{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:4KHFWZGQKES6AISUL4HAAKGOPX","short_pith_number":"pith:4KHFWZGQ","schema_version":"1.0","canonical_sha256":"e28e5b64d05125e022545f0e0028ce7de2640991702573820de96b9af674869c","source":{"kind":"arxiv","id":"1310.3155","version":1},"attestation_state":"computed","paper":{"title":"A Langevin canonical approach to the dynamics of chiral two level systems. Thermal averages and heat capacity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"A. Dorta-Urra, G. Rojas-Lorenzo, H. C. Pe\\~nate-Rodr\\'iguez, P. Bargue\\~no, S. Miret-Art\\'es","submitted_at":"2013-10-11T15:01:30Z","abstract_excerpt":"A Langevin canonical framework for a chiral two--level system coupled to a bath of harmonic oscillators is developed within a coupling scheme different to the well known spin-boson model. Thermal equilibrium values are reached at asymptotic times by solving the corresponding set of non--linear coupled equations in a Markovian regime. In particular, phase difference thermal values (or, equivalently, the so--called coherence factor) and heat capacity through energy fluctuations are obtained and discussed in terms of tunneling rates and asymmetries."},"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":"1310.3155","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2013-10-11T15:01:30Z","cross_cats_sorted":[],"title_canon_sha256":"d5904fcb764ef4710a625561b73fada832a40e51e89c93b0cadb54d7a2533054","abstract_canon_sha256":"8935c3e39914349ece01fc8b6d1a629e0654282fdc206b85d7a998b9cf1f23fa"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:51:23.162824Z","signature_b64":"h1ZtclDYroN0ELLNikbFxAMQQ82KmNhUAX6OET3LkpxdEcfKLCdFCIxRpUfrM8B22KJSpRpDxBHFm99mBsjyCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e28e5b64d05125e022545f0e0028ce7de2640991702573820de96b9af674869c","last_reissued_at":"2026-05-18T02:51:23.162259Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:51:23.162259Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A Langevin canonical approach to the dynamics of chiral two level systems. Thermal averages and heat capacity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"A. Dorta-Urra, G. Rojas-Lorenzo, H. C. Pe\\~nate-Rodr\\'iguez, P. Bargue\\~no, S. Miret-Art\\'es","submitted_at":"2013-10-11T15:01:30Z","abstract_excerpt":"A Langevin canonical framework for a chiral two--level system coupled to a bath of harmonic oscillators is developed within a coupling scheme different to the well known spin-boson model. Thermal equilibrium values are reached at asymptotic times by solving the corresponding set of non--linear coupled equations in a Markovian regime. In particular, phase difference thermal values (or, equivalently, the so--called coherence factor) and heat capacity through energy fluctuations are obtained and discussed in terms of tunneling rates and asymmetries."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.3155","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":"1310.3155","created_at":"2026-05-18T02:51:23.162357+00:00"},{"alias_kind":"arxiv_version","alias_value":"1310.3155v1","created_at":"2026-05-18T02:51:23.162357+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.3155","created_at":"2026-05-18T02:51:23.162357+00:00"},{"alias_kind":"pith_short_12","alias_value":"4KHFWZGQKES6","created_at":"2026-05-18T12:27:34.582898+00:00"},{"alias_kind":"pith_short_16","alias_value":"4KHFWZGQKES6AISU","created_at":"2026-05-18T12:27:34.582898+00:00"},{"alias_kind":"pith_short_8","alias_value":"4KHFWZGQ","created_at":"2026-05-18T12:27:34.582898+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/4KHFWZGQKES6AISUL4HAAKGOPX","json":"https://pith.science/pith/4KHFWZGQKES6AISUL4HAAKGOPX.json","graph_json":"https://pith.science/api/pith-number/4KHFWZGQKES6AISUL4HAAKGOPX/graph.json","events_json":"https://pith.science/api/pith-number/4KHFWZGQKES6AISUL4HAAKGOPX/events.json","paper":"https://pith.science/paper/4KHFWZGQ"},"agent_actions":{"view_html":"https://pith.science/pith/4KHFWZGQKES6AISUL4HAAKGOPX","download_json":"https://pith.science/pith/4KHFWZGQKES6AISUL4HAAKGOPX.json","view_paper":"https://pith.science/paper/4KHFWZGQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1310.3155&json=true","fetch_graph":"https://pith.science/api/pith-number/4KHFWZGQKES6AISUL4HAAKGOPX/graph.json","fetch_events":"https://pith.science/api/pith-number/4KHFWZGQKES6AISUL4HAAKGOPX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4KHFWZGQKES6AISUL4HAAKGOPX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4KHFWZGQKES6AISUL4HAAKGOPX/action/storage_attestation","attest_author":"https://pith.science/pith/4KHFWZGQKES6AISUL4HAAKGOPX/action/author_attestation","sign_citation":"https://pith.science/pith/4KHFWZGQKES6AISUL4HAAKGOPX/action/citation_signature","submit_replication":"https://pith.science/pith/4KHFWZGQKES6AISUL4HAAKGOPX/action/replication_record"}},"created_at":"2026-05-18T02:51:23.162357+00:00","updated_at":"2026-05-18T02:51:23.162357+00:00"}