{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:4FW44FHBBT4TSU6UBKKLWEJYTT","short_pith_number":"pith:4FW44FHB","canonical_record":{"source":{"id":"1012.0630","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-12-03T03:42:39Z","cross_cats_sorted":["physics.atom-ph"],"title_canon_sha256":"feca22d478da0f1639e2ab246baf180622c615a3e4e4e19c6f6c47c708c27bf5","abstract_canon_sha256":"fb2eee7ac645ec211e55c3aa3bdfea52f5eef1a7d1362a7fb70f24d9efb41d20"},"schema_version":"1.0"},"canonical_sha256":"e16dce14e10cf93953d40a94bb11389cf4e09dbc40a0e4c46fbe1988fd194c56","source":{"kind":"arxiv","id":"1012.0630","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1012.0630","created_at":"2026-05-18T04:15:50Z"},{"alias_kind":"arxiv_version","alias_value":"1012.0630v1","created_at":"2026-05-18T04:15:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1012.0630","created_at":"2026-05-18T04:15:50Z"},{"alias_kind":"pith_short_12","alias_value":"4FW44FHBBT4T","created_at":"2026-05-18T12:26:03Z"},{"alias_kind":"pith_short_16","alias_value":"4FW44FHBBT4TSU6U","created_at":"2026-05-18T12:26:03Z"},{"alias_kind":"pith_short_8","alias_value":"4FW44FHB","created_at":"2026-05-18T12:26:03Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:4FW44FHBBT4TSU6UBKKLWEJYTT","target":"record","payload":{"canonical_record":{"source":{"id":"1012.0630","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-12-03T03:42:39Z","cross_cats_sorted":["physics.atom-ph"],"title_canon_sha256":"feca22d478da0f1639e2ab246baf180622c615a3e4e4e19c6f6c47c708c27bf5","abstract_canon_sha256":"fb2eee7ac645ec211e55c3aa3bdfea52f5eef1a7d1362a7fb70f24d9efb41d20"},"schema_version":"1.0"},"canonical_sha256":"e16dce14e10cf93953d40a94bb11389cf4e09dbc40a0e4c46fbe1988fd194c56","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:15:50.192230Z","signature_b64":"D8AH2mr4TKU9nHfBTtuBtt71Vl04pDBX+ZwIicWmgQ2Y39pND37TMikkTvuw3DOERLHszOL/hjHT+vPATOqmBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e16dce14e10cf93953d40a94bb11389cf4e09dbc40a0e4c46fbe1988fd194c56","last_reissued_at":"2026-05-18T04:15:50.191717Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:15:50.191717Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1012.0630","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":"2026-05-18T04:15:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WLMnAww6WEsmjFO+sU6aIdLhLabAlwCvv6rbgzScyQhqgljoXnfhmSlYv6hu7zHOiTtX6MXyCW2LkKnxW8/4CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T17:40:08.678184Z"},"content_sha256":"9560e54f1dd79555cb68842f6df2d3cc7660cd38d3e6fea89638fc152fc79803","schema_version":"1.0","event_id":"sha256:9560e54f1dd79555cb68842f6df2d3cc7660cd38d3e6fea89638fc152fc79803"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:4FW44FHBBT4TSU6UBKKLWEJYTT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Lenses as an Atom-Photon Interface: A Semiclassical Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"quant-ph","authors_text":"Colin Teo, Valerio Scarani","submitted_at":"2010-12-03T03:42:39Z","abstract_excerpt":"Strong interaction between the light field and an atom is often achieved with cavities. Recent experiments have used a different configuration: a propagating light field is strongly focused using a system of lenses, the atom being supposed to sit at the focal position. In reality, this last condition holds only up to some approximation; in particular, at any finite temperature, the atom position fluctuates. We present a formalism that describes the focalized field and the atom sitting at an arbitrary position. As a first application, we show that thermal fluctuations do account for the extinct"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1012.0630","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":"2026-05-18T04:15:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"A9fjzsQOrAG3Xr7cnREVxnY5PiSYmBOOfOW5/4UVcwi8hlliQMzd9NdjCvVcEhNAY6mCeCn48EVrrC5EbD/EBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T17:40:08.678847Z"},"content_sha256":"8bcbcb3fd3c5e93be69c2499b6510ae863b4579ee96e272dfc4b0d16e31962c7","schema_version":"1.0","event_id":"sha256:8bcbcb3fd3c5e93be69c2499b6510ae863b4579ee96e272dfc4b0d16e31962c7"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4FW44FHBBT4TSU6UBKKLWEJYTT/bundle.json","state_url":"https://pith.science/pith/4FW44FHBBT4TSU6UBKKLWEJYTT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4FW44FHBBT4TSU6UBKKLWEJYTT/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":"2026-05-28T17:40:08Z","links":{"resolver":"https://pith.science/pith/4FW44FHBBT4TSU6UBKKLWEJYTT","bundle":"https://pith.science/pith/4FW44FHBBT4TSU6UBKKLWEJYTT/bundle.json","state":"https://pith.science/pith/4FW44FHBBT4TSU6UBKKLWEJYTT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4FW44FHBBT4TSU6UBKKLWEJYTT/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:4FW44FHBBT4TSU6UBKKLWEJYTT","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":"fb2eee7ac645ec211e55c3aa3bdfea52f5eef1a7d1362a7fb70f24d9efb41d20","cross_cats_sorted":["physics.atom-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-12-03T03:42:39Z","title_canon_sha256":"feca22d478da0f1639e2ab246baf180622c615a3e4e4e19c6f6c47c708c27bf5"},"schema_version":"1.0","source":{"id":"1012.0630","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1012.0630","created_at":"2026-05-18T04:15:50Z"},{"alias_kind":"arxiv_version","alias_value":"1012.0630v1","created_at":"2026-05-18T04:15:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1012.0630","created_at":"2026-05-18T04:15:50Z"},{"alias_kind":"pith_short_12","alias_value":"4FW44FHBBT4T","created_at":"2026-05-18T12:26:03Z"},{"alias_kind":"pith_short_16","alias_value":"4FW44FHBBT4TSU6U","created_at":"2026-05-18T12:26:03Z"},{"alias_kind":"pith_short_8","alias_value":"4FW44FHB","created_at":"2026-05-18T12:26:03Z"}],"graph_snapshots":[{"event_id":"sha256:8bcbcb3fd3c5e93be69c2499b6510ae863b4579ee96e272dfc4b0d16e31962c7","target":"graph","created_at":"2026-05-18T04:15:50Z","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":"Strong interaction between the light field and an atom is often achieved with cavities. Recent experiments have used a different configuration: a propagating light field is strongly focused using a system of lenses, the atom being supposed to sit at the focal position. In reality, this last condition holds only up to some approximation; in particular, at any finite temperature, the atom position fluctuates. We present a formalism that describes the focalized field and the atom sitting at an arbitrary position. As a first application, we show that thermal fluctuations do account for the extinct","authors_text":"Colin Teo, Valerio Scarani","cross_cats":["physics.atom-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-12-03T03:42:39Z","title":"Lenses as an Atom-Photon Interface: A Semiclassical Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1012.0630","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":"sha256:9560e54f1dd79555cb68842f6df2d3cc7660cd38d3e6fea89638fc152fc79803","target":"record","created_at":"2026-05-18T04:15:50Z","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":"fb2eee7ac645ec211e55c3aa3bdfea52f5eef1a7d1362a7fb70f24d9efb41d20","cross_cats_sorted":["physics.atom-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-12-03T03:42:39Z","title_canon_sha256":"feca22d478da0f1639e2ab246baf180622c615a3e4e4e19c6f6c47c708c27bf5"},"schema_version":"1.0","source":{"id":"1012.0630","kind":"arxiv","version":1}},"canonical_sha256":"e16dce14e10cf93953d40a94bb11389cf4e09dbc40a0e4c46fbe1988fd194c56","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e16dce14e10cf93953d40a94bb11389cf4e09dbc40a0e4c46fbe1988fd194c56","first_computed_at":"2026-05-18T04:15:50.191717Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:15:50.191717Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"D8AH2mr4TKU9nHfBTtuBtt71Vl04pDBX+ZwIicWmgQ2Y39pND37TMikkTvuw3DOERLHszOL/hjHT+vPATOqmBg==","signature_status":"signed_v1","signed_at":"2026-05-18T04:15:50.192230Z","signed_message":"canonical_sha256_bytes"},"source_id":"1012.0630","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9560e54f1dd79555cb68842f6df2d3cc7660cd38d3e6fea89638fc152fc79803","sha256:8bcbcb3fd3c5e93be69c2499b6510ae863b4579ee96e272dfc4b0d16e31962c7"],"state_sha256":"938299c5510c6653ef9b7f81892314e24cca6ed25c1d9cf545a2ead65e4b78b5"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DzD5jIWWhOGryaPYq7idJwpk18Z2BR/B5tz6p3+Jk+ZgaMBq+GlZSWCGpR1GKGvufcAKCBBhJwYDwZvPBx8SAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T17:40:08.682029Z","bundle_sha256":"25f387b427a7cc3d5077b84f2571ec4f6cf1e3f1ba509202cf906fbcd5dcd234"}}