{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:HVYDWQIYOMUOJRBF5J5LZ6C4AL","short_pith_number":"pith:HVYDWQIY","schema_version":"1.0","canonical_sha256":"3d703b41187328e4c425ea7abcf85c02dcaa0269b8ca16647c1e462a1bc0bbe5","source":{"kind":"arxiv","id":"2607.27028","version":1},"attestation_state":"computed","paper":{"title":"Unconventional Thermalization of a Three-Wave-Mixing Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Evangelos Varvelis, Joachim Ankerhold, Miriam Resch","submitted_at":"2026-07-29T15:23:42Z","abstract_excerpt":"Understanding the boundaries between quantum thermalization and localization in many-body systems remains a central frontier of condensed matter and quantum information science. In this work, we investigate the dynamics and spectral properties of a generic model with long-range three-body-interaction, namely, a system with non-local three-wave-mixing. This model has been realized recently with a microwave Fabry-Perot cavity terminated on one end by a superconducting qubit mirror. Utilizing exact diagonalization techniques, we uncover a striking paradox: the global energy level spacing statisti"},"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":"2607.27028","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2026-07-29T15:23:42Z","cross_cats_sorted":[],"title_canon_sha256":"b214d82c5ba5d73e3cd5a488a9e64ff387b915bf465f1eebeefe7db53a3976d1","abstract_canon_sha256":"dfc23a4929d9235281536c4b6ca09e5fccfb01d477c0243951377627624e079c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3d703b41187328e4c425ea7abcf85c02dcaa0269b8ca16647c1e462a1bc0bbe5","last_reissued_at":"2026-07-30T01:23:22.896326Z","signature_status":"unsigned_v0","first_computed_at":"2026-07-30T01:23:22.896326Z"},"graph_snapshot":{"paper":{"title":"Unconventional Thermalization of a Three-Wave-Mixing Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Evangelos Varvelis, Joachim Ankerhold, Miriam Resch","submitted_at":"2026-07-29T15:23:42Z","abstract_excerpt":"Understanding the boundaries between quantum thermalization and localization in many-body systems remains a central frontier of condensed matter and quantum information science. In this work, we investigate the dynamics and spectral properties of a generic model with long-range three-body-interaction, namely, a system with non-local three-wave-mixing. This model has been realized recently with a microwave Fabry-Perot cavity terminated on one end by a superconducting qubit mirror. Utilizing exact diagonalization techniques, we uncover a striking paradox: the global energy level spacing statisti"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.27028","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2607.27028/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":"2607.27028","created_at":"2026-07-30T01:23:22.901402+00:00"},{"alias_kind":"arxiv_version","alias_value":"2607.27028v1","created_at":"2026-07-30T01:23:22.901402+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.27028","created_at":"2026-07-30T01:23:22.901402+00:00"},{"alias_kind":"pith_short_12","alias_value":"HVYDWQIYOMUO","created_at":"2026-07-30T01:23:22.901402+00:00"},{"alias_kind":"pith_short_16","alias_value":"HVYDWQIYOMUOJRBF","created_at":"2026-07-30T01:23:22.901402+00:00"},{"alias_kind":"pith_short_8","alias_value":"HVYDWQIY","created_at":"2026-07-30T01:23:22.901402+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/HVYDWQIYOMUOJRBF5J5LZ6C4AL","json":"https://pith.science/pith/HVYDWQIYOMUOJRBF5J5LZ6C4AL.json","graph_json":"https://pith.science/api/pith-number/HVYDWQIYOMUOJRBF5J5LZ6C4AL/graph.json","events_json":"https://pith.science/api/pith-number/HVYDWQIYOMUOJRBF5J5LZ6C4AL/events.json","paper":"https://pith.science/paper/HVYDWQIY"},"agent_actions":{"view_html":"https://pith.science/pith/HVYDWQIYOMUOJRBF5J5LZ6C4AL","download_json":"https://pith.science/pith/HVYDWQIYOMUOJRBF5J5LZ6C4AL.json","view_paper":"https://pith.science/paper/HVYDWQIY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2607.27028&json=true","fetch_graph":"https://pith.science/api/pith-number/HVYDWQIYOMUOJRBF5J5LZ6C4AL/graph.json","fetch_events":"https://pith.science/api/pith-number/HVYDWQIYOMUOJRBF5J5LZ6C4AL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HVYDWQIYOMUOJRBF5J5LZ6C4AL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HVYDWQIYOMUOJRBF5J5LZ6C4AL/action/storage_attestation","attest_author":"https://pith.science/pith/HVYDWQIYOMUOJRBF5J5LZ6C4AL/action/author_attestation","sign_citation":"https://pith.science/pith/HVYDWQIYOMUOJRBF5J5LZ6C4AL/action/citation_signature","submit_replication":"https://pith.science/pith/HVYDWQIYOMUOJRBF5J5LZ6C4AL/action/replication_record"}},"created_at":"2026-07-30T01:23:22.901402+00:00","updated_at":"2026-07-30T01:23:22.901402+00:00"}