{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:BCGFEYOLV2E4HAGLCLMJRMWSXS","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"883a9c8cef5047ee04c078b6705695639f67bd431a6498e4ae2a7b132d5d970c","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2021-03-09T19:15:56Z","title_canon_sha256":"d55339d4d3a65cdf5a4272a4088da387c8db00204745f5df294edeb0d5895ddb"},"schema_version":"1.0","source":{"id":"2103.05670","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2103.05670","created_at":"2026-07-05T02:55:41Z"},{"alias_kind":"arxiv_version","alias_value":"2103.05670v1","created_at":"2026-07-05T02:55:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2103.05670","created_at":"2026-07-05T02:55:41Z"},{"alias_kind":"pith_short_12","alias_value":"BCGFEYOLV2E4","created_at":"2026-07-05T02:55:41Z"},{"alias_kind":"pith_short_16","alias_value":"BCGFEYOLV2E4HAGL","created_at":"2026-07-05T02:55:41Z"},{"alias_kind":"pith_short_8","alias_value":"BCGFEYOL","created_at":"2026-07-05T02:55:41Z"}],"graph_snapshots":[{"event_id":"sha256:b1a2c31c1e80ecca967ec4ff8812a1b526272e597b7717f9507a1d5532bb4769","target":"graph","created_at":"2026-07-05T02:55:41Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2103.05670/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present a semi-analytical approach for studying quantum thermal energy transport beyond the weak system-bath coupling regime. Our treatment, which results in a renormalized, effective Hamiltonian model is based on the reaction coordinate method. In our technique, applied to the nonequilibrium spin-boson model, a collective coordinate is extracted from each environment and added into the system to construct an enlarged system. After performing additional Hamiltonian's truncation and transformation, we attain an effective two-level system with renormalized parameters, which is weakly coupled ","authors_text":"Dvira Segal, Nicholas Anto-Sztrikacs","cross_cats":["cond-mat.mes-hall","cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2021-03-09T19:15:56Z","title":"Strong coupling effects in quantum thermal transport with the reaction coordinate method"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2103.05670","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:2e8783dde8d2572a5f1e2d716cf8e0023c69e45fa1ab512f9f29b0d39988f802","target":"record","created_at":"2026-07-05T02:55:41Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"883a9c8cef5047ee04c078b6705695639f67bd431a6498e4ae2a7b132d5d970c","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2021-03-09T19:15:56Z","title_canon_sha256":"d55339d4d3a65cdf5a4272a4088da387c8db00204745f5df294edeb0d5895ddb"},"schema_version":"1.0","source":{"id":"2103.05670","kind":"arxiv","version":1}},"canonical_sha256":"088c5261cbae89c380cb12d898b2d2bcbc8f2705175c3a533e10afc5ab37364e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"088c5261cbae89c380cb12d898b2d2bcbc8f2705175c3a533e10afc5ab37364e","first_computed_at":"2026-07-05T02:55:41.981803Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T02:55:41.981803Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"UXFRUPCfnobdsukXQT/nAZPB71hiwvM0gMIjJaQ+pg9S79PWgZGFAhSpSjtT7tRYbWVwRnu/s6rsP7v6R2/BDA==","signature_status":"signed_v1","signed_at":"2026-07-05T02:55:41.982251Z","signed_message":"canonical_sha256_bytes"},"source_id":"2103.05670","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2e8783dde8d2572a5f1e2d716cf8e0023c69e45fa1ab512f9f29b0d39988f802","sha256:b1a2c31c1e80ecca967ec4ff8812a1b526272e597b7717f9507a1d5532bb4769"],"state_sha256":"56913804a5033e35e20de18b1db0005fb8d269374349b5fc4af12377176c3cc6"}