{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:D7F3FM2R6HUAR6IUH73KJRACJ7","short_pith_number":"pith:D7F3FM2R","canonical_record":{"source":{"id":"1010.1903","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-10-10T09:01:48Z","cross_cats_sorted":[],"title_canon_sha256":"8907476d368fddf97bd006f3c2f51be869b3a0c6b87d6c7a3a1a8d6e06b7c5f4","abstract_canon_sha256":"d5904479a1371d01a4b1c51e255eb1e460ac8c5b69f2de49d759aa489f019df9"},"schema_version":"1.0"},"canonical_sha256":"1fcbb2b351f1e808f9143ff6a4c4024fe9ce5ee3bc93aa3a284c432d2a8d956d","source":{"kind":"arxiv","id":"1010.1903","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1010.1903","created_at":"2026-05-18T04:26:55Z"},{"alias_kind":"arxiv_version","alias_value":"1010.1903v1","created_at":"2026-05-18T04:26:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.1903","created_at":"2026-05-18T04:26:55Z"},{"alias_kind":"pith_short_12","alias_value":"D7F3FM2R6HUA","created_at":"2026-05-18T12:26:06Z"},{"alias_kind":"pith_short_16","alias_value":"D7F3FM2R6HUAR6IU","created_at":"2026-05-18T12:26:06Z"},{"alias_kind":"pith_short_8","alias_value":"D7F3FM2R","created_at":"2026-05-18T12:26:06Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:D7F3FM2R6HUAR6IUH73KJRACJ7","target":"record","payload":{"canonical_record":{"source":{"id":"1010.1903","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-10-10T09:01:48Z","cross_cats_sorted":[],"title_canon_sha256":"8907476d368fddf97bd006f3c2f51be869b3a0c6b87d6c7a3a1a8d6e06b7c5f4","abstract_canon_sha256":"d5904479a1371d01a4b1c51e255eb1e460ac8c5b69f2de49d759aa489f019df9"},"schema_version":"1.0"},"canonical_sha256":"1fcbb2b351f1e808f9143ff6a4c4024fe9ce5ee3bc93aa3a284c432d2a8d956d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:26:55.550646Z","signature_b64":"tCjEF21yTPHFicuOe8rS3G6j84Zas+2+PAn+SdowMZXCfAaPDPtePgFR6xVaUMk8WCIgl5jXNsjCUjDHjqspBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1fcbb2b351f1e808f9143ff6a4c4024fe9ce5ee3bc93aa3a284c432d2a8d956d","last_reissued_at":"2026-05-18T04:26:55.550278Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:26:55.550278Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1010.1903","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":"2026-05-18T04:26:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Q0YfiE27DuaChNHHYQCUrbwiSUDIMNDEGl3CIKn/zM+66SrD2m4q3MmvJ/62Egw9DE6QKrhcKySdrYKJ2XGOBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T20:03:14.139281Z"},"content_sha256":"8a7738058caeb5c806d1738fa8ea0092a227a86351342a0c524b6689389bd66f","schema_version":"1.0","event_id":"sha256:8a7738058caeb5c806d1738fa8ea0092a227a86351342a0c524b6689389bd66f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:D7F3FM2R6HUAR6IUH73KJRACJ7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Interaction of an atom with layered dielectrics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Claudia Eberlein, Robert Zietal","submitted_at":"2010-10-10T09:01:48Z","abstract_excerpt":"We determine the energy-level shift experienced by a neutral atom due the quantum electromagnetic interaction with a layered dielectric body. We use the technique of normal-mode expansion to quantize the electromagnetic field in the presence of a layered, non-dispersive and non-absorptive dielectric. We explicitly calculate the equal-time commutation relations between the electric field and vector potential operators. We show that the commutator can be expressed in terms of a generalized transverse delta-function and that this is a consequence of using the generalized Coulomb gauge to quantize"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.1903","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":"2026-05-18T04:26:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"avQbLGA2UnoFMdN3/ZbwGfVfx0eUEYXrnMasDVHt+yp8TIFl4pUqJ0uE9e8IjCEed6h7xTnIMPRTVxNSV9SbBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T20:03:14.139726Z"},"content_sha256":"fc913c3bd4f9f6ad4485cd7bbd076492f921977bb25d67258a905d3ec53e7bf5","schema_version":"1.0","event_id":"sha256:fc913c3bd4f9f6ad4485cd7bbd076492f921977bb25d67258a905d3ec53e7bf5"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/D7F3FM2R6HUAR6IUH73KJRACJ7/bundle.json","state_url":"https://pith.science/