{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:LBYPNKNAWVVLLJI2JRGN3IF5RY","short_pith_number":"pith:LBYPNKNA","canonical_record":{"source":{"id":"1707.08693","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-07-27T03:21:45Z","cross_cats_sorted":["physics.ins-det","physics.optics"],"title_canon_sha256":"8e137cdb9a1cfe4cd5bf5f031eedcae186c302477e8488615a61b768e6e4693b","abstract_canon_sha256":"2d06de9d707260d042219ae03e37aac9575afa1537bed02e0a18a07d049c1a62"},"schema_version":"1.0"},"canonical_sha256":"5870f6a9a0b56ab5a51a4c4cdda0bd8e1686955c3b5631b090949b0dd9e0793e","source":{"kind":"arxiv","id":"1707.08693","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1707.08693","created_at":"2026-05-18T00:23:56Z"},{"alias_kind":"arxiv_version","alias_value":"1707.08693v4","created_at":"2026-05-18T00:23:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.08693","created_at":"2026-05-18T00:23:56Z"},{"alias_kind":"pith_short_12","alias_value":"LBYPNKNAWVVL","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_16","alias_value":"LBYPNKNAWVVLLJI2","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_8","alias_value":"LBYPNKNA","created_at":"2026-05-18T12:31:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:LBYPNKNAWVVLLJI2JRGN3IF5RY","target":"record","payload":{"canonical_record":{"source":{"id":"1707.08693","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-07-27T03:21:45Z","cross_cats_sorted":["physics.ins-det","physics.optics"],"title_canon_sha256":"8e137cdb9a1cfe4cd5bf5f031eedcae186c302477e8488615a61b768e6e4693b","abstract_canon_sha256":"2d06de9d707260d042219ae03e37aac9575afa1537bed02e0a18a07d049c1a62"},"schema_version":"1.0"},"canonical_sha256":"5870f6a9a0b56ab5a51a4c4cdda0bd8e1686955c3b5631b090949b0dd9e0793e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:23:56.221614Z","signature_b64":"nA8EcTUVRyAQOJxfTD8Rx4vHvXRhmj14QQh3azM9MHZEWw9m/0S3JKca89Wukx7WlT2Rd+Nf0pUirjL8kWD5DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5870f6a9a0b56ab5a51a4c4cdda0bd8e1686955c3b5631b090949b0dd9e0793e","last_reissued_at":"2026-05-18T00:23:56.220958Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:23:56.220958Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1707.08693","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:23:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7g1uSrtxTRBg/gJMMySUbyVMWHI281M7lePaFDRdraT5FPjHeqd1ufZ+sjg4lO7xMJQx4gCUomIRpKn/Ce/sAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-19T16:37:14.664615Z"},"content_sha256":"1cca5e42002125a485c0a6de20058a1cb3826fbad0cdc332ecd9b17fda257b8d","schema_version":"1.0","event_id":"sha256:1cca5e42002125a485c0a6de20058a1cb3826fbad0cdc332ecd9b17fda257b8d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:LBYPNKNAWVVLLJI2JRGN3IF5RY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Multiaxis atom interferometry with a single diode laser and a pyramidal magneto-optical trap","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.ins-det","physics.optics"],"primary_cat":"physics.atom-ph","authors_text":"Fei Zi, Holger M\\\"uller, Jordan Dudley, Philip Canoza, Ryan J. Bilotta, Xuejian Wu","submitted_at":"2017-07-27T03:21:45Z","abstract_excerpt":"Atom interferometry has become one of the most powerful technologies for precision measurements. To develop simple, precise, and versatile atom interferometers for inertial sensing, we demonstrate an atom interferometer measuring acceleration, rotation, and inclination by pointing Raman beams toward individual faces of a pyramidal mirror. Only a single diode laser is used for all functions, including atom trapping, interferometry, and detection. Efficient Doppler-sensitive Raman transitions are achieved without the velocity selecting the atom sample, and with zero differential AC Stark shift b"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.08693","kind":"arxiv","version":4},"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":"2026-05-18T00:23:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dfUAQj4+51ViJGVa+AJ371ZxofZCLM/AYSkYjjjj310gqLTEMF/8bY4WoCbL+bT890PZ12Q4/5wXOcFXPHqXDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-19T16:37:14.664985Z"},"content_sha256":"6eb9f96252746beab891a9a5bb101571aaec8d8a4ed06dbe66af777fe53a4297","schema_version":"1.0","event_id":"sha256:6eb9f96252746beab891a9a5bb101571aaec8d8a4ed06dbe66af777fe53a4297"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LBYPNKNAWVVLLJI2JRGN3IF5RY/bundle.json","state_url":"https://pith