{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:AXSWY6NAPRGXHHXRNY7LMT7PSK","short_pith_number":"pith:AXSWY6NA","canonical_record":{"source":{"id":"1309.7339","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2013-09-27T19:38:19Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"0d2fd63e1fd40c4bc3d66651f261d344c1027fdadd38d0807b7e68e613d2dc5a","abstract_canon_sha256":"0ffe9f77cd59634b05fd409ae65e1e7a67374ab86c9f5c09694f530e296bdb4f"},"schema_version":"1.0"},"canonical_sha256":"05e56c79a07c4d739ef16e3eb64fef92925e039ddea3701b5b95d08a9724a60a","source":{"kind":"arxiv","id":"1309.7339","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1309.7339","created_at":"2026-05-18T03:07:22Z"},{"alias_kind":"arxiv_version","alias_value":"1309.7339v1","created_at":"2026-05-18T03:07:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1309.7339","created_at":"2026-05-18T03:07:22Z"},{"alias_kind":"pith_short_12","alias_value":"AXSWY6NAPRGX","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_16","alias_value":"AXSWY6NAPRGXHHXR","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_8","alias_value":"AXSWY6NA","created_at":"2026-05-18T12:27:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:AXSWY6NAPRGXHHXRNY7LMT7PSK","target":"record","payload":{"canonical_record":{"source":{"id":"1309.7339","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2013-09-27T19:38:19Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"0d2fd63e1fd40c4bc3d66651f261d344c1027fdadd38d0807b7e68e613d2dc5a","abstract_canon_sha256":"0ffe9f77cd59634b05fd409ae65e1e7a67374ab86c9f5c09694f530e296bdb4f"},"schema_version":"1.0"},"canonical_sha256":"05e56c79a07c4d739ef16e3eb64fef92925e039ddea3701b5b95d08a9724a60a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:07:22.579921Z","signature_b64":"Xukdkix2oKiNvNQjMoKEHcJR3qB1hvjKLByI6m0/DPrSD/FMbKSElv6adk8djUAdA5ketGwNGshofSsHjKyMDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"05e56c79a07c4d739ef16e3eb64fef92925e039ddea3701b5b95d08a9724a60a","last_reissued_at":"2026-05-18T03:07:22.579116Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:07:22.579116Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1309.7339","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":"2026-05-18T03:07:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0FPWX7STeCmyValMcC4vm3E+WR0YkVRg9u1lXf/6EaCx5KLE6+SerLFMow34qxPB1nWiM++mY1LXE7s2BQDSAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T10:00:35.320962Z"},"content_sha256":"4a07403c5af8cf833ca88ee94de65c0d725f216a4f313dc3986aded2e76c81e8","schema_version":"1.0","event_id":"sha256:4a07403c5af8cf833ca88ee94de65c0d725f216a4f313dc3986aded2e76c81e8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:AXSWY6NAPRGXHHXRNY7LMT7PSK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quantum Phase Transition of Light in the Rabi-Hubbard Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.other","authors_text":"B. \\\"Oztop, H. E. T\\\"ureci, M. Bordyuh, M. Schir\\'o","submitted_at":"2013-09-27T19:38:19Z","abstract_excerpt":"We discuss the physics of the Rabi-Hubbard model describing large arrays of coupled cavities interacting with two level atoms via a Rabi non-linearity. We show that the inclusion of counter-rotating terms in the light-matter interaction, often neglected in theoretical descriptions based on Jaynes-Cumming models, is crucial to stabilize finite-density quantum phases of correlated photons with no need for an artificially engineered chemical potential. We show that the physical properties of these phases and the quantum phase transition occurring between them is remarkably different from those of"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1309.7339","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":"2026-05-18T03:07:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Odgk/Q15rl4Fm2vTCWnf7oA0t5BJ3/jVIIcQtGQETl9dZZmCAEAJ+0DnCsa6QKa7vyKnM+7HxfDDjcDRod9rBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T10:00:35.321304Z"},"content_sha256":"24ae69e0bfaf47b73ec35dc5a981f51989d10fcfd1b55e4cf88d1cbbc96384f6","schema_version":"1.0","event_id":"sha256:24ae69e0bfaf47b73ec35dc5a981f51989d10fcfd1b55e4cf88d1cbbc96384f6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/AXSWY6NAPRGXHHXRNY7LMT7PSK/bundle.json","state_url":"https://pith.science/