{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:3AIR4N7HJ33QG7C4GOAWOAB7RO","short_pith_number":"pith:3AIR4N7H","canonical_record":{"source":{"id":"1406.6501","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2014-06-25T08:57:54Z","cross_cats_sorted":[],"title_canon_sha256":"22c19c1783fc8bbf1c7504d57ede7414fa84dc9ca67ee9349840ae5190ab84d8","abstract_canon_sha256":"988e047386c4de0001a0c0159cd5410e53a28c01a0088676ad81c7edeab781ec"},"schema_version":"1.0"},"canonical_sha256":"d8111e37e74ef7037c5c338167003f8b9f9413a2c6bb79d2cbfe08fe5cf8410c","source":{"kind":"arxiv","id":"1406.6501","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1406.6501","created_at":"2026-05-18T02:48:54Z"},{"alias_kind":"arxiv_version","alias_value":"1406.6501v2","created_at":"2026-05-18T02:48:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1406.6501","created_at":"2026-05-18T02:48:54Z"},{"alias_kind":"pith_short_12","alias_value":"3AIR4N7HJ33Q","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_16","alias_value":"3AIR4N7HJ33QG7C4","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_8","alias_value":"3AIR4N7H","created_at":"2026-05-18T12:28:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:3AIR4N7HJ33QG7C4GOAWOAB7RO","target":"record","payload":{"canonical_record":{"source":{"id":"1406.6501","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2014-06-25T08:57:54Z","cross_cats_sorted":[],"title_canon_sha256":"22c19c1783fc8bbf1c7504d57ede7414fa84dc9ca67ee9349840ae5190ab84d8","abstract_canon_sha256":"988e047386c4de0001a0c0159cd5410e53a28c01a0088676ad81c7edeab781ec"},"schema_version":"1.0"},"canonical_sha256":"d8111e37e74ef7037c5c338167003f8b9f9413a2c6bb79d2cbfe08fe5cf8410c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:48:54.403889Z","signature_b64":"1dWWUhr1+KfDyT9xnleIGoBX0ZN1XoNeOaN0Y2VFK6dF890NldBeHU6OIC8dzT8B6nLiM0lizRKoEvCQhx/IAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d8111e37e74ef7037c5c338167003f8b9f9413a2c6bb79d2cbfe08fe5cf8410c","last_reissued_at":"2026-05-18T02:48:54.403285Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:48:54.403285Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1406.6501","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":"2026-05-18T02:48:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fTqqEZRrORQJXqQostO4QwRPnqYpkwWWAFt8HUEJKrLlZ5qq7yrq2T8oyvWLJqAU3XTQaqHsuPeMLEOZlPYADQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-25T14:08:32.373618Z"},"content_sha256":"a337c7e8407cab844036ae2e9e44933ca7e8ef1d2c76386ae8fd222920c65ad5","schema_version":"1.0","event_id":"sha256:a337c7e8407cab844036ae2e9e44933ca7e8ef1d2c76386ae8fd222920c65ad5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:3AIR4N7HJ33QG7C4GOAWOAB7RO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"g factor of lithiumlike silicon 28Si11+","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"Andrey V. Volotka, Anke Wagner, Dmitry A. Glazov, Florian K\\\"ohler, G\\\"unter Plunien, G\\\"unter Werth, Klaus Blaum, Sven Sturm, Vladimir M. Shabaev, Wolfgang Quint","submitted_at":"2014-06-25T08:57:54Z","abstract_excerpt":"The g factor of lithiumlike 28Si11+ has been measured in a triple-Penning trap with a relative uncertainty of 1.1x10^{-9} to be g_exp=2.0008898899(21). The theoretical prediction for this value was calculated to be g_th=2.000889909(51) improving the accuracy to 2.5x10^{-8} due to the first rigorous evaluation of the two-photon exchange correction. The measured value is in excellent agreement with the state-of-the-art theoretical prediction and yields the most stringent test of bound-state QED for the g factor of the 1s^22s state and the relativistic many-electron calculations in a magnetic fie"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1406.6501","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":"2026-05-18T02:48:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"EQjEwuMyskU9/KlXKtGBzKs0sjkvbPzQirl3a7HgFoUSQT04Bxa+823dosG2TvudoPGpEzDiHoeg7Q7bXg4bAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-25T14:08:32.373969Z"},"content_sha256":"fb8dacb97540916f5a978e37638c8e349a10100e66d97714057908beaf7cc45f","schema_version":"1.0","event_id":"sha256:fb8dacb97540916f5a978e37638c8e349a10100e66d97714057908beaf7cc45f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3AIR4N7HJ33QG7C4GOAWOAB7RO/bundle.json","state_url":"https://pith.