{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:TJL3OWS6IMSZJXUM4HBPWL24MS","short_pith_number":"pith:TJL3OWS6","schema_version":"1.0","canonical_sha256":"9a57b75a5e432594de8ce1c2fb2f5c64bd36c0cbc1bb19cc108db37e179e4874","source":{"kind":"arxiv","id":"1704.05474","version":3},"attestation_state":"computed","paper":{"title":"Work extraction in an isolated quantum lattice system: Grand canonical and generalized Gibbs ensemble predictions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","quant-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Marcos Rigol, Ranjan Modak","submitted_at":"2017-04-18T18:01:02Z","abstract_excerpt":"We study work extraction (defined as the difference between the initial and the final energy) in noninteracting and (effectively) weakly interacting isolated fermionic quantum lattice systems in one dimension, which undergo a sequence of quenches and equilibration. The systems are divided in two parts, which we identify as the subsystem of interest and the bath. We extract work by quenching the on-site potentials in the subsystem, letting the entire system equilibrate, and returning to the initial parameters in the subsystem using a quasi-static process (the bath is never acted upon). We selec"},"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":"1704.05474","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-04-18T18:01:02Z","cross_cats_sorted":["cond-mat.quant-gas","quant-ph"],"title_canon_sha256":"4dae787d79f4e60e6639745694adcb419e602e7447473457cba6dabbf79b1ba5","abstract_canon_sha256":"b98696a84527da7af131b8ad0a9b8abe2da3edde204829e6184d17d309caddd3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:40:57.957424Z","signature_b64":"qQlast/DUToqQx9CaThsX+Ip5CY2aHB1+/iXlTnFHE6r0iZI5yCNPyvCYXVwkVveIoRxBERAnv2iWbHN+r8rCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9a57b75a5e432594de8ce1c2fb2f5c64bd36c0cbc1bb19cc108db37e179e4874","last_reissued_at":"2026-05-18T00:40:57.956997Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:40:57.956997Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Work extraction in an isolated quantum lattice system: Grand canonical and generalized Gibbs ensemble predictions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","quant-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Marcos Rigol, Ranjan Modak","submitted_at":"2017-04-18T18:01:02Z","abstract_excerpt":"We study work extraction (defined as the difference between the initial and the final energy) in noninteracting and (effectively) weakly interacting isolated fermionic quantum lattice systems in one dimension, which undergo a sequence of quenches and equilibration. The systems are divided in two parts, which we identify as the subsystem of interest and the bath. We extract work by quenching the on-site potentials in the subsystem, letting the entire system equilibrate, and returning to the initial parameters in the subsystem using a quasi-static process (the bath is never acted upon). We selec"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.05474","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":"1704.05474","created_at":"2026-05-18T00:40:57.957063+00:00"},{"alias_kind":"arxiv_version","alias_value":"1704.05474v3","created_at":"2026-05-18T00:40:57.957063+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.05474","created_at":"2026-05-18T00:40:57.957063+00:00"},{"alias_kind":"pith_short_12","alias_value":"TJL3OWS6IMSZ","created_at":"2026-05-18T12:31:46.661854+00:00"},{"alias_kind":"pith_short_16","alias_value":"TJL3OWS6IMSZJXUM","created_at":"2026-05-18T12:31:46.661854+00:00"},{"alias_kind":"pith_short_8","alias_value":"TJL3OWS6","created_at":"2026-05-18T12:31:46.661854+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/TJL3OWS6IMSZJXUM4HBPWL24MS","json":"https://pith.science/pith/TJL3OWS6IMSZJXUM4HBPWL24MS.json","graph_json":"https://pith.science/api/pith-number/TJL3OWS6IMSZJXUM4HBPWL24MS/graph.json","events_json":"https://pith.science/api/pith-number/TJL3OWS6IMSZJXUM4HBPWL24MS/events.json","paper":"https://pith.science/paper/TJL3OWS6"},"agent_actions":{"view_html":"https://pith.science/pith/TJL3OWS6IMSZJXUM4HBPWL24MS","download_json":"https://pith.science/pith/TJL3OWS6IMSZJXUM4HBPWL24MS.json","view_paper":"https://pith.science/paper/TJL3OWS6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1704.05474&json=true","fetch_graph":"https://pith.science/api/pith-number/TJL3OWS6IMSZJXUM4HBPWL24MS/graph.json","fetch_events":"https://pith.science/api/pith-number/TJL3OWS6IMSZJXUM4HBPWL24MS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TJL3OWS6IMSZJXUM4HBPWL24MS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TJL3OWS6IMSZJXUM4HBPWL24MS/action/storage_attestation","attest_author":"https://pith.science/pith/TJL3OWS6IMSZJXUM4HBPWL24MS/action/author_attestation","sign_citation":"https://pith.science/pith/TJL3OWS6IMSZJXUM4HBPWL24MS/action/citation_signature","submit_replication":"https://pith.science/pith/TJL3OWS6IMSZJXUM4HBPWL24MS/action/replication_record"}},"created_at":"2026-05-18T00:40:57.957063+00:00","updated_at":"2026-05-18T00:40:57.957063+00:00"}