{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2009:PB4RYRR4G75B6Q3K25TLZW5UFA","short_pith_number":"pith:PB4RYRR4","canonical_record":{"source":{"id":"0908.1717","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2009-08-12T14:11:54Z","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.other"],"title_canon_sha256":"45429cbd0bad94f989ac50d620aec262b8b2842f2a04df319bf56cff41c6c712","abstract_canon_sha256":"62113cd2a5f488c8e59a49682ba72c043e5ab8bb4364413b3ed695ada89c2d30"},"schema_version":"1.0"},"canonical_sha256":"78791c463c37fa1f436ad766bcdbb428102d4b180af0e4550ecab346be7b9cab","source":{"kind":"arxiv","id":"0908.1717","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0908.1717","created_at":"2026-05-18T04:40:00Z"},{"alias_kind":"arxiv_version","alias_value":"0908.1717v1","created_at":"2026-05-18T04:40:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0908.1717","created_at":"2026-05-18T04:40:00Z"},{"alias_kind":"pith_short_12","alias_value":"PB4RYRR4G75B","created_at":"2026-05-18T12:26:01Z"},{"alias_kind":"pith_short_16","alias_value":"PB4RYRR4G75B6Q3K","created_at":"2026-05-18T12:26:01Z"},{"alias_kind":"pith_short_8","alias_value":"PB4RYRR4","created_at":"2026-05-18T12:26:01Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2009:PB4RYRR4G75B6Q3K25TLZW5UFA","target":"record","payload":{"canonical_record":{"source":{"id":"0908.1717","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2009-08-12T14:11:54Z","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.other"],"title_canon_sha256":"45429cbd0bad94f989ac50d620aec262b8b2842f2a04df319bf56cff41c6c712","abstract_canon_sha256":"62113cd2a5f488c8e59a49682ba72c043e5ab8bb4364413b3ed695ada89c2d30"},"schema_version":"1.0"},"canonical_sha256":"78791c463c37fa1f436ad766bcdbb428102d4b180af0e4550ecab346be7b9cab","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:40:00.726233Z","signature_b64":"6smy/meXy4gXQmWK5RXybQA7lbwslIz8hn5b3epSQqCGcDRiV9PtG2eGrn596KgCxGd8V8EvPP33lY4uAojNDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"78791c463c37fa1f436ad766bcdbb428102d4b180af0e4550ecab346be7b9cab","last_reissued_at":"2026-05-18T04:40:00.725707Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:40:00.725707Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0908.1717","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":"2026-05-18T04:40:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JcaMxCvOqMkwnmRHeS0j5JDVLlq3ATr6h9G9nvC17q1nlSfgmXi0gzHPvkwO9bJOw4bhvdsmOw99O17y/RcnCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T01:45:34.006225Z"},"content_sha256":"1b277dd8d5238944e5e6c4f8cc6ffbc36e4f6e2f29fdf7c2f3e161c2f85d96d7","schema_version":"1.0","event_id":"sha256:1b277dd8d5238944e5e6c4f8cc6ffbc36e4f6e2f29fdf7c2f3e161c2f85d96d7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2009:PB4RYRR4G75B6Q3K25TLZW5UFA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Travelling to exotic places with cavity QED systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","cond-mat.other"],"primary_cat":"quant-ph","authors_text":"Jonas Larson","submitted_at":"2009-08-12T14:11:54Z","abstract_excerpt":"Recent theoretical schemes for utilizing cavity QED models as quantum simulators are reviewed. By considering a quadrature representation for the fields, it is shown how Jahn-Teller models, effective Abelian or non-Abelian gauge potentials, transverse Hall currents, and relativistic effects naturally arise in these systems. Some of the analytical predictions are verified numerically using realistic experimental parameters taking into account for system losses. Thereby demonstrating their feasibility with current experimental setups."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0908.1717","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":"2026-05-18T04:40:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MS/vF7TD0/lwME2cT92nbT6yxlkfnQ+sl5UyKEFo+UxVlwfnYS7VOXuUNHgScAl7HQ5USC6OUjoRjHbbeH9QBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T01:45:34.007037Z"},"content_sha256":"97b87c3fbcbd9ab3d9b91ed4f68468a2e4050f065e54e81d5123a286a1d26f3b","schema_version":"1.0","event_id":"sha256:97b87c3fbcbd9ab3d9b91ed4f68468a2e4050f065e54e81d5123a286a1d26f3b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PB4RYRR4G75B6Q3K25TLZW5UFA/bundle.json","state_url":"https://pith.science/pith/PB4RYRR4G75B6Q