{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:CEVD7X3LEBVYPJ4XGZVDVN543Y","short_pith_number":"pith:CEVD7X3L","schema_version":"1.0","canonical_sha256":"112a3fdf6b206b87a797366a3ab7bcde1789ac9c313350f08ed1778803d8b00d","source":{"kind":"arxiv","id":"1704.03918","version":1},"attestation_state":"computed","paper":{"title":"Modelling a Bistable System Strongly Coupled to a Debye Bath: A Quasiclassical Approach Based on the Generalised Langevin Equation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"C.D. Lorenz, H. Ness, L. Kantorovich, L. Stella","submitted_at":"2017-04-12T20:25:27Z","abstract_excerpt":"Bistable systems present two degenerate metastable configurations separated by an energy barrier. Thermal or quantum fluctuations can promote the transition between the configurations at a rate which depends on the dynamical properties of the local environment (i.e., a thermal bath). In the case of classical systems, strong system-bath interaction has been successfully modelled by the Generalised Langevin Equation (GLE) formalism. Here we show that the efficient GLE algorithm introduced in Phys. Rev. B 89, 134303 (2014) can be extended to include some crucial aspects of the quantum fluctuation"},"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":"1704.03918","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-04-12T20:25:27Z","cross_cats_sorted":[],"title_canon_sha256":"17af3dde6beecc8cc17a3d75406e5db129548b9e2e2820c1e70079b9d227ad40","abstract_canon_sha256":"2e0e6a7c4a8f7ecdb8765e2869d1ce3c9bae1696bf24b491522f20efc945b473"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:10:19.470495Z","signature_b64":"TULG/bQn1f36Y/7XzL6Avfeu5CGn+WNujkuGExc+Br15GYLqO+x2w0ZBkB/W1VOgpsXyG2bFH/KzeIXT0pJdDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"112a3fdf6b206b87a797366a3ab7bcde1789ac9c313350f08ed1778803d8b00d","last_reissued_at":"2026-05-18T00:10:19.469987Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:10:19.469987Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Modelling a Bistable System Strongly Coupled to a Debye Bath: A Quasiclassical Approach Based on the Generalised Langevin Equation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"C.D. Lorenz, H. Ness, L. Kantorovich, L. Stella","submitted_at":"2017-04-12T20:25:27Z","abstract_excerpt":"Bistable systems present two degenerate metastable configurations separated by an energy barrier. Thermal or quantum fluctuations can promote the transition between the configurations at a rate which depends on the dynamical properties of the local environment (i.e., a thermal bath). In the case of classical systems, strong system-bath interaction has been successfully modelled by the Generalised Langevin Equation (GLE) formalism. Here we show that the efficient GLE algorithm introduced in Phys. Rev. B 89, 134303 (2014) can be extended to include some crucial aspects of the quantum fluctuation"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.03918","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":"1704.03918","created_at":"2026-05-18T00:10:19.470060+00:00"},{"alias_kind":"arxiv_version","alias_value":"1704.03918v1","created_at":"2026-05-18T00:10:19.470060+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.03918","created_at":"2026-05-18T00:10:19.470060+00:00"},{"alias_kind":"pith_short_12","alias_value":"CEVD7X3LEBVY","created_at":"2026-05-18T12:31:10.602751+00:00"},{"alias_kind":"pith_short_16","alias_value":"CEVD7X3LEBVYPJ4X","created_at":"2026-05-18T12:31:10.602751+00:00"},{"alias_kind":"pith_short_8","alias_value":"CEVD7X3L","created_at":"2026-05-18T12:31:10.602751+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/CEVD7X3LEBVYPJ4XGZVDVN543Y","json":"https://pith.science/pith/CEVD7X3LEBVYPJ4XGZVDVN543Y.json","graph_json":"https://pith.science/api/pith-number/CEVD7X3LEBVYPJ4XGZVDVN543Y/graph.json","events_json":"https://pith.science/api/pith-number/CEVD7X3LEBVYPJ4XGZVDVN543Y/events.json","paper":"https://pith.science/paper/CEVD7X3L"},"agent_actions":{"view_html":"https://pith.science/pith/CEVD7X3LEBVYPJ4XGZVDVN543Y","download_json":"https://pith.science/pith/CEVD7X3LEBVYPJ4XGZVDVN543Y.json","view_paper":"https://pith.science/paper/CEVD7X3L","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1704.03918&json=true","fetch_graph":"https://pith.science/api/pith-number/CEVD7X3LEBVYPJ4XGZVDVN543Y/graph.json","fetch_events":"https://pith.science/api/pith-number/CEVD7X3LEBVYPJ4XGZVDVN543Y/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CEVD7X3LEBVYPJ4XGZVDVN543Y/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CEVD7X3LEBVYPJ4XGZVDVN543Y/action/storage_attestation","attest_author":"https://pith.science/pith/CEVD7X3LEBVYPJ4XGZVDVN543Y/action/author_attestation","sign_citation":"https://pith.science/pith/CEVD7X3LEBVYPJ4XGZVDVN543Y/action/citation_signature","submit_replication":"https://pith.science/pith/CEVD7X3LEBVYPJ4XGZVDVN543Y/action/replication_record"}},"created_at":"2026-05-18T00:10:19.470060+00:00","updated_at":"2026-05-18T00:10:19.470060+00:00"}