{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:JIFCOQVS3I5IHEZB4UBOZZ5ZLM","short_pith_number":"pith:JIFCOQVS","canonical_record":{"source":{"id":"1007.2661","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-07-15T21:26:20Z","cross_cats_sorted":["physics.atom-ph"],"title_canon_sha256":"4f251c2988ad663c401e08bf9be9b75c184e13bee41dbcf093c190e2c5bfdac0","abstract_canon_sha256":"64bf5cdac6f863b0bb8a8c95574343988a0bfe56b22b2ce0d5c5974ae9c9b618"},"schema_version":"1.0"},"canonical_sha256":"4a0a2742b2da3a839321e502ece7b95b096b0ab15937b0e2b348e7836ea66dcd","source":{"kind":"arxiv","id":"1007.2661","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1007.2661","created_at":"2026-05-18T02:06:21Z"},{"alias_kind":"arxiv_version","alias_value":"1007.2661v1","created_at":"2026-05-18T02:06:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1007.2661","created_at":"2026-05-18T02:06:21Z"},{"alias_kind":"pith_short_12","alias_value":"JIFCOQVS3I5I","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_16","alias_value":"JIFCOQVS3I5IHEZB","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_8","alias_value":"JIFCOQVS","created_at":"2026-05-18T12:26:09Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:JIFCOQVS3I5IHEZB4UBOZZ5ZLM","target":"record","payload":{"canonical_record":{"source":{"id":"1007.2661","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-07-15T21:26:20Z","cross_cats_sorted":["physics.atom-ph"],"title_canon_sha256":"4f251c2988ad663c401e08bf9be9b75c184e13bee41dbcf093c190e2c5bfdac0","abstract_canon_sha256":"64bf5cdac6f863b0bb8a8c95574343988a0bfe56b22b2ce0d5c5974ae9c9b618"},"schema_version":"1.0"},"canonical_sha256":"4a0a2742b2da3a839321e502ece7b95b096b0ab15937b0e2b348e7836ea66dcd","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:06:21.456738Z","signature_b64":"rdWPQ/OqiUa3d3B2tSx9qDz/d+Y4MdSMIPoWjCcTa8v3EVSd3oNguBSbyasZPJahiXK3wBEva4AvGYN/1KPWBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4a0a2742b2da3a839321e502ece7b95b096b0ab15937b0e2b348e7836ea66dcd","last_reissued_at":"2026-05-18T02:06:21.456113Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:06:21.456113Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1007.2661","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:06:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AzbXfstrayLT/TWZHz6es4cWcLwsIlgduJOJFxXpoiYcNv3e2dPMnN17ynMn+lxBmOrvYdn8Ef1BqfPAR40VAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T15:29:45.666248Z"},"content_sha256":"7eb281effb67b22f4f93ab17f162522e8d494f66bf339d69d41ae404406e125a","schema_version":"1.0","event_id":"sha256:7eb281effb67b22f4f93ab17f162522e8d494f66bf339d69d41ae404406e125a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:JIFCOQVS3I5IHEZB4UBOZZ5ZLM","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Decoherence due to elastic Rayleigh scattering","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"quant-ph","authors_text":"A.P. VanDevender, C. Ospelkaus, D. Meiser, H. Uys, J.J. Bollinger, M.J. Biercuk, R. Ozeri","submitted_at":"2010-07-15T21:26:20Z","abstract_excerpt":"We present theoretical and experimental studies of the decoherence of hyperfine ground-state superpositions due to elastic Rayleigh scattering of light off-resonant with higher lying excited states. We demonstrate that under appropriate conditions, elastic Rayleigh scattering can be the dominant source of decoherence, contrary to previous discussions in the literature. We show that the elastic-scattering decoherence rate of a two-level system is given by the square of the difference between the elastic-scattering \\textit{amplitudes} for the two levels, and that for certain detunings of the lig"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1007.2661","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:06:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UCathf6inQkf8nZKazDuBbiPLX2cW4hLGbIepnOgl+Lndu0qJE8CQe4CZWLU4FtC2kNu4cKbv6A47djNtctVAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T15:29:45.666981Z"},"content_sha256":"9abbe8762e6087f37eb0bb9a2880747d29f60d582989b19c5f46e3a77636dd4f","schema_version":"1.0","event_id":"sha256:9abbe8762e6087f37eb0bb9a2880747d29f60d582989b19c5f46e3a77636dd4f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JIFCOQVS3I5IHEZB4UBOZZ5ZLM/bundle.json","state_url":"https://pith.science/pith/JIFCOQVS3I5IHEZB4UBOZZ5ZLM/