{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:5TM2XA4EWGRMP653UPMXSLFGUK","short_pith_number":"pith:5TM2XA4E","schema_version":"1.0","canonical_sha256":"ecd9ab8384b1a2c7fbbba3d9792ca6a2823471677cc1f8cc765ffa5873da80fa","source":{"kind":"arxiv","id":"2007.01422","version":3},"attestation_state":"computed","paper":{"title":"Driven-dissipative phase transition in a Kerr oscillator: From semiclassical $\\mathcal{PT}$ symmetry to quantum fluctuations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"quant-ph","authors_text":"Harold U. Baranger, Xin H. H. Zhang","submitted_at":"2020-07-02T22:39:35Z","abstract_excerpt":"We study a minimal model that has a driven-dissipative quantum phase transition, namely a Kerr non-linear oscillator subject to driving and dissipation. Using mean-field theory, exact diagonalization, and the Keldysh formalism, we analyze the critical phenomena in this system, showing which aspects can be captured by each approach and how the approaches complement each other. Then critical scaling and finite-size scaling are calculated analytically using the quantum Langevin equation. The physics contained in this simple model is surprisingly rich: it includes a continuous phase transition, $Z"},"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":"2007.01422","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2020-07-02T22:39:35Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"ecb57434482ef16ca96effd71be06c4dd5a6fc8e2f9bf8b595ca1718f1fe909b","abstract_canon_sha256":"f95d1cd4cb0f0b31b2398e50e562a341e54aa5a7f4e46afcd6822d86cca173ea"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:26:12.929492Z","signature_b64":"N2uMGISHGg2LeEWIQ0cFEMd2ljW0uaDSUFWzw13AfdW/HNcW6eRkuuaRUSoyTcLQ0PYNMSMrY+Fz5rOdRxLSDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ecd9ab8384b1a2c7fbbba3d9792ca6a2823471677cc1f8cc765ffa5873da80fa","last_reissued_at":"2026-07-05T02:26:12.929024Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:26:12.929024Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Driven-dissipative phase transition in a Kerr oscillator: From semiclassical $\\mathcal{PT}$ symmetry to quantum fluctuations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"quant-ph","authors_text":"Harold U. Baranger, Xin H. H. Zhang","submitted_at":"2020-07-02T22:39:35Z","abstract_excerpt":"We study a minimal model that has a driven-dissipative quantum phase transition, namely a Kerr non-linear oscillator subject to driving and dissipation. Using mean-field theory, exact diagonalization, and the Keldysh formalism, we analyze the critical phenomena in this system, showing which aspects can be captured by each approach and how the approaches complement each other. Then critical scaling and finite-size scaling are calculated analytically using the quantum Langevin equation. The physics contained in this simple model is surprisingly rich: it includes a continuous phase transition, $Z"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2007.01422","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2007.01422/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2007.01422","created_at":"2026-07-05T02:26:12.929079+00:00"},{"alias_kind":"arxiv_version","alias_value":"2007.01422v3","created_at":"2026-07-05T02:26:12.929079+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2007.01422","created_at":"2026-07-05T02:26:12.929079+00:00"},{"alias_kind":"pith_short_12","alias_value":"5TM2XA4EWGRM","created_at":"2026-07-05T02:26:12.929079+00:00"},{"alias_kind":"pith_short_16","alias_value":"5TM2XA4EWGRMP653","created_at":"2026-07-05T02:26:12.929079+00:00"},{"alias_kind":"pith_short_8","alias_value":"5TM2XA4E","created_at":"2026-07-05T02:26:12.929079+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2508.20116","citing_title":"Experimental observation of multimode quantum phase transitions in a superconducting Bose-Hubbard simulator","ref_index":60,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5TM2XA4EWGRMP653UPMXSLFGUK","json":"https://pith.science/pith/5TM2XA4EWGRMP653UPMXSLFGUK.json","graph_json":"https://pith.science/api/pith-number/5TM2XA4EWGRMP653UPMXSLFGUK/graph.json","events_json":"https://pith.science/api/pith-number/5TM2XA4EWGRMP653UPMXSLFGUK/events.json","paper":"https://pith.science/paper/5TM2XA4E"},"agent_actions":{"view_html":"https://pith.science/pith/5TM2XA4EWGRMP653UPMXSLFGUK","download_json":"https://pith.science/pith/5TM2XA4EWGRMP653UPMXSLFGUK.json","view_paper":"https://pith.science/paper/5TM2XA4E","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2007.01422&json=true","fetch_graph":"https://pith.science/api/pith-number/5TM2XA4EWGRMP653UPMXSLFGUK/graph.json","fetch_events":"https://pith.science/api/pith-number/5TM2XA4EWGRMP653UPMXSLFGUK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5TM2XA4EWGRMP653UPMXSLFGUK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5TM2XA4EWGRMP653UPMXSLFGUK/action/storage_attestation","attest_author":"https://pith.science/pith/5TM2XA4EWGRMP653UPMXSLFGUK/action/author_attestation","sign_citation":"https://pith.science/pith/5TM2XA4EWGRMP653UPMXSLFGUK/action/citation_signature","submit_replication":"https://pith.science/pith/5TM2XA4EWGRMP653UPMXSLFGUK/action/replication_record"}},"created_at":"2026-07-05T02:26:12.929079+00:00","updated_at":"2026-07-05T02:26:12.929079+00:00"}