{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:AOSX2BOHLI6V6BNIIZY2T4YSZW","short_pith_number":"pith:AOSX2BOH","schema_version":"1.0","canonical_sha256":"03a57d05c75a3d5f05a84671a9f312cdb959f33a77356faec217bd9df57d59bd","source":{"kind":"arxiv","id":"1310.0694","version":1},"attestation_state":"computed","paper":{"title":"Elimination of the A-square problem from cavity QED","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Andr\\'as Vukics, Peter Domokos, Tobias Grie{\\ss}er","submitted_at":"2013-10-02T13:12:04Z","abstract_excerpt":"We generalize the Power-Zineau-Woolley transformation to obtain a canonical Hamiltonian of cavity quantum electrodynamics for arbitrary geometry of boundaries. This Hamiltonian is free from the A-square term and the instantaneous Coulomb interaction between distinct atoms. The single-mode models of cavity QED (Dicke, Tavis-Cummings, Jaynes-Cummings) are justified by a term by term mapping to the proposed microscopic Hamiltonian. As one straightforward consequence, the basis of no-go argumentations concerning the Dicke phase transition with atoms in electromagnetic fields dissolves."},"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":"1310.0694","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-10-02T13:12:04Z","cross_cats_sorted":[],"title_canon_sha256":"40f92a602686df47a115c68667944567474417629843e146530e9d7a523c3ab0","abstract_canon_sha256":"56148298431bf42d1491675e2756857b98020db12960321d05fbeb289821e961"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:58:21.640159Z","signature_b64":"FmHIIedgOPenlUjZV7bfxn3IJtpk6KK9ak6ztBY63eDrb1CvyVf9sItF2TTw4SLX9QrJ0HTjazbnwE4O/bURCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"03a57d05c75a3d5f05a84671a9f312cdb959f33a77356faec217bd9df57d59bd","last_reissued_at":"2026-05-18T02:58:21.639601Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:58:21.639601Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Elimination of the A-square problem from cavity QED","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Andr\\'as Vukics, Peter Domokos, Tobias Grie{\\ss}er","submitted_at":"2013-10-02T13:12:04Z","abstract_excerpt":"We generalize the Power-Zineau-Woolley transformation to obtain a canonical Hamiltonian of cavity quantum electrodynamics for arbitrary geometry of boundaries. This Hamiltonian is free from the A-square term and the instantaneous Coulomb interaction between distinct atoms. The single-mode models of cavity QED (Dicke, Tavis-Cummings, Jaynes-Cummings) are justified by a term by term mapping to the proposed microscopic Hamiltonian. As one straightforward consequence, the basis of no-go argumentations concerning the Dicke phase transition with atoms in electromagnetic fields dissolves."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.0694","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1310.0694","created_at":"2026-05-18T02:58:21.639685+00:00"},{"alias_kind":"arxiv_version","alias_value":"1310.0694v1","created_at":"2026-05-18T02:58:21.639685+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.0694","created_at":"2026-05-18T02:58:21.639685+00:00"},{"alias_kind":"pith_short_12","alias_value":"AOSX2BOHLI6V","created_at":"2026-05-18T12:27:38.830355+00:00"},{"alias_kind":"pith_short_16","alias_value":"AOSX2BOHLI6V6BNI","created_at":"2026-05-18T12:27:38.830355+00:00"},{"alias_kind":"pith_short_8","alias_value":"AOSX2BOH","created_at":"2026-05-18T12:27:38.830355+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/AOSX2BOHLI6V6BNIIZY2T4YSZW","json":"https://pith.science/pith/AOSX2BOHLI6V6BNIIZY2T4YSZW.json","graph_json":"https://pith.science/api/pith-number/AOSX2BOHLI6V6BNIIZY2T4YSZW/graph.json","events_json":"https://pith.science/api/pith-number/AOSX2BOHLI6V6BNIIZY2T4YSZW/events.json","paper":"https://pith.science/paper/AOSX2BOH"},"agent_actions":{"view_html":"https://pith.science/pith/AOSX2BOHLI6V6BNIIZY2T4YSZW","download_json":"https://pith.science/pith/AOSX2BOHLI6V6BNIIZY2T4YSZW.json","view_paper":"https://pith.science/paper/AOSX2BOH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1310.0694&json=true","fetch_graph":"https://pith.science/api/pith-number/AOSX2BOHLI6V6BNIIZY2T4YSZW/graph.json","fetch_events":"https://pith.science/api/pith-number/AOSX2BOHLI6V6BNIIZY2T4YSZW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AOSX2BOHLI6V6BNIIZY2T4YSZW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AOSX2BOHLI6V6BNIIZY2T4YSZW/action/storage_attestation","attest_author":"https://pith.science/pith/AOSX2BOHLI6V6BNIIZY2T4YSZW/action/author_attestation","sign_citation":"https://pith.science/pith/AOSX2BOHLI6V6BNIIZY2T4YSZW/action/citation_signature","submit_replication":"https://pith.science/pith/AOSX2BOHLI6V6BNIIZY2T4YSZW/action/replication_record"}},"created_at":"2026-05-18T02:58:21.639685+00:00","updated_at":"2026-05-18T02:58:21.639685+00:00"}