{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:BAFNDBMEU6EA65TFZT2RO7IU4I","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":"07c80b9e7832175d78782d32664d609eb86099d58b06fcc5fe614e70e5fd9c91","cross_cats_sorted":["hep-ex","nucl-th","physics.atom-ph","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2016-12-21T23:32:35Z","title_canon_sha256":"cdab331dbce31feacbc75cf2d59afc4e1b9ca8c4eaa27bec319eff5c62edf5cf"},"schema_version":"1.0","source":{"id":"1612.07390","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1612.07390","created_at":"2026-05-18T00:43:20Z"},{"alias_kind":"arxiv_version","alias_value":"1612.07390v2","created_at":"2026-05-18T00:43:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1612.07390","created_at":"2026-05-18T00:43:20Z"},{"alias_kind":"pith_short_12","alias_value":"BAFNDBMEU6EA","created_at":"2026-05-18T12:30:07Z"},{"alias_kind":"pith_short_16","alias_value":"BAFNDBMEU6EA65TF","created_at":"2026-05-18T12:30:07Z"},{"alias_kind":"pith_short_8","alias_value":"BAFNDBME","created_at":"2026-05-18T12:30:07Z"}],"graph_snapshots":[{"event_id":"sha256:e97060be1f8324b5b785d96b7548fccff7b1a0a353f31cf131d6c9457134319b","target":"graph","created_at":"2026-05-18T00:43:20Z","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 introduce an improved model that links the frequency shift of the $^{133}\\text{Cs}$ hyperfine Zeeman transitions $\\vert F = 3, m_F> \\longleftrightarrow \\vert F = 4, m_F >$ to the Lorentz-violating Standard-Model Extension (SME) coefficients of the proton and neutron. The new model uses Lorentz transformations developed to second order in boost and additionally takes the nuclear structure into account, beyond the simple Schmidt model used previously in SME analyses, thereby providing access to both proton and neutron SME coefficients including the isotropic coefficient $\\tilde{c}_{TT}$. Usin","authors_text":"C. Guerlin, E. Khan, H. Pihan-Le Bars, J.-P. Ebran, P. Wolf, Q. G. Bailey, R.-D. Lasseri, S. Bize","cross_cats":["hep-ex","nucl-th","physics.atom-ph","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2016-12-21T23:32:35Z","title":"Lorentz-symmetry test at Planck-scale suppression with nucleons in a spin-polarized $^{133}$Cs cold atom clock"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1612.07390","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:ef97b33d156d308d020d163b7101ba737c3358586b5ce5ca9b02d132590a4cab","target":"record","created_at":"2026-05-18T00:43:20Z","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":"07c80b9e7832175d78782d32664d609eb86099d58b06fcc5fe614e70e5fd9c91","cross_cats_sorted":["hep-ex","nucl-th","physics.atom-ph","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2016-12-21T23:32:35Z","title_canon_sha256":"cdab331dbce31feacbc75cf2d59afc4e1b9ca8c4eaa27bec319eff5c62edf5cf"},"schema_version":"1.0","source":{"id":"1612.07390","kind":"arxiv","version":2}},"canonical_sha256":"080ad18584a7880f7665ccf5177d14e211b0839f1b9958ce61a25a7b49018dd9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"080ad18584a7880f7665ccf5177d14e211b0839f1b9958ce61a25a7b49018dd9","first_computed_at":"2026-05-18T00:43:20.804402Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:43:20.804402Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"AZYe9wqojyongIp303C0djhbmIuxOymilrYlx6LO55SaOylWAu29kZm76GrMJuoFfSIH8q9Gk1Rxddn4CAbuCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:43:20.804879Z","signed_message":"canonical_sha256_bytes"},"source_id":"1612.07390","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ef97b33d156d308d020d163b7101ba737c3358586b5ce5ca9b02d132590a4cab","sha256:e97060be1f8324b5b785d96b7548fccff7b1a0a353f31cf131d6c9457134319b"],"state_sha256":"e05751538d4b724ab0ba73cfb41f0062576d9eddc54e56bfbd650890c39072c9"}