.science/pith/LBYPNKNAWVVLLJI2JRGN3IF5RY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LBYPNKNAWVVLLJI2JRGN3IF5RY/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":"2026-05-19T16:37:14Z","links":{"resolver":"https://pith.science/pith/LBYPNKNAWVVLLJI2JRGN3IF5RY","bundle":"https://pith.science/pith/LBYPNKNAWVVLLJI2JRGN3IF5RY/bundle.json","state":"https://pith.science/pith/LBYPNKNAWVVLLJI2JRGN3IF5RY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LBYPNKNAWVVLLJI2JRGN3IF5RY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:LBYPNKNAWVVLLJI2JRGN3IF5RY","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":"2d06de9d707260d042219ae03e37aac9575afa1537bed02e0a18a07d049c1a62","cross_cats_sorted":["physics.ins-det","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-07-27T03:21:45Z","title_canon_sha256":"8e137cdb9a1cfe4cd5bf5f031eedcae186c302477e8488615a61b768e6e4693b"},"schema_version":"1.0","source":{"id":"1707.08693","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1707.08693","created_at":"2026-05-18T00:23:56Z"},{"alias_kind":"arxiv_version","alias_value":"1707.08693v4","created_at":"2026-05-18T00:23:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.08693","created_at":"2026-05-18T00:23:56Z"},{"alias_kind":"pith_short_12","alias_value":"LBYPNKNAWVVL","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_16","alias_value":"LBYPNKNAWVVLLJI2","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_8","alias_value":"LBYPNKNA","created_at":"2026-05-18T12:31:28Z"}],"graph_snapshots":[{"event_id":"sha256:6eb9f96252746beab891a9a5bb101571aaec8d8a4ed06dbe66af777fe53a4297","target":"graph","created_at":"2026-05-18T00:23:56Z","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":"Atom interferometry has become one of the most powerful technologies for precision measurements. To develop simple, precise, and versatile atom interferometers for inertial sensing, we demonstrate an atom interferometer measuring acceleration, rotation, and inclination by pointing Raman beams toward individual faces of a pyramidal mirror. Only a single diode laser is used for all functions, including atom trapping, interferometry, and detection. Efficient Doppler-sensitive Raman transitions are achieved without the velocity selecting the atom sample, and with zero differential AC Stark shift b","authors_text":"Fei Zi, Holger M\\\"uller, Jordan Dudley, Philip Canoza, Ryan J. Bilotta, Xuejian Wu","cross_cats":["physics.ins-det","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-07-27T03:21:45Z","title":"Multiaxis atom interferometry with a single diode laser and a pyramidal magneto-optical trap"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.08693","kind":"arxiv","version":4},"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":"sha256:1cca5e42002125a485c0a6de20058a1cb3826fbad0cdc332ecd9b17fda257b8d","target":"record","created_at":"2026-05-18T00:23:56Z","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":"2d06de9d707260d042219ae03e37aac9575afa1537bed02e0a18a07d049c1a62","cross_cats_sorted":["physics.ins-det","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-07-27T03:21:45Z","title_canon_sha256":"8e137cdb9a1cfe4cd5bf5f031eedcae186c302477e8488615a61b768e6e4693b"},"schema_version":"1.0","source":{"id":"1707.08693","kind":"arxiv","version":4}},"canonical_sha256":"5870f6a9a0b56ab5a51a4c4cdda0bd8e1686955c3b5631b090949b0dd9e0793e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5870f6a9a0b56ab5a51a4c4cdda0bd8e1686955c3b5631b090949b0dd9e0793e","first_computed_at":"2026-05-18T00:23:56.220958Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:23:56.220958Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nA8EcTUVRyAQOJxfTD8Rx4vHvXRhmj14QQh3azM9MHZEWw9m/0S3JKca89Wukx7WlT2Rd+Nf0pUirjL8kWD5DA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:23:56.221614Z","signed_message":"canonical_sha256_bytes"},"source_id":"1707.08693","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1cca5e42002125a485c0a6de20058a1cb3826fbad0cdc332ecd9b17fda257b8d","sha256:6eb9f96252746beab891a9a5bb101571aaec8d8a4ed06dbe66af777fe53a4297"],"state_sha256":"39d8362d17d48b87fd1d8e01ffb394d8901bfad19f59ac17cd96b1c98314cbce"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OSdxNWs1aNrlOomw2tY8tExtLNbSW9E+/WiTc2F+eonI9oy6R0UEBKv7M7f5JvmpIngqdGdoMAiFZzBcH34nAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-19T16:37:14.666956Z","bundle_sha256":"a2a4524b97496696b274a33e695986452bb9416d77348fd44935da8e1aacb95e"}}