science/pith/3AIR4N7HJ33QG7C4GOAWOAB7RO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3AIR4N7HJ33QG7C4GOAWOAB7RO/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":"2026-06-25T14:08:32Z","links":{"resolver":"https://pith.science/pith/3AIR4N7HJ33QG7C4GOAWOAB7RO","bundle":"https://pith.science/pith/3AIR4N7HJ33QG7C4GOAWOAB7RO/bundle.json","state":"https://pith.science/pith/3AIR4N7HJ33QG7C4GOAWOAB7RO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3AIR4N7HJ33QG7C4GOAWOAB7RO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:3AIR4N7HJ33QG7C4GOAWOAB7RO","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":"988e047386c4de0001a0c0159cd5410e53a28c01a0088676ad81c7edeab781ec","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2014-06-25T08:57:54Z","title_canon_sha256":"22c19c1783fc8bbf1c7504d57ede7414fa84dc9ca67ee9349840ae5190ab84d8"},"schema_version":"1.0","source":{"id":"1406.6501","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1406.6501","created_at":"2026-05-18T02:48:54Z"},{"alias_kind":"arxiv_version","alias_value":"1406.6501v2","created_at":"2026-05-18T02:48:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1406.6501","created_at":"2026-05-18T02:48:54Z"},{"alias_kind":"pith_short_12","alias_value":"3AIR4N7HJ33Q","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_16","alias_value":"3AIR4N7HJ33QG7C4","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_8","alias_value":"3AIR4N7H","created_at":"2026-05-18T12:28:11Z"}],"graph_snapshots":[{"event_id":"sha256:fb8dacb97540916f5a978e37638c8e349a10100e66d97714057908beaf7cc45f","target":"graph","created_at":"2026-05-18T02:48:54Z","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 g factor of lithiumlike 28Si11+ has been measured in a triple-Penning trap with a relative uncertainty of 1.1x10^{-9} to be g_exp=2.0008898899(21). The theoretical prediction for this value was calculated to be g_th=2.000889909(51) improving the accuracy to 2.5x10^{-8} due to the first rigorous evaluation of the two-photon exchange correction. The measured value is in excellent agreement with the state-of-the-art theoretical prediction and yields the most stringent test of bound-state QED for the g factor of the 1s^22s state and the relativistic many-electron calculations in a magnetic fie","authors_text":"Andrey V. Volotka, Anke Wagner, Dmitry A. Glazov, Florian K\\\"ohler, G\\\"unter Plunien, G\\\"unter Werth, Klaus Blaum, Sven Sturm, Vladimir M. Shabaev, Wolfgang Quint","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2014-06-25T08:57:54Z","title":"g factor of lithiumlike silicon 28Si11+"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1406.6501","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:a337c7e8407cab844036ae2e9e44933ca7e8ef1d2c76386ae8fd222920c65ad5","target":"record","created_at":"2026-05-18T02:48:54Z","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":"988e047386c4de0001a0c0159cd5410e53a28c01a0088676ad81c7edeab781ec","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2014-06-25T08:57:54Z","title_canon_sha256":"22c19c1783fc8bbf1c7504d57ede7414fa84dc9ca67ee9349840ae5190ab84d8"},"schema_version":"1.0","source":{"id":"1406.6501","kind":"arxiv","version":2}},"canonical_sha256":"d8111e37e74ef7037c5c338167003f8b9f9413a2c6bb79d2cbfe08fe5cf8410c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d8111e37e74ef7037c5c338167003f8b9f9413a2c6bb79d2cbfe08fe5cf8410c","first_computed_at":"2026-05-18T02:48:54.403285Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:48:54.403285Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"1dWWUhr1+KfDyT9xnleIGoBX0ZN1XoNeOaN0Y2VFK6dF890NldBeHU6OIC8dzT8B6nLiM0lizRKoEvCQhx/IAA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:48:54.403889Z","signed_message":"canonical_sha256_bytes"},"source_id":"1406.6501","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a337c7e8407cab844036ae2e9e44933ca7e8ef1d2c76386ae8fd222920c65ad5","sha256:fb8dacb97540916f5a978e37638c8e349a10100e66d97714057908beaf7cc45f"],"state_sha256":"3b194974929abedb4ac28833bf51d64a7ac7dc6f02e3d7bae4d3c64ac1d01774"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BTIx7XVRwZDoETLdO1JJB0hNcRL8Cdq3AFxznlSOEjBT3g4jf+3mP2QDivK9KvPqojfT0Qfu84x9ZPTQUH0BAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-25T14:08:32.375990Z","bundle_sha256":"87d231589fd399707fb49c2ef3ce29b3ca2b10b71deedba58a90867b942dd9b9"}}