{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:4TOMJ35UIRNB5HC3RPKOUV5KLS","short_pith_number":"pith:4TOMJ35U","canonical_record":{"source":{"id":"1601.01057","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2016-01-06T02:40:01Z","cross_cats_sorted":[],"title_canon_sha256":"5776ec26c2cdfbc8aa6fa3ae7c24f1720e843aa4bc8fedaae2126107ff8bf866","abstract_canon_sha256":"f49f21c8a9097246981c913ed4bde14d0272b9d3df94756196af6eb55a9c55e3"},"schema_version":"1.0"},"canonical_sha256":"e4dcc4efb4445a1e9c5b8bd4ea57aa5cb64d05efcdf9b1a62910cd3aedef96b7","source":{"kind":"arxiv","id":"1601.01057","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1601.01057","created_at":"2026-05-18T01:19:47Z"},{"alias_kind":"arxiv_version","alias_value":"1601.01057v1","created_at":"2026-05-18T01:19:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1601.01057","created_at":"2026-05-18T01:19:47Z"},{"alias_kind":"pith_short_12","alias_value":"4TOMJ35UIRNB","created_at":"2026-05-18T12:29:58Z"},{"alias_kind":"pith_short_16","alias_value":"4TOMJ35UIRNB5HC3","created_at":"2026-05-18T12:29:58Z"},{"alias_kind":"pith_short_8","alias_value":"4TOMJ35U","created_at":"2026-05-18T12:29:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:4TOMJ35UIRNB5HC3RPKOUV5KLS","target":"record","payload":{"canonical_record":{"source":{"id":"1601.01057","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2016-01-06T02:40:01Z","cross_cats_sorted":[],"title_canon_sha256":"5776ec26c2cdfbc8aa6fa3ae7c24f1720e843aa4bc8fedaae2126107ff8bf866","abstract_canon_sha256":"f49f21c8a9097246981c913ed4bde14d0272b9d3df94756196af6eb55a9c55e3"},"schema_version":"1.0"},"canonical_sha256":"e4dcc4efb4445a1e9c5b8bd4ea57aa5cb64d05efcdf9b1a62910cd3aedef96b7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:19:47.399546Z","signature_b64":"XDlXK8P/sdGu1R1gmAEdnYG2ukzOM8ww5pushrlbJJk5gwts09q0zo6w4kDyILpasHDjU7qTI3ogdZOW0xF6Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e4dcc4efb4445a1e9c5b8bd4ea57aa5cb64d05efcdf9b1a62910cd3aedef96b7","last_reissued_at":"2026-05-18T01:19:47.399132Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:19:47.399132Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1601.01057","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":"2026-05-18T01:19:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"taiHvJNQ3YgYFxCwE6YeMGJeczLVaBIoGBM5nNfjY+5X/x/WZDCHciYUCCaO0pTnsAIF49ICPzQMFQMO2VRCCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T16:14:27.735194Z"},"content_sha256":"282f7e5dd5a452b57d09439c9269da74ddd2d8747d14e0798215fa545aeea77b","schema_version":"1.0","event_id":"sha256:282f7e5dd5a452b57d09439c9269da74ddd2d8747d14e0798215fa545aeea77b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:4TOMJ35UIRNB5HC3RPKOUV5KLS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A tabulation of the bound-state energies of atomic hydrogen","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"E.A. Hessels, M. Horbatsch","submitted_at":"2016-01-06T02:40:01Z","abstract_excerpt":"We present tables for the bound-state energies for atomic hydrogen. The tabulated energies include the hyperfine structure, and thus this work extends the work of Rev. Mod. Phys. {\\bf 84}, 1527 (2012), which excludes hyperfine structure. The tabulation includes corrections of the hyperfine structure due to the anomalous moment of the electron, due to the finite mass of the proton, and due to off-diagonal matrix elements of the hyperfine Hamiltonian. These corrections are treated incorrectly in most other works. Simple formulas valid for all quantum numbers are presented for the hyperfine corre"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1601.01057","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":"2026-05-18T01:19:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Vl990/xcuueP/ZbtABtp0o7uBQZW7IV/BdOB+PGbJrxG2ZWYkvEfEhJjgB7cxJ69IBb2frypCI9ZxbMJIw/3DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T16:14:27.735955Z"},"content_sha256":"c98eeba6ec0d6861b9360c04eb7be79553206475f6d6eb41946bf6d07e4ee090","schema_version":"1.0","event_id":"sha256:c98eeba6ec0d6861b9360c04eb7be79553206475f6d6eb41946bf6d07e4ee090"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4TOMJ35UIRNB5HC3RPKOUV5KLS/bundle.json","state_url":"https://pith.science