{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:JAADEZDS5YJCIUPJZLR4IYTUQL","short_pith_number":"pith:JAADEZDS","schema_version":"1.0","canonical_sha256":"4800326472ee122451e9cae3c4627482f4ad65159edd39e59a363f22a1b84e0a","source":{"kind":"arxiv","id":"quant-ph/0106082","version":3},"attestation_state":"computed","paper":{"title":"Entanglement and quantal coherence: a study of two limiting cases of rapid system--bath interactions","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"quant-ph","authors_text":"Nicole F. Bell, Raymond R. Volkas, R. F. Sawyer","submitted_at":"2001-06-15T02:28:00Z","abstract_excerpt":"We consider the dynamics of a system coupled to a thermal bath, going beyond the standard two-level system through the addition of an energy excitation degree of freedom. Further extensions are to systems containing many fermions, with the master equations modified to take Fermi-Dirac statistics into account, and to potentials with a time-dependent bias that induce resonant avoided crossing transitions. The limit $Q \\to \\infty$, where the interaction rate with the bath is much greater than all free oscillation rates for the system, is interrogated. Two behaviors are possible: freezing (quantum"},"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":"quant-ph/0106082","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"quant-ph","submitted_at":"2001-06-15T02:28:00Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"ef2acdb8a54460a5be566e428063867533a1d205ca977d04fdcdc992e81a85d9","abstract_canon_sha256":"9c395a23d15fedbeff12f5421d721b4a80a07e8963dab72321bb9974b1aa158c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:16:20.975824Z","signature_b64":"7xlC+xEoZSQnOUf3kzFYKcSuWVwDbjsUtMQVCC0HiymPPj6nRSku5m4T09MH3CxGyAjwvU2vBDTsVi7mMzchBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4800326472ee122451e9cae3c4627482f4ad65159edd39e59a363f22a1b84e0a","last_reissued_at":"2026-05-18T04:16:20.975103Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:16:20.975103Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Entanglement and quantal coherence: a study of two limiting cases of rapid system--bath interactions","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"quant-ph","authors_text":"Nicole F. Bell, Raymond R. Volkas, R. F. Sawyer","submitted_at":"2001-06-15T02:28:00Z","abstract_excerpt":"We consider the dynamics of a system coupled to a thermal bath, going beyond the standard two-level system through the addition of an energy excitation degree of freedom. Further extensions are to systems containing many fermions, with the master equations modified to take Fermi-Dirac statistics into account, and to potentials with a time-dependent bias that induce resonant avoided crossing transitions. The limit $Q \\to \\infty$, where the interaction rate with the bath is much greater than all free oscillation rates for the system, is interrogated. Two behaviors are possible: freezing (quantum"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"quant-ph/0106082","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"quant-ph/0106082","created_at":"2026-05-18T04:16:20.975221+00:00"},{"alias_kind":"arxiv_version","alias_value":"quant-ph/0106082v3","created_at":"2026-05-18T04:16:20.975221+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.quant-ph/0106082","created_at":"2026-05-18T04:16:20.975221+00:00"},{"alias_kind":"pith_short_12","alias_value":"JAADEZDS5YJC","created_at":"2026-05-18T12:25:50.254431+00:00"},{"alias_kind":"pith_short_16","alias_value":"JAADEZDS5YJCIUPJ","created_at":"2026-05-18T12:25:50.254431+00:00"},{"alias_kind":"pith_short_8","alias_value":"JAADEZDS","created_at":"2026-05-18T12:25:50.254431+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/JAADEZDS5YJCIUPJZLR4IYTUQL","json":"https://pith.science/pith/JAADEZDS5YJCIUPJZLR4IYTUQL.json","graph_json":"https://pith.science/api/pith-number/JAADEZDS5YJCIUPJZLR4IYTUQL/graph.json","events_json":"https://pith.science/api/pith-number/JAADEZDS5YJCIUPJZLR4IYTUQL/events.json","paper":"https://pith.science/paper/JAADEZDS"},"agent_actions":{"view_html":"https://pith.science/pith/JAADEZDS5YJCIUPJZLR4IYTUQL","download_json":"https://pith.science/pith/JAADEZDS5YJCIUPJZLR4IYTUQL.json","view_paper":"https://pith.science/paper/JAADEZDS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=quant-ph/0106082&json=true","fetch_graph":"https://pith.science/api/pith-number/JAADEZDS5YJCIUPJZLR4IYTUQL/graph.json","fetch_events":"https://pith.science/api/pith-number/JAADEZDS5YJCIUPJZLR4IYTUQL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JAADEZDS5YJCIUPJZLR4IYTUQL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JAADEZDS5YJCIUPJZLR4IYTUQL/action/storage_attestation","attest_author":"https://pith.science/pith/JAADEZDS5YJCIUPJZLR4IYTUQL/action/author_attestation","sign_citation":"https://pith.science/pith/JAADEZDS5YJCIUPJZLR4IYTUQL/action/citation_signature","submit_replication":"https://pith.science/pith/JAADEZDS5YJCIUPJZLR4IYTUQL/action/replication_record"}},"created_at":"2026-05-18T04:16:20.975221+00:00","updated_at":"2026-05-18T04:16:20.975221+00:00"}