{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:DJBZRW42LYZ4SOYMJYDW3G46U5","short_pith_number":"pith:DJBZRW42","schema_version":"1.0","canonical_sha256":"1a4398db9a5e33c93b0c4e076d9b9ea774ccea8247c29cdc25fde3fcfbb28701","source":{"kind":"arxiv","id":"1701.04629","version":1},"attestation_state":"computed","paper":{"title":"A phase shift formulation for N-light-pulse atom interferometers: application to inertial sensing","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"Alexandre Bresson, Alexis Bonnin, Cl\\'ement Diboune, Fabien Th\\'eron, Malo Cadoret, Nassim Zahzam, Yannick Bidel","submitted_at":"2017-01-17T11:51:33Z","abstract_excerpt":"We report on an original and simple formulation of the phase shift in N-light-pulse atom interferometers. We consider atomic interferometers based on two-photon transitions (Raman transitions or Bragg pulses). Starting from the exact analytical phase shift formula obtained from the atom optics ABCD formalism, we use a power series expansion in time of the position of the atomic wave packet with respect to the initial condition. The result of this expansion leads to a formulation of the interferometer phase shift where the leading coefficient in the phase terms up to T^k dependences (k >= 0) in"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1701.04629","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-01-17T11:51:33Z","cross_cats_sorted":[],"title_canon_sha256":"62d43215e0ab43e5fc4ec0486247e05953351aafff96affca389363e49bece95","abstract_canon_sha256":"e987de2ac41cc4889475c3980fe3948a6293e56ed795b225c37c3cc82ffb3a5f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:52:43.075533Z","signature_b64":"ED3Kyp7Z0RoPEBoyZkrtLn/KHyZNWcYDnO3/mSFC+rZna39RgBa8p23Uwq/pfNj46QWkOJj9LLvriblcrxYlBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1a4398db9a5e33c93b0c4e076d9b9ea774ccea8247c29cdc25fde3fcfbb28701","last_reissued_at":"2026-05-18T00:52:43.075017Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:52:43.075017Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A phase shift formulation for N-light-pulse atom interferometers: application to inertial sensing","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"Alexandre Bresson, Alexis Bonnin, Cl\\'ement Diboune, Fabien Th\\'eron, Malo Cadoret, Nassim Zahzam, Yannick Bidel","submitted_at":"2017-01-17T11:51:33Z","abstract_excerpt":"We report on an original and simple formulation of the phase shift in N-light-pulse atom interferometers. We consider atomic interferometers based on two-photon transitions (Raman transitions or Bragg pulses). Starting from the exact analytical phase shift formula obtained from the atom optics ABCD formalism, we use a power series expansion in time of the position of the atomic wave packet with respect to the initial condition. The result of this expansion leads to a formulation of the interferometer phase shift where the leading coefficient in the phase terms up to T^k dependences (k >= 0) in"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.04629","kind":"arxiv","version":1},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1701.04629","created_at":"2026-05-18T00:52:43.075080+00:00"},{"alias_kind":"arxiv_version","alias_value":"1701.04629v1","created_at":"2026-05-18T00:52:43.075080+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.04629","created_at":"2026-05-18T00:52:43.075080+00:00"},{"alias_kind":"pith_short_12","alias_value":"DJBZRW42LYZ4","created_at":"2026-05-18T12:31:10.602751+00:00"},{"alias_kind":"pith_short_16","alias_value":"DJBZRW42LYZ4SOYM","created_at":"2026-05-18T12:31:10.602751+00:00"},{"alias_kind":"pith_short_8","alias_value":"DJBZRW42","created_at":"2026-05-18T12:31:10.602751+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/DJBZRW42LYZ4SOYMJYDW3G46U5","json":"https://pith.science/pith/DJBZRW42LYZ4SOYMJYDW3G46U5.json","graph_json":"https://pith.science/api/pith-number/DJBZRW42LYZ4SOYMJYDW3G46U5/graph.json","events_json":"https://pith.science/api/pith-number/DJBZRW42LYZ4SOYMJYDW3G46U5/events.json","paper":"https://pith.science/paper/DJBZRW42"},"agent_actions":{"view_html":"https://pith.science/pith/DJBZRW42LYZ4SOYMJYDW3G46U5","download_json":"https://pith.science/pith/DJBZRW42LYZ4SOYMJYDW3G46U5.json","view_paper":"https://pith.science/paper/DJBZRW42","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1701.04629&json=true","fetch_graph":"https://pith.science/api/pith-number/DJBZRW42LYZ4SOYMJYDW3G46U5/graph.json","fetch_events":"https://pith.science/api/pith-number/DJBZRW42LYZ4SOYMJYDW3G46U5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DJBZRW42LYZ4SOYMJYDW3G46U5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DJBZRW42LYZ4SOYMJYDW3G46U5/action/storage_attestation","attest_author":"https://pith.science/pith/DJBZRW42LYZ4SOYMJYDW3G46U5/action/author_attestation","sign_citation":"https://pith.science/pith/DJBZRW42LYZ4SOYMJYDW3G46U5/action/citation_signature","submit_replication":"https://pith.science/pith/DJBZRW42LYZ4SOYMJYDW3G46U5/action/replication_record"}},"created_at":"2026-05-18T00:52:43.075080+00:00","updated_at":"2026-05-18T00:52:43.075080+00:00"}