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JIFCOQVS3I5IHEZB4UBOZZ5ZLM/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":"2026-05-27T15:29:45Z","links":{"resolver":"https://pith.science/pith/JIFCOQVS3I5IHEZB4UBOZZ5ZLM","bundle":"https://pith.science/pith/JIFCOQVS3I5IHEZB4UBOZZ5ZLM/bundle.json","state":"https://pith.science/pith/JIFCOQVS3I5IHEZB4UBOZZ5ZLM/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JIFCOQVS3I5IHEZB4UBOZZ5ZLM/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:JIFCOQVS3I5IHEZB4UBOZZ5ZLM","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":"64bf5cdac6f863b0bb8a8c95574343988a0bfe56b22b2ce0d5c5974ae9c9b618","cross_cats_sorted":["physics.atom-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-07-15T21:26:20Z","title_canon_sha256":"4f251c2988ad663c401e08bf9be9b75c184e13bee41dbcf093c190e2c5bfdac0"},"schema_version":"1.0","source":{"id":"1007.2661","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1007.2661","created_at":"2026-05-18T02:06:21Z"},{"alias_kind":"arxiv_version","alias_value":"1007.2661v1","created_at":"2026-05-18T02:06:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1007.2661","created_at":"2026-05-18T02:06:21Z"},{"alias_kind":"pith_short_12","alias_value":"JIFCOQVS3I5I","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_16","alias_value":"JIFCOQVS3I5IHEZB","created_at":"2026-05-18T12:26:09Z"},{"alias_kind":"pith_short_8","alias_value":"JIFCOQVS","created_at":"2026-05-18T12:26:09Z"}],"graph_snapshots":[{"event_id":"sha256:9abbe8762e6087f37eb0bb9a2880747d29f60d582989b19c5f46e3a77636dd4f","target":"graph","created_at":"2026-05-18T02:06:21Z","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 present theoretical and experimental studies of the decoherence of hyperfine ground-state superpositions due to elastic Rayleigh scattering of light off-resonant with higher lying excited states. We demonstrate that under appropriate conditions, elastic Rayleigh scattering can be the dominant source of decoherence, contrary to previous discussions in the literature. We show that the elastic-scattering decoherence rate of a two-level system is given by the square of the difference between the elastic-scattering \\textit{amplitudes} for the two levels, and that for certain detunings of the lig","authors_text":"A.P. VanDevender, C. Ospelkaus, D. Meiser, H. Uys, J.J. Bollinger, M.J. Biercuk, R. Ozeri","cross_cats":["physics.atom-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-07-15T21:26:20Z","title":"Decoherence due to elastic Rayleigh scattering"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1007.2661","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":"sha256:7eb281effb67b22f4f93ab17f162522e8d494f66bf339d69d41ae404406e125a","target":"record","created_at":"2026-05-18T02:06:21Z","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":"64bf5cdac6f863b0bb8a8c95574343988a0bfe56b22b2ce0d5c5974ae9c9b618","cross_cats_sorted":["physics.atom-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-07-15T21:26:20Z","title_canon_sha256":"4f251c2988ad663c401e08bf9be9b75c184e13bee41dbcf093c190e2c5bfdac0"},"schema_version":"1.0","source":{"id":"1007.2661","kind":"arxiv","version":1}},"canonical_sha256":"4a0a2742b2da3a839321e502ece7b95b096b0ab15937b0e2b348e7836ea66dcd","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4a0a2742b2da3a839321e502ece7b95b096b0ab15937b0e2b348e7836ea66dcd","first_computed_at":"2026-05-18T02:06:21.456113Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:06:21.456113Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"rdWPQ/OqiUa3d3B2tSx9qDz/d+Y4MdSMIPoWjCcTa8v3EVSd3oNguBSbyasZPJahiXK3wBEva4AvGYN/1KPWBg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:06:21.456738Z","signed_message":"canonical_sha256_bytes"},"source_id":"1007.2661","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7eb281effb67b22f4f93ab17f162522e8d494f66bf339d69d41ae404406e125a","sha256:9abbe8762e6087f37eb0bb9a2880747d29f60d582989b19c5f46e3a77636dd4f"],"state_sha256":"82a4d95b143d8ed972983f95e1080e1e42bd0e0820a893e07cca40714285b530"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kLEvxSskYYwePRUapVynv7FI7BLJn3khIIpULqciZ8Jl34tfDfEBR+YyI9KkWThE0n3XRQ85oCvtwLwqbQVHCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T15:29:45.670543Z","bundle_sha256":"7ce88a0648bc094547e51d99662dfb547205d869af351b7803ac4cf28d6789bf"}}