{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:XMGTQ7OUZY7YLW265MYJXS4J6L","short_pith_number":"pith:XMGTQ7OU","schema_version":"1.0","canonical_sha256":"bb0d387dd4ce3f85db5eeb309bcb89f2c2bc249e35663a7c5f471930a03fa442","source":{"kind":"arxiv","id":"1707.05921","version":1},"attestation_state":"computed","paper":{"title":"Thermalization without eigenstate thermalization hypothesis after a quantum quench","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Naoto Shiraishi, Takashi Mori","submitted_at":"2017-07-19T02:16:02Z","abstract_excerpt":"Nonequilibrium dynamics of a nonintegrable system without the eigenstate thermalization hypothesis is studied. It is shown that, in the thermodynamic limit, this model thermalizes after an arbitrary quantum quench at finite temperature, although it does not satisfy the eigenstate thermalization hypothesis. In contrast, when the system size is finite and the temperature is low enough, the system may not thermalize. In this case, the steady state is well described by the generalized Gibbs ensemble constructed by using highly nonlocal conserved quantities. We also show that this model exhibits pr"},"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":"1707.05921","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-07-19T02:16:02Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"8b1ece95f87ed3167b43b0768cc497faf6b49871d95a0140c1b6cbd9c3b2325a","abstract_canon_sha256":"9e00465c96e0cefc7aad385de36d09400ccf6e6423504010069987cf2bf7bde8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:35:58.297462Z","signature_b64":"vYPFAtkLP5HwI2WsS7kzwt+ZFqvvxQsJmar/ZvtcjY2BnP5Crn+Ab6kyJCt1vHN0mAxMeSZaaN7hhYOERdfbBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bb0d387dd4ce3f85db5eeb309bcb89f2c2bc249e35663a7c5f471930a03fa442","last_reissued_at":"2026-05-18T00:35:58.296712Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:35:58.296712Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermalization without eigenstate thermalization hypothesis after a quantum quench","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Naoto Shiraishi, Takashi Mori","submitted_at":"2017-07-19T02:16:02Z","abstract_excerpt":"Nonequilibrium dynamics of a nonintegrable system without the eigenstate thermalization hypothesis is studied. It is shown that, in the thermodynamic limit, this model thermalizes after an arbitrary quantum quench at finite temperature, although it does not satisfy the eigenstate thermalization hypothesis. In contrast, when the system size is finite and the temperature is low enough, the system may not thermalize. In this case, the steady state is well described by the generalized Gibbs ensemble constructed by using highly nonlocal conserved quantities. We also show that this model exhibits pr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.05921","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":"1707.05921","created_at":"2026-05-18T00:35:58.296844+00:00"},{"alias_kind":"arxiv_version","alias_value":"1707.05921v1","created_at":"2026-05-18T00:35:58.296844+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.05921","created_at":"2026-05-18T00:35:58.296844+00:00"},{"alias_kind":"pith_short_12","alias_value":"XMGTQ7OUZY7Y","created_at":"2026-05-18T12:31:56.362134+00:00"},{"alias_kind":"pith_short_16","alias_value":"XMGTQ7OUZY7YLW26","created_at":"2026-05-18T12:31:56.362134+00:00"},{"alias_kind":"pith_short_8","alias_value":"XMGTQ7OU","created_at":"2026-05-18T12:31:56.362134+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2310.18880","citing_title":"Nature abhors a vacuum: A simple rigorous example of thermalization in an isolated macroscopic quantum system","ref_index":37,"is_internal_anchor":true},{"citing_arxiv_id":"2412.18504","citing_title":"The $S=\\frac{1}{2}$ XY and XYZ models on the two or higher dimensional hypercubic lattice do not possess nontrivial local conserved quantities","ref_index":13,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XMGTQ7OUZY7YLW265MYJXS4J6L","json":"https://pith.science/pith/XMGTQ7OUZY7YLW265MYJXS4J6L.json","graph_json":"https://pith.science/api/pith-number/XMGTQ7OUZY7YLW265MYJXS4J6L/graph.json","events_json":"https://pith.science/api/pith-number/XMGTQ7OUZY7YLW265MYJXS4J6L/events.json","paper":"https://pith.science/paper/XMGTQ7OU"},"agent_actions":{"view_html":"https://pith.science/pith/XMGTQ7OUZY7YLW265MYJXS4J6L","download_json":"https://pith.science/pith/XMGTQ7OUZY7YLW265MYJXS4J6L.json","view_paper":"https://pith.science/paper/XMGTQ7OU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1707.05921&json=true","fetch_graph":"https://pith.science/api/pith-number/XMGTQ7OUZY7YLW265MYJXS4J6L/graph.json","fetch_events":"https://pith.science/api/pith-number/XMGTQ7OUZY7YLW265MYJXS4J6L/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XMGTQ7OUZY7YLW265MYJXS4J6L/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XMGTQ7OUZY7YLW265MYJXS4J6L/action/storage_attestation","attest_author":"https://pith.science/pith/XMGTQ7OUZY7YLW265MYJXS4J6L/action/author_attestation","sign_citation":"https://pith.science/pith/XMGTQ7OUZY7YLW265MYJXS4J6L/action/citation_signature","submit_replication":"https://pith.science/pith/XMGTQ7OUZY7YLW265MYJXS4J6L/action/replication_record"}},"created_at":"2026-05-18T00:35:58.296844+00:00","updated_at":"2026-05-18T00:35:58.296844+00:00"}