{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:RNC4SOQPSBIOR5ZT6SDPZCLTEW","short_pith_number":"pith:RNC4SOQP","schema_version":"1.0","canonical_sha256":"8b45c93a0f9050e8f733f486fc897325aecfcd4392e03c43d4bfb8c606d76763","source":{"kind":"arxiv","id":"1908.00502","version":1},"attestation_state":"computed","paper":{"title":"Upside/Downside statistical mechanics of nonequilibrium Brownian motion. II. Heat transfer and energy partitioning of a free particle","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Abraham Nitzan, Galen T. Craven, Renai Chen","submitted_at":"2019-08-01T16:51:54Z","abstract_excerpt":"The energy partitioning during activation and relaxation events under steady-state conditions for a Brownian particle driven by multiple thermal reservoirs of different local temperatures is investigated. Specifically, we apply the formalism derived in a previous article [G. T. Craven and A. Nitzan, J. Chem. Phys. 148, 044101 (2018)] to examine the thermal transport properties of two sub-ensembles of Brownian processes, distinguished at any given time by the specification that all the trajectories in each group have, at that time, energy either above (upside) or below (downside) a preselected "},"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":"1908.00502","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2019-08-01T16:51:54Z","cross_cats_sorted":[],"title_canon_sha256":"cc241dd0c803ebcec7302ed6c483ceba247904ce0edf71a590981bc6b9f11a90","abstract_canon_sha256":"9ece27da1683296fc9e02b350befc1ed3559c15cbd1676558d342c5ad5607edf"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T23:51:01.247527Z","signature_b64":"g47v5N56rrglH1ps5Sz3PiHD50z7vOMUuqfluYeL44r+rGAmlymFQD9tYdfzOX4SSJrwG0lm2LsNdFrzlcN2Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8b45c93a0f9050e8f733f486fc897325aecfcd4392e03c43d4bfb8c606d76763","last_reissued_at":"2026-07-04T23:51:01.247132Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T23:51:01.247132Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Upside/Downside statistical mechanics of nonequilibrium Brownian motion. II. Heat transfer and energy partitioning of a free particle","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Abraham Nitzan, Galen T. Craven, Renai Chen","submitted_at":"2019-08-01T16:51:54Z","abstract_excerpt":"The energy partitioning during activation and relaxation events under steady-state conditions for a Brownian particle driven by multiple thermal reservoirs of different local temperatures is investigated. Specifically, we apply the formalism derived in a previous article [G. T. Craven and A. Nitzan, J. Chem. Phys. 148, 044101 (2018)] to examine the thermal transport properties of two sub-ensembles of Brownian processes, distinguished at any given time by the specification that all the trajectories in each group have, at that time, energy either above (upside) or below (downside) a preselected "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1908.00502","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/1908.00502/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":"1908.00502","created_at":"2026-07-04T23:51:01.247190+00:00"},{"alias_kind":"arxiv_version","alias_value":"1908.00502v1","created_at":"2026-07-04T23:51:01.247190+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1908.00502","created_at":"2026-07-04T23:51:01.247190+00:00"},{"alias_kind":"pith_short_12","alias_value":"RNC4SOQPSBIO","created_at":"2026-07-04T23:51:01.247190+00:00"},{"alias_kind":"pith_short_16","alias_value":"RNC4SOQPSBIOR5ZT","created_at":"2026-07-04T23:51:01.247190+00:00"},{"alias_kind":"pith_short_8","alias_value":"RNC4SOQP","created_at":"2026-07-04T23:51:01.247190+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/RNC4SOQPSBIOR5ZT6SDPZCLTEW","json":"https://pith.science/pith/RNC4SOQPSBIOR5ZT6SDPZCLTEW.json","graph_json":"https://pith.science/api/pith-number/RNC4SOQPSBIOR5ZT6SDPZCLTEW/graph.json","events_json":"https://pith.science/api/pith-number/RNC4SOQPSBIOR5ZT6SDPZCLTEW/events.json","paper":"https://pith.science/paper/RNC4SOQP"},"agent_actions":{"view_html":"https://pith.science/pith/RNC4SOQPSBIOR5ZT6SDPZCLTEW","download_json":"https://pith.science/pith/RNC4SOQPSBIOR5ZT6SDPZCLTEW.json","view_paper":"https://pith.science/paper/RNC4SOQP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1908.00502&json=true","fetch_graph":"https://pith.science/api/pith-number/RNC4SOQPSBIOR5ZT6SDPZCLTEW/graph.json","fetch_events":"https://pith.science/api/pith-number/RNC4SOQPSBIOR5ZT6SDPZCLTEW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RNC4SOQPSBIOR5ZT6SDPZCLTEW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RNC4SOQPSBIOR5ZT6SDPZCLTEW/action/storage_attestation","attest_author":"https://pith.science/pith/RNC4SOQPSBIOR5ZT6SDPZCLTEW/action/author_attestation","sign_citation":"https://pith.science/pith/RNC4SOQPSBIOR5ZT6SDPZCLTEW/action/citation_signature","submit_replication":"https://pith.science/pith/RNC4SOQPSBIOR5ZT6SDPZCLTEW/action/replication_record"}},"created_at":"2026-07-04T23:51:01.247190+00:00","updated_at":"2026-07-04T23:51:01.247190+00:00"}