{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:GHEI27QF4TPOM3SV2WMMMX3ITZ","short_pith_number":"pith:GHEI27QF","canonical_record":{"source":{"id":"1306.5546","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-06-24T09:21:14Z","cross_cats_sorted":[],"title_canon_sha256":"9314c867611eead9bde06f047b1c7d4fbbdb5b0fa4a9300384777b51e8c09e69","abstract_canon_sha256":"542e92ffcd4b9e1fbad78fc462ffcb851c63d62153532bc5ff8d4488fa7d8dc4"},"schema_version":"1.0"},"canonical_sha256":"31c88d7e05e4dee66e55d598c65f689e61a27ddf90f66ef65648c6ca870680b8","source":{"kind":"arxiv","id":"1306.5546","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1306.5546","created_at":"2026-05-18T03:13:09Z"},{"alias_kind":"arxiv_version","alias_value":"1306.5546v2","created_at":"2026-05-18T03:13:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.5546","created_at":"2026-05-18T03:13:09Z"},{"alias_kind":"pith_short_12","alias_value":"GHEI27QF4TPO","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_16","alias_value":"GHEI27QF4TPOM3SV","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_8","alias_value":"GHEI27QF","created_at":"2026-05-18T12:27:45Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:GHEI27QF4TPOM3SV2WMMMX3ITZ","target":"record","payload":{"canonical_record":{"source":{"id":"1306.5546","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-06-24T09:21:14Z","cross_cats_sorted":[],"title_canon_sha256":"9314c867611eead9bde06f047b1c7d4fbbdb5b0fa4a9300384777b51e8c09e69","abstract_canon_sha256":"542e92ffcd4b9e1fbad78fc462ffcb851c63d62153532bc5ff8d4488fa7d8dc4"},"schema_version":"1.0"},"canonical_sha256":"31c88d7e05e4dee66e55d598c65f689e61a27ddf90f66ef65648c6ca870680b8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:13:09.872599Z","signature_b64":"MtZh4D2rmos1FVfsiPwE7cPYdUtZNVy1e3CzjXagqYAdyMKj4drDpmEW9f10051oBuhCZ1w6JZ83c1cYmtBZCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"31c88d7e05e4dee66e55d598c65f689e61a27ddf90f66ef65648c6ca870680b8","last_reissued_at":"2026-05-18T03:13:09.871815Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:13:09.871815Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1306.5546","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":"2026-05-18T03:13:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kgc6TjeJd2dd5zM9M711nUotY+SECR1P/pAVPAkQmalBDeARfjU1R4Gs4CfdHFuBEMolAN7E8fM+/jMtccHMBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T16:53:14.843909Z"},"content_sha256":"718f1b5b980c4dea5c0b99ecbab8cd231bcb7b6c639ca4fe9bee2dc8bd15fb9e","schema_version":"1.0","event_id":"sha256:718f1b5b980c4dea5c0b99ecbab8cd231bcb7b6c639ca4fe9bee2dc8bd15fb9e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:GHEI27QF4TPOM3SV2WMMMX3ITZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The electroweak contributions to (g-2)_\\mu\\ after the Higgs boson mass measurement","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"C. Gnendiger, D. St\\\"ockinger, H. St\\\"ockinger-Kim","submitted_at":"2013-06-24T09:21:14Z","abstract_excerpt":"The Higgs boson mass used to be the only unknown input parameter of the electroweak contributions to (g-2)_\\mu\\ in the Standard Model. It enters at the two-loop level in diagrams with e.g. top loops, W- or Z-exchange. We re-evaluate these contributions, providing analytic expressions and exact numerical results for the Higgs boson mass recently measured at the LHC. Our final result for the full Standard Model electroweak contributions is (153.6\\pm1.0)*10^{-11}, where the remaining theory error comes from unknown three-loop contributions and hadronic uncertainties."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.5546","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":"2026-05-18T03:13:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"p5yQ2aiZpGgeHtmqv3lbMQ6RSqkPWBDmhljCVkldZXaWrAlcQEPuJrbXu9X8kB6aIw2b+U+aU2PMF7pVQcTECg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T16:53:14.844660Z"},"content_sha256":"e8bf1c8301181d79809cb40806377a253f3ca4ad6d87eeca2e8514db922521fb","schema_version":"1.0","event_id":"sha256:e8bf1c8301181d79809cb40806377a253f3ca4ad6d87eeca2e8514db922521fb"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GHEI27QF4TPOM3SV2WMMMX3ITZ/bundle.json","state_url":"https://pith.science/