313e2ab03758fc88de206c941d1f96","target":"graph","created_at":"2026-05-18T04:37:34Z","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":"To search for the temporal variation of the fundamental constants one needs to know dependence of atomic transition frequencies on these constants. We study the dependence of the hyperfine structure of atomic $s$-levels on nuclear radius and, via radius, on quark masses. An analytical formula has been derived and tested by the numerical relativistic Hartree-Fock calculations for Rb, Cd$^+$, Cs, Yb$^+$ and Hg$^+$. The results of this work allow the use of the results of past and future atomic clock experiments and quasar spectra measurements to put constrains on time variation of the quark mass","authors_text":"A. Dunning, T. H. Dinh, 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":"2009-03-12T05:23:11Z","title":"The sensitivity of hyperfine structure to nuclear radius and quark mass variation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0903.2090","kind":"arxiv","version":3},"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:f927187b51994212d415d9ba544ba8f586f90b4c5d4f44349c4a92245e64d467","target":"record","created_at":"2026-05-18T04:37:34Z","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":"e65096843dcfb875c92a01776bda233d2a0ae16499e9c4376e9eaa743c6aef71","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2009-03-12T05:23:11Z","title_canon_sha256":"cdd2fd11c341221234539bec23eb74125f3258f7e768705bf0ea6c9f43c4d466"},"schema_version":"1.0","source":{"id":"0903.2090","kind":"arxiv","version":3}},"canonical_sha256":"c6926f4242921368d9e16c56f860b262d64f57bc9a7ca6b681184f21504b7f7c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c6926f4242921368d9e16c56f860b262d64f57bc9a7ca6b681184f21504b7f7c","first_computed_at":"2026-05-18T04:37:34.358611Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:37:34.358611Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"o0hdcgX0wQ3r6B5qvWZefv4ykZEte5Q23nmLvvCmYcU0MhYch/A6/H9E+BVpn2EPE5y9oBnSmzZV/nfrVLvuDA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:37:34.359224Z","signed_message":"canonical_sha256_bytes"},"source_id":"0903.2090","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f927187b51994212d415d9ba544ba8f586f90b4c5d4f44349c4a92245e64d467","sha256:56a07328713a913b0549bdee2819a59282313e2ab03758fc88de206c941d1f96"],"state_sha256":"830645d415ba792e5f35a43e69dbc54476564cfd6b09abc348b37fd8e749c9ff"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2ckTkWrL7ZCLFj4/yUoxJMDEkW5nQG4s+zitHThUbS/fBlWNGvo0bkw17gbXvhi+NrG8ZuRibSSja38hHt6EDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T11:09:26.669240Z","bundle_sha256":"0767b051a26f630c63f2fc8262bcd28030d0c2b714ef035f8eeb6cfdcf14f4c5"}}