pith/D7F3FM2R6HUAR6IUH73KJRACJ7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/D7F3FM2R6HUAR6IUH73KJRACJ7/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":"2026-05-26T20:03:14Z","links":{"resolver":"https://pith.science/pith/D7F3FM2R6HUAR6IUH73KJRACJ7","bundle":"https://pith.science/pith/D7F3FM2R6HUAR6IUH73KJRACJ7/bundle.json","state":"https://pith.science/pith/D7F3FM2R6HUAR6IUH73KJRACJ7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/D7F3FM2R6HUAR6IUH73KJRACJ7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:D7F3FM2R6HUAR6IUH73KJRACJ7","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":"d5904479a1371d01a4b1c51e255eb1e460ac8c5b69f2de49d759aa489f019df9","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-10-10T09:01:48Z","title_canon_sha256":"8907476d368fddf97bd006f3c2f51be869b3a0c6b87d6c7a3a1a8d6e06b7c5f4"},"schema_version":"1.0","source":{"id":"1010.1903","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1010.1903","created_at":"2026-05-18T04:26:55Z"},{"alias_kind":"arxiv_version","alias_value":"1010.1903v1","created_at":"2026-05-18T04:26:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.1903","created_at":"2026-05-18T04:26:55Z"},{"alias_kind":"pith_short_12","alias_value":"D7F3FM2R6HUA","created_at":"2026-05-18T12:26:06Z"},{"alias_kind":"pith_short_16","alias_value":"D7F3FM2R6HUAR6IU","created_at":"2026-05-18T12:26:06Z"},{"alias_kind":"pith_short_8","alias_value":"D7F3FM2R","created_at":"2026-05-18T12:26:06Z"}],"graph_snapshots":[{"event_id":"sha256:fc913c3bd4f9f6ad4485cd7bbd076492f921977bb25d67258a905d3ec53e7bf5","target":"graph","created_at":"2026-05-18T04:26:55Z","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 determine the energy-level shift experienced by a neutral atom due the quantum electromagnetic interaction with a layered dielectric body. We use the technique of normal-mode expansion to quantize the electromagnetic field in the presence of a layered, non-dispersive and non-absorptive dielectric. We explicitly calculate the equal-time commutation relations between the electric field and vector potential operators. We show that the commutator can be expressed in terms of a generalized transverse delta-function and that this is a consequence of using the generalized Coulomb gauge to quantize","authors_text":"Claudia Eberlein, Robert Zietal","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-10-10T09:01:48Z","title":"Interaction of an atom with layered dielectrics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.1903","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":"sha256:8a7738058caeb5c806d1738fa8ea0092a227a86351342a0c524b6689389bd66f","target":"record","created_at":"2026-05-18T04:26:55Z","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":"d5904479a1371d01a4b1c51e255eb1e460ac8c5b69f2de49d759aa489f019df9","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2010-10-10T09:01:48Z","title_canon_sha256":"8907476d368fddf97bd006f3c2f51be869b3a0c6b87d6c7a3a1a8d6e06b7c5f4"},"schema_version":"1.0","source":{"id":"1010.1903","kind":"arxiv","version":1}},"canonical_sha256":"1fcbb2b351f1e808f9143ff6a4c4024fe9ce5ee3bc93aa3a284c432d2a8d956d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1fcbb2b351f1e808f9143ff6a4c4024fe9ce5ee3bc93aa3a284c432d2a8d956d","first_computed_at":"2026-05-18T04:26:55.550278Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:26:55.550278Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"tCjEF21yTPHFicuOe8rS3G6j84Zas+2+PAn+SdowMZXCfAaPDPtePgFR6xVaUMk8WCIgl5jXNsjCUjDHjqspBA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:26:55.550646Z","signed_message":"canonical_sha256_bytes"},"source_id":"1010.1903","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8a7738058caeb5c806d1738fa8ea0092a227a86351342a0c524b6689389bd66f","sha256:fc913c3bd4f9f6ad4485cd7bbd076492f921977bb25d67258a905d3ec53e7bf5"],"state_sha256":"f4673bc4f69aa6fd13563bab724c29e1aeb484a51d88076499837e11160bfd8c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UJR+nrk/RRzmTckYEYbZBpk9vvzLgeBRx4/OLajsZcpw2V53TYoX2NTqlE8mouPFH1mv+GMLLzsi7zFpy5WBDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T20:03:14.143068Z","bundle_sha256":"c28e18bec1e812506335880dc907ec34852f11e9b851572fac5fc8f43aa621be"}}