pith/GHEI27QF4TPOM3SV2WMMMX3ITZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GHEI27QF4TPOM3SV2WMMMX3ITZ/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":"2026-05-27T16:53:14Z","links":{"resolver":"https://pith.science/pith/GHEI27QF4TPOM3SV2WMMMX3ITZ","bundle":"https://pith.science/pith/GHEI27QF4TPOM3SV2WMMMX3ITZ/bundle.json","state":"https://pith.science/pith/GHEI27QF4TPOM3SV2WMMMX3ITZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GHEI27QF4TPOM3SV2WMMMX3ITZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:GHEI27QF4TPOM3SV2WMMMX3ITZ","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":"542e92ffcd4b9e1fbad78fc462ffcb851c63d62153532bc5ff8d4488fa7d8dc4","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-06-24T09:21:14Z","title_canon_sha256":"9314c867611eead9bde06f047b1c7d4fbbdb5b0fa4a9300384777b51e8c09e69"},"schema_version":"1.0","source":{"id":"1306.5546","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1306.5546","created_at":"2026-05-18T03:13:09Z"},{"alias_kind":"arxiv_version","alias_value":"1306.5546v2","created_at":"2026-05-18T03:13:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.5546","created_at":"2026-05-18T03:13:09Z"},{"alias_kind":"pith_short_12","alias_value":"GHEI27QF4TPO","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_16","alias_value":"GHEI27QF4TPOM3SV","created_at":"2026-05-18T12:27:45Z"},{"alias_kind":"pith_short_8","alias_value":"GHEI27QF","created_at":"2026-05-18T12:27:45Z"}],"graph_snapshots":[{"event_id":"sha256:e8bf1c8301181d79809cb40806377a253f3ca4ad6d87eeca2e8514db922521fb","target":"graph","created_at":"2026-05-18T03:13:09Z","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 Higgs boson mass used to be the only unknown input parameter of the electroweak contributions to (g-2)_\\mu\\ in the Standard Model. It enters at the two-loop level in diagrams with e.g. top loops, W- or Z-exchange. We re-evaluate these contributions, providing analytic expressions and exact numerical results for the Higgs boson mass recently measured at the LHC. Our final result for the full Standard Model electroweak contributions is (153.6\\pm1.0)*10^{-11}, where the remaining theory error comes from unknown three-loop contributions and hadronic uncertainties.","authors_text":"C. Gnendiger, D. St\\\"ockinger, H. St\\\"ockinger-Kim","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-06-24T09:21:14Z","title":"The electroweak contributions to (g-2)_\\mu\\ after the Higgs boson mass measurement"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.5546","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":"sha256:718f1b5b980c4dea5c0b99ecbab8cd231bcb7b6c639ca4fe9bee2dc8bd15fb9e","target":"record","created_at":"2026-05-18T03:13:09Z","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":"542e92ffcd4b9e1fbad78fc462ffcb851c63d62153532bc5ff8d4488fa7d8dc4","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-06-24T09:21:14Z","title_canon_sha256":"9314c867611eead9bde06f047b1c7d4fbbdb5b0fa4a9300384777b51e8c09e69"},"schema_version":"1.0","source":{"id":"1306.5546","kind":"arxiv","version":2}},"canonical_sha256":"31c88d7e05e4dee66e55d598c65f689e61a27ddf90f66ef65648c6ca870680b8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"31c88d7e05e4dee66e55d598c65f689e61a27ddf90f66ef65648c6ca870680b8","first_computed_at":"2026-05-18T03:13:09.871815Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:13:09.871815Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"MtZh4D2rmos1FVfsiPwE7cPYdUtZNVy1e3CzjXagqYAdyMKj4drDpmEW9f10051oBuhCZ1w6JZ83c1cYmtBZCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:13:09.872599Z","signed_message":"canonical_sha256_bytes"},"source_id":"1306.5546","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:718f1b5b980c4dea5c0b99ecbab8cd231bcb7b6c639ca4fe9bee2dc8bd15fb9e","sha256:e8bf1c8301181d79809cb40806377a253f3ca4ad6d87eeca2e8514db922521fb"],"state_sha256":"2699f6ce406b45df6feec1218ddb295a047e76fc10ee783b6d5e8d1ab3d81488"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"26mVz1RtKCU45bwUbUACmEBGCKxOWCzaO7c13uRR4K4pBCVWwn4yIMSWC7dFS0Ctau5aejjVoKS94zj9mUJmCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T16:53:14.848478Z","bundle_sha256":"e7015ade653a9750b24511294cd5663c1cf74fea4107bf983ac4c2503b75c6b3"}}