{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:35PFSCQCQGJR6FPDG6D5XUCAAW","short_pith_number":"pith:35PFSCQC","schema_version":"1.0","canonical_sha256":"df5e590a0281931f15e33787dbd040058a83314ef2905d42e6af33c00234bcc3","source":{"kind":"arxiv","id":"1106.0801","version":2},"attestation_state":"computed","paper":{"title":"Dynamical critical exponent of the Jaynes-Cummings-Hubbard model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.str-el","authors_text":"L. Pollet, M. Aichhorn, M. Hohenadler, S. Schmidt","submitted_at":"2011-06-04T08:15:18Z","abstract_excerpt":"An array of high-Q electromagnetic resonators coupled to qubits gives rise to the Jaynes-Cummings-Hubbard model describing a superfluid to Mott insulator transition of lattice polaritons. From mean-field and strong coupling expansions, the critical properties of the model are expected to be identical to the scalar Bose-Hubbard model. A recent Monte Carlo study of the superfluid density on the square lattice suggested that this does not hold for the fixed-density transition through the Mott lobe tip. Instead, mean-field behavior with a dynamical critical exponent z=2 was found. We perform large"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1106.0801","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-06-04T08:15:18Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"b40d2353fd1fd99c12d98b928981be8295eb08c64ec2a41089a8ce8b41d7289e","abstract_canon_sha256":"24ef8c352fb21d2f48721e6974da92a7fe7d9358d225ab12be14a67344a5fc53"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:10:34.138258Z","signature_b64":"lnlhJzCJDNN9CoTHMrelfc8v6vap0qrJ0qM+RqX/jV5S6fYDK1MDFZL1k86CJBBz1XQmexAsrOW0K8uTfF8kCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"df5e590a0281931f15e33787dbd040058a83314ef2905d42e6af33c00234bcc3","last_reissued_at":"2026-05-18T04:10:34.137453Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:10:34.137453Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dynamical critical exponent of the Jaynes-Cummings-Hubbard model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.str-el","authors_text":"L. Pollet, M. Aichhorn, M. Hohenadler, S. Schmidt","submitted_at":"2011-06-04T08:15:18Z","abstract_excerpt":"An array of high-Q electromagnetic resonators coupled to qubits gives rise to the Jaynes-Cummings-Hubbard model describing a superfluid to Mott insulator transition of lattice polaritons. From mean-field and strong coupling expansions, the critical properties of the model are expected to be identical to the scalar Bose-Hubbard model. A recent Monte Carlo study of the superfluid density on the square lattice suggested that this does not hold for the fixed-density transition through the Mott lobe tip. Instead, mean-field behavior with a dynamical critical exponent z=2 was found. We perform large"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.0801","kind":"arxiv","version":2},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1106.0801","created_at":"2026-05-18T04:10:34.137611+00:00"},{"alias_kind":"arxiv_version","alias_value":"1106.0801v2","created_at":"2026-05-18T04:10:34.137611+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.0801","created_at":"2026-05-18T04:10:34.137611+00:00"},{"alias_kind":"pith_short_12","alias_value":"35PFSCQCQGJR","created_at":"2026-05-18T12:26:18.847500+00:00"},{"alias_kind":"pith_short_16","alias_value":"35PFSCQCQGJR6FPD","created_at":"2026-05-18T12:26:18.847500+00:00"},{"alias_kind":"pith_short_8","alias_value":"35PFSCQC","created_at":"2026-05-18T12:26:18.847500+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/35PFSCQCQGJR6FPDG6D5XUCAAW","json":"https://pith.science/pith/35PFSCQCQGJR6FPDG6D5XUCAAW.json","graph_json":"https://pith.science/api/pith-number/35PFSCQCQGJR6FPDG6D5XUCAAW/graph.json","events_json":"https://pith.science/api/pith-number/35PFSCQCQGJR6FPDG6D5XUCAAW/events.json","paper":"https://pith.science/paper/35PFSCQC"},"agent_actions":{"view_html":"https://pith.science/pith/35PFSCQCQGJR6FPDG6D5XUCAAW","download_json":"https://pith.science/pith/35PFSCQCQGJR6FPDG6D5XUCAAW.json","view_paper":"https://pith.science/paper/35PFSCQC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1106.0801&json=true","fetch_graph":"https://pith.science/api/pith-number/35PFSCQCQGJR6FPDG6D5XUCAAW/graph.json","fetch_events":"https://pith.science/api/pith-number/35PFSCQCQGJR6FPDG6D5XUCAAW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/35PFSCQCQGJR6FPDG6D5XUCAAW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/35PFSCQCQGJR6FPDG6D5XUCAAW/action/storage_attestation","attest_author":"https://pith.science/pith/35PFSCQCQGJR6FPDG6D5XUCAAW/action/author_attestation","sign_citation":"https://pith.science/pith/35PFSCQCQGJR6FPDG6D5XUCAAW/action/citation_signature","submit_replication":"https://pith.science/pith/35PFSCQCQGJR6FPDG6D5XUCAAW/action/replication_record"}},"created_at":"2026-05-18T04:10:34.137611+00:00","updated_at":"2026-05-18T04:10:34.137611+00:00"}