{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:4DCAR5LZUPD7SW6CLJLSTZ267U","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":"64ff1a0dee7bd27cff84b49fbcb0a52cec479d846a5cc681130d4416ae3fa4b1","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2026-07-10T23:47:25Z","title_canon_sha256":"061eecda18d3b91120ba515d2a44281376178a4059358f9c1229cadc1d8e329d"},"schema_version":"1.0","source":{"id":"2607.10042","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2607.10042","created_at":"2026-07-14T00:18:49Z"},{"alias_kind":"arxiv_version","alias_value":"2607.10042v1","created_at":"2026-07-14T00:18:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.10042","created_at":"2026-07-14T00:18:49Z"},{"alias_kind":"pith_short_12","alias_value":"4DCAR5LZUPD7","created_at":"2026-07-14T00:18:49Z"},{"alias_kind":"pith_short_16","alias_value":"4DCAR5LZUPD7SW6C","created_at":"2026-07-14T00:18:49Z"},{"alias_kind":"pith_short_8","alias_value":"4DCAR5LZ","created_at":"2026-07-14T00:18:49Z"}],"graph_snapshots":[{"event_id":"sha256:1afa1ace08c477a6c7749772d77074cf5ac4f1d4467cd39e0ad3ae29ffa31d28","target":"graph","created_at":"2026-07-14T00:18:49Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2607.10042/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Atom interferometry is a sensitive tool for measuring relativistic effects, but there are no known non-trivial exact solutions for relativistic atom interferometer phase shifts. Here we derive relativistically exact expressions within the usual semiclassical approximation for a wide range of experimentally interesting atom interferometer pulse sequences in flat spacetime, including Mach-Zehnder, resonant, and large momentum transfer interferometer geometries. As an example, the leading order phase shift $\\omega_a g T^2/c$ for a Mach-Zehnder clock atom interferometer is found to become $\\omega_","authors_text":"Hunter Swan, Jason M. Hogan","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2026-07-10T23:47:25Z","title":"Exact Semiclassical Phase Shifts for Relativistic Atom Interferometers in Flat Spacetime"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.10042","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:edcb6bbde026acc3bde36d38a95dbe5d1d06b45d8561b395fcb48d002aff7d3f","target":"record","created_at":"2026-07-14T00:18:49Z","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":"64ff1a0dee7bd27cff84b49fbcb0a52cec479d846a5cc681130d4416ae3fa4b1","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2026-07-10T23:47:25Z","title_canon_sha256":"061eecda18d3b91120ba515d2a44281376178a4059358f9c1229cadc1d8e329d"},"schema_version":"1.0","source":{"id":"2607.10042","kind":"arxiv","version":1}},"canonical_sha256":"e0c408f579a3c7f95bc25a5729e75efd167defef5d2f0062659949d2943a2204","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e0c408f579a3c7f95bc25a5729e75efd167defef5d2f0062659949d2943a2204","first_computed_at":"2026-07-14T00:18:49.012695Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-14T00:18:49.012695Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"hM1RxL65iQXTsKxh7wNLY/8LdwhhoIhYinEs5ZCbAZgMG/tYFbMnkTX7RHcIMFiVfzjr5iarv7/RCgB8CvlaBA==","signature_status":"signed_v1","signed_at":"2026-07-14T00:18:49.013486Z","signed_message":"canonical_sha256_bytes"},"source_id":"2607.10042","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:edcb6bbde026acc3bde36d38a95dbe5d1d06b45d8561b395fcb48d002aff7d3f","sha256:1afa1ace08c477a6c7749772d77074cf5ac4f1d4467cd39e0ad3ae29ffa31d28"],"state_sha256":"a8077e501335644d19500fc1a8f8bd0e5a8f847ec321fed66534affe9fb6dd04"}