{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:GH6NHVN7QKPVDQSCHRAI53BOJW","short_pith_number":"pith:GH6NHVN7","canonical_record":{"source":{"id":"1708.02129","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-08-07T14:24:44Z","cross_cats_sorted":[],"title_canon_sha256":"346c4bfbbf5af1f70c82262e445c52f7e61ae0fd214600e7bb62ad2c7bc79cf7","abstract_canon_sha256":"ef48d9392a6d715c8bbd4059e03dd045527cf688cd681854b5660b1fd458db17"},"schema_version":"1.0"},"canonical_sha256":"31fcd3d5bf829f51c2423c408eec2e4dbc353bff98aa5c8b8e04bebe563adf15","source":{"kind":"arxiv","id":"1708.02129","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.02129","created_at":"2026-05-18T00:32:39Z"},{"alias_kind":"arxiv_version","alias_value":"1708.02129v3","created_at":"2026-05-18T00:32:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.02129","created_at":"2026-05-18T00:32:39Z"},{"alias_kind":"pith_short_12","alias_value":"GH6NHVN7QKPV","created_at":"2026-05-18T12:31:15Z"},{"alias_kind":"pith_short_16","alias_value":"GH6NHVN7QKPVDQSC","created_at":"2026-05-18T12:31:15Z"},{"alias_kind":"pith_short_8","alias_value":"GH6NHVN7","created_at":"2026-05-18T12:31:15Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:GH6NHVN7QKPVDQSCHRAI53BOJW","target":"record","payload":{"canonical_record":{"source":{"id":"1708.02129","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-08-07T14:24:44Z","cross_cats_sorted":[],"title_canon_sha256":"346c4bfbbf5af1f70c82262e445c52f7e61ae0fd214600e7bb62ad2c7bc79cf7","abstract_canon_sha256":"ef48d9392a6d715c8bbd4059e03dd045527cf688cd681854b5660b1fd458db17"},"schema_version":"1.0"},"canonical_sha256":"31fcd3d5bf829f51c2423c408eec2e4dbc353bff98aa5c8b8e04bebe563adf15","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:32:39.484572Z","signature_b64":"MFXrUCCAr6DRR/BHD/X/15K5KKTBzagL2HheBl4UlfMmvKR2xKwPUFc14feg5w+ObUAF6uTB6L+tmQvkpvl0AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"31fcd3d5bf829f51c2423c408eec2e4dbc353bff98aa5c8b8e04bebe563adf15","last_reissued_at":"2026-05-18T00:32:39.483941Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:32:39.483941Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1708.02129","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:32:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"L4mYZbQZug6eoPGa2/uTla23ZQ/VFdjV9Xe4rtd2/eiRb22H5Am7g8BrbzXbceFP89DImJHJt3Ukgkyy92V1Aw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T13:09:46.058769Z"},"content_sha256":"a1092d2677bce7e9742307382a9d83cadbca24e8193752b97f03e39459f31afc","schema_version":"1.0","event_id":"sha256:a1092d2677bce7e9742307382a9d83cadbca24e8193752b97f03e39459f31afc"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:GH6NHVN7QKPVDQSCHRAI53BOJW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Revival of Raman Coherence of Trapped Atoms","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"Alexander Mil, Gadi Afek, Jonathan Coslovsky, Nir Davidson","submitted_at":"2017-08-07T14:24:44Z","abstract_excerpt":"We perform Raman spectroscopy of optically trapped non interacting \\Rb atoms, and observe revivals of the atomic coherence at integer multiples of the trap period. The effect of coherence control methods such as echo and dynamical decoupling is investigated experimentally, analytically and numerically, along with the effect of the anharmonicity of the trapping potential. The latter is shown to be responsible for incompleteness of the revivals. Coherent Raman control of trapped atoms can be useful in the context of free-oscillation atom intefrerometry and spatial multi-mode quantum memory."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.02129","kind":"arxiv","version":3},"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":"2026-05-18T00:32:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ihZIw8StJYjm1Yk7iQTxWojeQC15DRyKIg6VCeOmmjYy4G27qFqmhrLjfAFijPtnA6xThegM6u13uADOxQ8BDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T13:09:46.059116Z"},"content_sha256":"c150a496f66dcee4fa21bffdbc9f5c2d661369cc4f4107b1548716d780203f1c","schema_version":"1.0","event_id":"sha256:c150a496f66dcee4fa21bffdbc9f5c2d661369cc4f4107b1548716d780203f1c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GH6NHVN7QKPVDQSCHRAI53BOJW/bundle.json","state_url":"https://pith.science