{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:NHI2I2NRAOGBIGZ5ANCICQF4O6","short_pith_number":"pith:NHI2I2NR","canonical_record":{"source":{"id":"1310.4548","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2013-10-16T23:55:53Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"738106f309f47ad1cf51cc92c4dc1ce54260c30389d68aaae5d7064bfe2b45ca","abstract_canon_sha256":"80aedee0967a9691a707ad929f77851a0e0441017b2f4913a6d2c4164d58fb50"},"schema_version":"1.0"},"canonical_sha256":"69d1a469b1038c141b3d03448140bc77a581597ff5de424c8fd0020d9d7e8cca","source":{"kind":"arxiv","id":"1310.4548","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1310.4548","created_at":"2026-05-18T02:41:01Z"},{"alias_kind":"arxiv_version","alias_value":"1310.4548v3","created_at":"2026-05-18T02:41:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.4548","created_at":"2026-05-18T02:41:01Z"},{"alias_kind":"pith_short_12","alias_value":"NHI2I2NRAOGB","created_at":"2026-05-18T12:27:52Z"},{"alias_kind":"pith_short_16","alias_value":"NHI2I2NRAOGBIGZ5","created_at":"2026-05-18T12:27:52Z"},{"alias_kind":"pith_short_8","alias_value":"NHI2I2NR","created_at":"2026-05-18T12:27:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:NHI2I2NRAOGBIGZ5ANCICQF4O6","target":"record","payload":{"canonical_record":{"source":{"id":"1310.4548","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2013-10-16T23:55:53Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"738106f309f47ad1cf51cc92c4dc1ce54260c30389d68aaae5d7064bfe2b45ca","abstract_canon_sha256":"80aedee0967a9691a707ad929f77851a0e0441017b2f4913a6d2c4164d58fb50"},"schema_version":"1.0"},"canonical_sha256":"69d1a469b1038c141b3d03448140bc77a581597ff5de424c8fd0020d9d7e8cca","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:41:01.177672Z","signature_b64":"gF7sxTtwcFCabBbe5E+Q0Wwcvs4M0EUCXVqA6kK40HW441ts7n0qj8v6LnFkUbP/Jc64ZXstpZFpGO675yzQDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"69d1a469b1038c141b3d03448140bc77a581597ff5de424c8fd0020d9d7e8cca","last_reissued_at":"2026-05-18T02:41:01.177175Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:41:01.177175Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1310.4548","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:41:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/iyvnql6eZwWLdcFiBSbBP044yfg3EMkGjRrv5W94b1RQk6EMExHKc5GGooMtE4xDj+O9IMkFkss/mWrKONqDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T08:39:15.513269Z"},"content_sha256":"29306ef32fe5bea1395748b0986ca4413fea696c8d682c8ae3d056cc36150b8a","schema_version":"1.0","event_id":"sha256:29306ef32fe5bea1395748b0986ca4413fea696c8d682c8ae3d056cc36150b8a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:NHI2I2NRAOGBIGZ5ANCICQF4O6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Supersolid phases of light in extended Jaynes-Cummings-Hubbard systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.other","authors_text":"Andrew L.C. Hayward, Andy M. Martin, Bogusz Bujnowski, Jared H. Cole, Justine K. Corso","submitted_at":"2013-10-16T23:55:53Z","abstract_excerpt":"Jaynes-Cummings-Hubbard lattices provide unique properties for the study of correlated phases as they exhibit convenient state preparation and measurement, as well as \"in situ\" tuning of parameters. We show how to realize charge density and supersolid phases in Jaynes-Cummings-Hubbard lattices in the presence of long-range interactions. The long-range interactions are realized by the consideration of Rydberg states in coupled atom-cavity systems and the introduction of additional capacitive couplings in quantum-electrodynamics circuits. We demonstrate the emergence of supersolid and checkerboa"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.4548","kind":"arxiv","version":3},"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":"2026-05-18T02:41:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CyEoCppTTttCFrJMj1gV42prv6pRjTNULq3UMBbURf89U02B/bMZmliUdMU3khSowoN+tkyGohbYt8kQXjQzBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T08:39:15.513638Z"},"content_sha256":"e2da711f7db2e757e76ae1bbc2803394951975c4009a1a1463e736365aa92147","schema_version":"1.0","event_id":"sha256:e2da711f7db2e757e76ae1bbc2803394951975c4009a1a1463e736365aa92147"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/NHI2I2NRAOGBIGZ5ANCICQF4O6/bundle.json","state_url":"https://pith.science/pith/NHI2I2NRAOGBIGZ5ANCICQF4O6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/NHI2I2NRAOGBIGZ5ANCICQF4O6/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":"2026-06-01T08:39:15Z","links":{"resolver":"https://pith.science/pith/NHI2I2NRAOGBIGZ5ANCICQF4O6","bundle":"https://pith.science/pith/NHI2I2NRAOGBIGZ5ANCICQF4O6/bundle.json","state":"https://pith.science/pith/NHI2I2NRAOGBIGZ5ANCICQF4O6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/NHI2I2NRAOGBIGZ5ANCICQF4O6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:NHI2I2NRAOGBIGZ5ANCICQF4O6","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":"80aedee0967a9691a707ad929f77851a0e0441017b2f4913a6d2c4164d58fb50","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2013-10-16T23:55:53Z","title_canon_sha256":"738106f309f47ad1cf51cc92c4dc1ce54260c30389d68aaae5d7064bfe2b45ca"},"schema_version":"1.0","source":{"id":"1310.4548","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1310.4548","created_at":"2026-05-18T02:41:01Z"},{"alias_kind":"arxiv_version","alias_value":"1310.4548v3","created_at":"2026-05-18T02:41:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.4548","created_at":"2026-05-18T02:41:01Z"},{"alias_kind":"pith_short_12","alias_value":"NHI2I2NRAOGB","created_at":"2026-05-18T12:27:52Z"},{"alias_kind":"pith_short_16","alias_value":"NHI2I2NRAOGBIGZ5","created_at":"2026-05-18T12:27:52Z"},{"alias_kind":"pith_short_8","alias_value":"NHI2I2NR","created_at":"2026-05-18T12:27:52Z"}],"graph_snapshots":[{"event_id":"sha256:e2da711f7db2e757e76ae1bbc2803394951975c4009a1a1463e736365aa92147","target":"graph","created_at":"2026-05-18T02:41:01Z","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":"Jaynes-Cummings-Hubbard lattices provide unique properties for the study of correlated phases as they exhibit convenient state preparation and measurement, as well as \"in situ\" tuning of parameters. We show how to realize charge density and supersolid phases in Jaynes-Cummings-Hubbard lattices in the presence of long-range interactions. The long-range interactions are realized by the consideration of Rydberg states in coupled atom-cavity systems and the introduction of additional capacitive couplings in quantum-electrodynamics circuits. We demonstrate the emergence of supersolid and checkerboa","authors_text":"Andrew L.C. Hayward, Andy M. Martin, Bogusz Bujnowski, Jared H. Cole, Justine K. Corso","cross_cats":["quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2013-10-16T23:55:53Z","title":"Supersolid phases of light in extended Jaynes-Cummings-Hubbard systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.4548","kind":"arxiv","version":3},"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":"sha256:29306ef32fe5bea1395748b0986ca4413fea696c8d682c8ae3d056cc36150b8a","target":"record","created_at":"2026-05-18T02:41:01Z","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":"80aedee0967a9691a707ad929f77851a0e0441017b2f4913a6d2c4164d58fb50","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.other","submitted_at":"2013-10-16T23:55:53Z","title_canon_sha256":"738106f309f47ad1cf51cc92c4dc1ce54260c30389d68aaae5d7064bfe2b45ca"},"schema_version":"1.0","source":{"id":"1310.4548","kind":"arxiv","version":3}},"canonical_sha256":"69d1a469b1038c141b3d03448140bc77a581597ff5de424c8fd0020d9d7e8cca","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"69d1a469b1038c141b3d03448140bc77a581597ff5de424c8fd0020d9d7e8cca","first_computed_at":"2026-05-18T02:41:01.177175Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:41:01.177175Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"gF7sxTtwcFCabBbe5E+Q0Wwcvs4M0EUCXVqA6kK40HW441ts7n0qj8v6LnFkUbP/Jc64ZXstpZFpGO675yzQDA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:41:01.177672Z","signed_message":"canonical_sha256_bytes"},"source_id":"1310.4548","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:29306ef32fe5bea1395748b0986ca4413fea696c8d682c8ae3d056cc36150b8a","sha256:e2da711f7db2e757e76ae1bbc2803394951975c4009a1a1463e736365aa92147"],"state_sha256":"7d4248ffd6951f8c0b10367c3b5d735de3c9d030b048a6a99302bea13940fc9d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/iMeh4zo5+jagTBDy0XlJCDhMilRo0AUPvJEcDwI/aQvZ93EOxCEFBa2oIrP3GNWp0Gimfgs9fKJCD6NAr57Aw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T08:39:15.515644Z","bundle_sha256":"9630ead55901ebe9d0fa0b1eead4411e91bb4ef74423ae9bedd4ae4329fbc936"}}