{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:RSCAGI2AUFUQNPKNPH74SEV6L3","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":"83b8045dad131f9c2f08c0b1fa4d463da59306cb12ac8f50fbddcddff4106d77","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2018-09-28T22:00:06Z","title_canon_sha256":"b8769d6563d601c730e7f1e0335e81935ef662b61186746624beca38284865e0"},"schema_version":"1.0","source":{"id":"1810.00102","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1810.00102","created_at":"2026-05-18T00:04:28Z"},{"alias_kind":"arxiv_version","alias_value":"1810.00102v1","created_at":"2026-05-18T00:04:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1810.00102","created_at":"2026-05-18T00:04:28Z"},{"alias_kind":"pith_short_12","alias_value":"RSCAGI2AUFUQ","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_16","alias_value":"RSCAGI2AUFUQNPKN","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_8","alias_value":"RSCAGI2A","created_at":"2026-05-18T12:32:50Z"}],"graph_snapshots":[{"event_id":"sha256:aaaf111a5ffe19832617d00733372afad730c3264712d76004e3fd04f9705a8d","target":"graph","created_at":"2026-05-18T00:04:28Z","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":"The low-energy electron spectra emitted in the radioactive decay of the $^{83}$Rb and $^{83}$Sr isotopes were measured with a combined electrostatic electron spectrometer. Radioactive sources used were prepared by ion implantation of $^{83}$Sr into a high purity polycrystalline platinum foil at 30 keV and by vacuum-evaporation deposition of\n  $^{83}$ Rb on the same type of foil. From the measured conversion electron spectra, the electron binding energies (referenced to the Fermi level) for the K, L$_1$ , L$_2$ , L$_3$ , M$_1$ , M$_2$, and M$_3$ shell/subshells of krypton in the platinum host w","authors_text":"A.E. Stuchbery, A. Kh. Inoyatov, A. Koval\\'ik, B.Q. Lee, D.V. Filosofov, L.L. Perevoshchikov, M. Ry\\v{s}av\\'y, T. Kib\\'edi, V.S. Zhdanov, Yu.V. Yushkevich","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2018-09-28T22:00:06Z","title":"Influence of host matrices on krypton electron binding energies and KLL Auger transition energies"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1810.00102","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:d7d711573e55354f845c036800c0acc828e84b244959cd9ca99185d45acdbf4f","target":"record","created_at":"2026-05-18T00:04:28Z","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":"83b8045dad131f9c2f08c0b1fa4d463da59306cb12ac8f50fbddcddff4106d77","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2018-09-28T22:00:06Z","title_canon_sha256":"b8769d6563d601c730e7f1e0335e81935ef662b61186746624beca38284865e0"},"schema_version":"1.0","source":{"id":"1810.00102","kind":"arxiv","version":1}},"canonical_sha256":"8c84032340a16906bd4d79ffc912be5ed02aca96c35e2e12b0b9dc406042eba5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8c84032340a16906bd4d79ffc912be5ed02aca96c35e2e12b0b9dc406042eba5","first_computed_at":"2026-05-18T00:04:28.777057Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:04:28.777057Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Ihx7VwcBI5V/fJGMZXLR7vf6MrQFIKecduncpwiZjSpZO4jqKEPLk8+5cLGeqEZdBnasmEzxB4WF4l5q9wmXDA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:04:28.777516Z","signed_message":"canonical_sha256_bytes"},"source_id":"1810.00102","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d7d711573e55354f845c036800c0acc828e84b244959cd9ca99185d45acdbf4f","sha256:aaaf111a5ffe19832617d00733372afad730c3264712d76004e3fd04f9705a8d"],"state_sha256":"22f059c37431509a654ddbfff9e9233458c43f3dd19dc815e5c8b5457e451fb0"}