/pith/GH6NHVN7QKPVDQSCHRAI53BOJW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GH6NHVN7QKPVDQSCHRAI53BOJW/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":"2026-06-03T13:09:46Z","links":{"resolver":"https://pith.science/pith/GH6NHVN7QKPVDQSCHRAI53BOJW","bundle":"https://pith.science/pith/GH6NHVN7QKPVDQSCHRAI53BOJW/bundle.json","state":"https://pith.science/pith/GH6NHVN7QKPVDQSCHRAI53BOJW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GH6NHVN7QKPVDQSCHRAI53BOJW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:GH6NHVN7QKPVDQSCHRAI53BOJW","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":"ef48d9392a6d715c8bbd4059e03dd045527cf688cd681854b5660b1fd458db17","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-08-07T14:24:44Z","title_canon_sha256":"346c4bfbbf5af1f70c82262e445c52f7e61ae0fd214600e7bb62ad2c7bc79cf7"},"schema_version":"1.0","source":{"id":"1708.02129","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.02129","created_at":"2026-05-18T00:32:39Z"},{"alias_kind":"arxiv_version","alias_value":"1708.02129v3","created_at":"2026-05-18T00:32:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.02129","created_at":"2026-05-18T00:32:39Z"},{"alias_kind":"pith_short_12","alias_value":"GH6NHVN7QKPV","created_at":"2026-05-18T12:31:15Z"},{"alias_kind":"pith_short_16","alias_value":"GH6NHVN7QKPVDQSC","created_at":"2026-05-18T12:31:15Z"},{"alias_kind":"pith_short_8","alias_value":"GH6NHVN7","created_at":"2026-05-18T12:31:15Z"}],"graph_snapshots":[{"event_id":"sha256:c150a496f66dcee4fa21bffdbc9f5c2d661369cc4f4107b1548716d780203f1c","target":"graph","created_at":"2026-05-18T00:32:39Z","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 perform Raman spectroscopy of optically trapped non interacting \\Rb atoms, and observe revivals of the atomic coherence at integer multiples of the trap period. The effect of coherence control methods such as echo and dynamical decoupling is investigated experimentally, analytically and numerically, along with the effect of the anharmonicity of the trapping potential. The latter is shown to be responsible for incompleteness of the revivals. Coherent Raman control of trapped atoms can be useful in the context of free-oscillation atom intefrerometry and spatial multi-mode quantum memory.","authors_text":"Alexander Mil, Gadi Afek, Jonathan Coslovsky, Nir Davidson","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-08-07T14:24:44Z","title":"Revival of Raman Coherence of Trapped Atoms"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.02129","kind":"arxiv","version":3},"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:a1092d2677bce7e9742307382a9d83cadbca24e8193752b97f03e39459f31afc","target":"record","created_at":"2026-05-18T00:32:39Z","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":"ef48d9392a6d715c8bbd4059e03dd045527cf688cd681854b5660b1fd458db17","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-08-07T14:24:44Z","title_canon_sha256":"346c4bfbbf5af1f70c82262e445c52f7e61ae0fd214600e7bb62ad2c7bc79cf7"},"schema_version":"1.0","source":{"id":"1708.02129","kind":"arxiv","version":3}},"canonical_sha256":"31fcd3d5bf829f51c2423c408eec2e4dbc353bff98aa5c8b8e04bebe563adf15","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"31fcd3d5bf829f51c2423c408eec2e4dbc353bff98aa5c8b8e04bebe563adf15","first_computed_at":"2026-05-18T00:32:39.483941Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:32:39.483941Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"MFXrUCCAr6DRR/BHD/X/15K5KKTBzagL2HheBl4UlfMmvKR2xKwPUFc14feg5w+ObUAF6uTB6L+tmQvkpvl0AA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:32:39.484572Z","signed_message":"canonical_sha256_bytes"},"source_id":"1708.02129","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a1092d2677bce7e9742307382a9d83cadbca24e8193752b97f03e39459f31afc","sha256:c150a496f66dcee4fa21bffdbc9f5c2d661369cc4f4107b1548716d780203f1c"],"state_sha256":"5b93f19bfc2cf3af5a5231ba5fb19f7d0047dea1bb773d7e2c22fffb8a23a31c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OcF6c/0iZ1oRnf3bG7N/Kv4kpXFRfXGZj12fWZhlP3pwF4nmHW+8WhwIq8YwUZVnywrPDgzFXdUvrslIH0snDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T13:09:46.061845Z","bundle_sha256":"726d339e97d332b11cb774ae51950c1827947cc25286159a1928e29e69d0043b"}}