{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:LTUSRWGRZX2NDIC7NAHSKOYSF3","short_pith_number":"pith:LTUSRWGR","schema_version":"1.0","canonical_sha256":"5ce928d8d1cdf4d1a05f680f253b122eded1b63fd4088e42f6409f9c55ca718a","source":{"kind":"arxiv","id":"1711.09880","version":1},"attestation_state":"computed","paper":{"title":"A microscopically motivated renormalization scheme for the MBL/ETH transition","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn"],"primary_cat":"cond-mat.stat-mech","authors_text":"Markus M\\\"uller, Thimoth\\'ee Thiery, Wojciech De Roeck","submitted_at":"2017-11-27T18:53:25Z","abstract_excerpt":"We introduce a multi-scale diagonalization scheme to study the transition between the many-body localized and the ergodic phase in disordered quantum chains. The scheme assumes a sharp dichotomy between subsystems that behave as localized and resonant spots that obey the Eigenstate Thermalization Hypothesis (ETH). We establish a set of microscopic principles defining the diagonalization scheme, and use them to numerically study the transition in very large systems. To a large extent the results are in agreement with an analytically tractable mean-field analysis of the scheme: We find that at t"},"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":"1711.09880","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-11-27T18:53:25Z","cross_cats_sorted":["cond-mat.dis-nn"],"title_canon_sha256":"b0e65220bbe17c0826eff28b0a2298ecec9d197eaa096c8f5a7246f35000ff3c","abstract_canon_sha256":"e4b9c0dd96313cc815200a879ccfbc18850a64c094e8052a61626360ac9dd169"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:29:34.270943Z","signature_b64":"sL5XrN+/PQMC7gKZdC+si2+LqjMpkDXETHkwPGdgxjrZ/TGoqj3bfqjAoKx8xwdnqJjeQ0ZHtRHpUSBzYLhBBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5ce928d8d1cdf4d1a05f680f253b122eded1b63fd4088e42f6409f9c55ca718a","last_reissued_at":"2026-05-18T00:29:34.270470Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:29:34.270470Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A microscopically motivated renormalization scheme for the MBL/ETH transition","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn"],"primary_cat":"cond-mat.stat-mech","authors_text":"Markus M\\\"uller, Thimoth\\'ee Thiery, Wojciech De Roeck","submitted_at":"2017-11-27T18:53:25Z","abstract_excerpt":"We introduce a multi-scale diagonalization scheme to study the transition between the many-body localized and the ergodic phase in disordered quantum chains. The scheme assumes a sharp dichotomy between subsystems that behave as localized and resonant spots that obey the Eigenstate Thermalization Hypothesis (ETH). We establish a set of microscopic principles defining the diagonalization scheme, and use them to numerically study the transition in very large systems. To a large extent the results are in agreement with an analytically tractable mean-field analysis of the scheme: We find that at t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.09880","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":"1711.09880","created_at":"2026-05-18T00:29:34.270542+00:00"},{"alias_kind":"arxiv_version","alias_value":"1711.09880v1","created_at":"2026-05-18T00:29:34.270542+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.09880","created_at":"2026-05-18T00:29:34.270542+00:00"},{"alias_kind":"pith_short_12","alias_value":"LTUSRWGRZX2N","created_at":"2026-05-18T12:31:28.150371+00:00"},{"alias_kind":"pith_short_16","alias_value":"LTUSRWGRZX2NDIC7","created_at":"2026-05-18T12:31:28.150371+00:00"},{"alias_kind":"pith_short_8","alias_value":"LTUSRWGR","created_at":"2026-05-18T12:31:28.150371+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/LTUSRWGRZX2NDIC7NAHSKOYSF3","json":"https://pith.science/pith/LTUSRWGRZX2NDIC7NAHSKOYSF3.json","graph_json":"https://pith.science/api/pith-number/LTUSRWGRZX2NDIC7NAHSKOYSF3/graph.json","events_json":"https://pith.science/api/pith-number/LTUSRWGRZX2NDIC7NAHSKOYSF3/events.json","paper":"https://pith.science/paper/LTUSRWGR"},"agent_actions":{"view_html":"https://pith.science/pith/LTUSRWGRZX2NDIC7NAHSKOYSF3","download_json":"https://pith.science/pith/LTUSRWGRZX2NDIC7NAHSKOYSF3.json","view_paper":"https://pith.science/paper/LTUSRWGR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1711.09880&json=true","fetch_graph":"https://pith.science/api/pith-number/LTUSRWGRZX2NDIC7NAHSKOYSF3/graph.json","fetch_events":"https://pith.science/api/pith-number/LTUSRWGRZX2NDIC7NAHSKOYSF3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LTUSRWGRZX2NDIC7NAHSKOYSF3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LTUSRWGRZX2NDIC7NAHSKOYSF3/action/storage_attestation","attest_author":"https://pith.science/pith/LTUSRWGRZX2NDIC7NAHSKOYSF3/action/author_attestation","sign_citation":"https://pith.science/pith/LTUSRWGRZX2NDIC7NAHSKOYSF3/action/citation_signature","submit_replication":"https://pith.science/pith/LTUSRWGRZX2NDIC7NAHSKOYSF3/action/replication_record"}},"created_at":"2026-05-18T00:29:34.270542+00:00","updated_at":"2026-05-18T00:29:34.270542+00:00"}