/pith/4TOMJ35UIRNB5HC3RPKOUV5KLS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4TOMJ35UIRNB5HC3RPKOUV5KLS/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":"2026-06-07T16:14:27Z","links":{"resolver":"https://pith.science/pith/4TOMJ35UIRNB5HC3RPKOUV5KLS","bundle":"https://pith.science/pith/4TOMJ35UIRNB5HC3RPKOUV5KLS/bundle.json","state":"https://pith.science/pith/4TOMJ35UIRNB5HC3RPKOUV5KLS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4TOMJ35UIRNB5HC3RPKOUV5KLS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:4TOMJ35UIRNB5HC3RPKOUV5KLS","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":"f49f21c8a9097246981c913ed4bde14d0272b9d3df94756196af6eb55a9c55e3","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2016-01-06T02:40:01Z","title_canon_sha256":"5776ec26c2cdfbc8aa6fa3ae7c24f1720e843aa4bc8fedaae2126107ff8bf866"},"schema_version":"1.0","source":{"id":"1601.01057","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1601.01057","created_at":"2026-05-18T01:19:47Z"},{"alias_kind":"arxiv_version","alias_value":"1601.01057v1","created_at":"2026-05-18T01:19:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1601.01057","created_at":"2026-05-18T01:19:47Z"},{"alias_kind":"pith_short_12","alias_value":"4TOMJ35UIRNB","created_at":"2026-05-18T12:29:58Z"},{"alias_kind":"pith_short_16","alias_value":"4TOMJ35UIRNB5HC3","created_at":"2026-05-18T12:29:58Z"},{"alias_kind":"pith_short_8","alias_value":"4TOMJ35U","created_at":"2026-05-18T12:29:58Z"}],"graph_snapshots":[{"event_id":"sha256:c98eeba6ec0d6861b9360c04eb7be79553206475f6d6eb41946bf6d07e4ee090","target":"graph","created_at":"2026-05-18T01:19:47Z","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 tables for the bound-state energies for atomic hydrogen. The tabulated energies include the hyperfine structure, and thus this work extends the work of Rev. Mod. Phys. {\\bf 84}, 1527 (2012), which excludes hyperfine structure. The tabulation includes corrections of the hyperfine structure due to the anomalous moment of the electron, due to the finite mass of the proton, and due to off-diagonal matrix elements of the hyperfine Hamiltonian. These corrections are treated incorrectly in most other works. Simple formulas valid for all quantum numbers are presented for the hyperfine corre","authors_text":"E.A. Hessels, M. Horbatsch","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2016-01-06T02:40:01Z","title":"A tabulation of the bound-state energies of atomic hydrogen"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1601.01057","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":"sha256:282f7e5dd5a452b57d09439c9269da74ddd2d8747d14e0798215fa545aeea77b","target":"record","created_at":"2026-05-18T01:19:47Z","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":"f49f21c8a9097246981c913ed4bde14d0272b9d3df94756196af6eb55a9c55e3","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2016-01-06T02:40:01Z","title_canon_sha256":"5776ec26c2cdfbc8aa6fa3ae7c24f1720e843aa4bc8fedaae2126107ff8bf866"},"schema_version":"1.0","source":{"id":"1601.01057","kind":"arxiv","version":1}},"canonical_sha256":"e4dcc4efb4445a1e9c5b8bd4ea57aa5cb64d05efcdf9b1a62910cd3aedef96b7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e4dcc4efb4445a1e9c5b8bd4ea57aa5cb64d05efcdf9b1a62910cd3aedef96b7","first_computed_at":"2026-05-18T01:19:47.399132Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:19:47.399132Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"XDlXK8P/sdGu1R1gmAEdnYG2ukzOM8ww5pushrlbJJk5gwts09q0zo6w4kDyILpasHDjU7qTI3ogdZOW0xF6Cg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:19:47.399546Z","signed_message":"canonical_sha256_bytes"},"source_id":"1601.01057","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:282f7e5dd5a452b57d09439c9269da74ddd2d8747d14e0798215fa545aeea77b","sha256:c98eeba6ec0d6861b9360c04eb7be79553206475f6d6eb41946bf6d07e4ee090"],"state_sha256":"674b23e03a44f3b49bbf798fc7d4a19c6f7a0f7c75bd99246372071baece1274"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UbhO5KnIaWzHNTVArWMPOxW9i6/9P6JTG2LrOcXT04rPuUoUpun1h0vesMoehy2DjSBi8TEwM/BDlCDJvgOEDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-07T16:14:27.739621Z","bundle_sha256":"1d087a1d33db949d3f328891b55ba64f6a66d2553bbdc8ef4750cdc2f6c172fa"}}