3K25TLZW5UFA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PB4RYRR4G75B6Q3K25TLZW5UFA/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":"2026-06-11T01:45:34Z","links":{"resolver":"https://pith.science/pith/PB4RYRR4G75B6Q3K25TLZW5UFA","bundle":"https://pith.science/pith/PB4RYRR4G75B6Q3K25TLZW5UFA/bundle.json","state":"https://pith.science/pith/PB4RYRR4G75B6Q3K25TLZW5UFA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PB4RYRR4G75B6Q3K25TLZW5UFA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2009:PB4RYRR4G75B6Q3K25TLZW5UFA","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":"62113cd2a5f488c8e59a49682ba72c043e5ab8bb4364413b3ed695ada89c2d30","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.other"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2009-08-12T14:11:54Z","title_canon_sha256":"45429cbd0bad94f989ac50d620aec262b8b2842f2a04df319bf56cff41c6c712"},"schema_version":"1.0","source":{"id":"0908.1717","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0908.1717","created_at":"2026-05-18T04:40:00Z"},{"alias_kind":"arxiv_version","alias_value":"0908.1717v1","created_at":"2026-05-18T04:40:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0908.1717","created_at":"2026-05-18T04:40:00Z"},{"alias_kind":"pith_short_12","alias_value":"PB4RYRR4G75B","created_at":"2026-05-18T12:26:01Z"},{"alias_kind":"pith_short_16","alias_value":"PB4RYRR4G75B6Q3K","created_at":"2026-05-18T12:26:01Z"},{"alias_kind":"pith_short_8","alias_value":"PB4RYRR4","created_at":"2026-05-18T12:26:01Z"}],"graph_snapshots":[{"event_id":"sha256:97b87c3fbcbd9ab3d9b91ed4f68468a2e4050f065e54e81d5123a286a1d26f3b","target":"graph","created_at":"2026-05-18T04:40:00Z","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":"Recent theoretical schemes for utilizing cavity QED models as quantum simulators are reviewed. By considering a quadrature representation for the fields, it is shown how Jahn-Teller models, effective Abelian or non-Abelian gauge potentials, transverse Hall currents, and relativistic effects naturally arise in these systems. Some of the analytical predictions are verified numerically using realistic experimental parameters taking into account for system losses. Thereby demonstrating their feasibility with current experimental setups.","authors_text":"Jonas Larson","cross_cats":["cond-mat.mtrl-sci","cond-mat.other"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2009-08-12T14:11:54Z","title":"Travelling to exotic places with cavity QED systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0908.1717","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":"sha256:1b277dd8d5238944e5e6c4f8cc6ffbc36e4f6e2f29fdf7c2f3e161c2f85d96d7","target":"record","created_at":"2026-05-18T04:40:00Z","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":"62113cd2a5f488c8e59a49682ba72c043e5ab8bb4364413b3ed695ada89c2d30","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.other"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2009-08-12T14:11:54Z","title_canon_sha256":"45429cbd0bad94f989ac50d620aec262b8b2842f2a04df319bf56cff41c6c712"},"schema_version":"1.0","source":{"id":"0908.1717","kind":"arxiv","version":1}},"canonical_sha256":"78791c463c37fa1f436ad766bcdbb428102d4b180af0e4550ecab346be7b9cab","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"78791c463c37fa1f436ad766bcdbb428102d4b180af0e4550ecab346be7b9cab","first_computed_at":"2026-05-18T04:40:00.725707Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:40:00.725707Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"6smy/meXy4gXQmWK5RXybQA7lbwslIz8hn5b3epSQqCGcDRiV9PtG2eGrn596KgCxGd8V8EvPP33lY4uAojNDg==","signature_status":"signed_v1","signed_at":"2026-05-18T04:40:00.726233Z","signed_message":"canonical_sha256_bytes"},"source_id":"0908.1717","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1b277dd8d5238944e5e6c4f8cc6ffbc36e4f6e2f29fdf7c2f3e161c2f85d96d7","sha256:97b87c3fbcbd9ab3d9b91ed4f68468a2e4050f065e54e81d5123a286a1d26f3b"],"state_sha256":"77da0336af70325f42cb56804194e6ab900dee7dcc1a98475e36fbdc1e57fffa"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7r3C7JG4VkW4SnTL0+tiS3k7Y45VGS9Yj5aGGmvHiFgxXLqGhthU6NJYMZ/3tFkdsaCR1gwulrqVjcgY6zM8AA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-11T01:45:34.011743Z","bundle_sha256":"57a5f0e0a94e8390a27edac119b089924ecc22750b05de9f7d396c1e30556c9f"}}