pith/AXSWY6NAPRGXHHXRNY7LMT7PSK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/AXSWY6NAPRGXHHXRNY7LMT7PSK/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":"2026-06-02T10:00:35Z","links":{"resolver":"https://pith.science/pith/AXSWY6NAPRGXHHXRNY7LMT7PSK","bundle":"https://pith.science/pith/AXSWY6NAPRGXHHXRNY7LMT7PSK/bundle.json","state":"https://pith.science/pith/AXSWY6NAPRGXHHXRNY7LMT7PSK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/AXSWY6NAPRGXHHXRNY7LMT7PSK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:AXSWY6NAPRGXHHXRNY7LMT7PSK","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":"0ffe9f77cd59634b05fd409ae65e1e7a67374ab86c9f5c09694f530e296bdb4f","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2013-09-27T19:38:19Z","title_canon_sha256":"0d2fd63e1fd40c4bc3d66651f261d344c1027fdadd38d0807b7e68e613d2dc5a"},"schema_version":"1.0","source":{"id":"1309.7339","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1309.7339","created_at":"2026-05-18T03:07:22Z"},{"alias_kind":"arxiv_version","alias_value":"1309.7339v1","created_at":"2026-05-18T03:07:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1309.7339","created_at":"2026-05-18T03:07:22Z"},{"alias_kind":"pith_short_12","alias_value":"AXSWY6NAPRGX","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_16","alias_value":"AXSWY6NAPRGXHHXR","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_8","alias_value":"AXSWY6NA","created_at":"2026-05-18T12:27:38Z"}],"graph_snapshots":[{"event_id":"sha256:24ae69e0bfaf47b73ec35dc5a981f51989d10fcfd1b55e4cf88d1cbbc96384f6","target":"graph","created_at":"2026-05-18T03:07:22Z","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 discuss the physics of the Rabi-Hubbard model describing large arrays of coupled cavities interacting with two level atoms via a Rabi non-linearity. We show that the inclusion of counter-rotating terms in the light-matter interaction, often neglected in theoretical descriptions based on Jaynes-Cumming models, is crucial to stabilize finite-density quantum phases of correlated photons with no need for an artificially engineered chemical potential. We show that the physical properties of these phases and the quantum phase transition occurring between them is remarkably different from those of","authors_text":"B. \\\"Oztop, H. E. T\\\"ureci, M. Bordyuh, M. Schir\\'o","cross_cats":["cond-mat.mes-hall"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2013-09-27T19:38:19Z","title":"Quantum Phase Transition of Light in the Rabi-Hubbard Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1309.7339","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":"sha256:4a07403c5af8cf833ca88ee94de65c0d725f216a4f313dc3986aded2e76c81e8","target":"record","created_at":"2026-05-18T03:07:22Z","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":"0ffe9f77cd59634b05fd409ae65e1e7a67374ab86c9f5c09694f530e296bdb4f","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2013-09-27T19:38:19Z","title_canon_sha256":"0d2fd63e1fd40c4bc3d66651f261d344c1027fdadd38d0807b7e68e613d2dc5a"},"schema_version":"1.0","source":{"id":"1309.7339","kind":"arxiv","version":1}},"canonical_sha256":"05e56c79a07c4d739ef16e3eb64fef92925e039ddea3701b5b95d08a9724a60a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"05e56c79a07c4d739ef16e3eb64fef92925e039ddea3701b5b95d08a9724a60a","first_computed_at":"2026-05-18T03:07:22.579116Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:07:22.579116Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Xukdkix2oKiNvNQjMoKEHcJR3qB1hvjKLByI6m0/DPrSD/FMbKSElv6adk8djUAdA5ketGwNGshofSsHjKyMDA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:07:22.579921Z","signed_message":"canonical_sha256_bytes"},"source_id":"1309.7339","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4a07403c5af8cf833ca88ee94de65c0d725f216a4f313dc3986aded2e76c81e8","sha256:24ae69e0bfaf47b73ec35dc5a981f51989d10fcfd1b55e4cf88d1cbbc96384f6"],"state_sha256":"fb1b86eb03a0eacdc0e6e4d57c5a94fd16eecea89cafbd3cd71ab97ab4778076"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AxjiBjZA+HNP94ihGl7hCiUduCivvKIwHDgygVJhgfzi0Eywis6hcNvl6Txzu2EqswhYcuiEjb/Dm0JL7lhMDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T10:00:35.323251Z","bundle_sha256":"90b44ccb4edcffa8a2274a9ddaaafdd70578b74470e71d1a82faabcff834cdbd"}}