{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2020:T3XSBEKLCES6MDIIJX2VFANB4Z","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":"f7f5cd6952aa794714a1851d149f44b81d7c6195e9c526b02804b9088fb1b667","cross_cats_sorted":["cond-mat.quant-gas","cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2020-12-23T18:09:21Z","title_canon_sha256":"04239b47614c94c4786e23f6c6d3e99282e606de643b1085165688143a4793f3"},"schema_version":"1.0","source":{"id":"2012.12841","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2012.12841","created_at":"2026-07-05T02:27:35Z"},{"alias_kind":"arxiv_version","alias_value":"2012.12841v2","created_at":"2026-07-05T02:27:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2012.12841","created_at":"2026-07-05T02:27:35Z"},{"alias_kind":"pith_short_12","alias_value":"T3XSBEKLCES6","created_at":"2026-07-05T02:27:35Z"},{"alias_kind":"pith_short_16","alias_value":"T3XSBEKLCES6MDII","created_at":"2026-07-05T02:27:35Z"},{"alias_kind":"pith_short_8","alias_value":"T3XSBEKL","created_at":"2026-07-05T02:27:35Z"}],"graph_snapshots":[{"event_id":"sha256:2c610d0f29244f12eeefa0afdba81db85fe25c289d3ddb79fbdd365a995896e4","target":"graph","created_at":"2026-07-05T02:27:35Z","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/2012.12841/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In this paper we consider an extension of the Rosenzweig-Porter (RP) model, the L\\'evy-RP (L-RP) model, in which the off-diagonal matrix elements are broadly distributed, providing a more realistic benchmark to develop an effective description of non-ergodic extended (NEE) states in interacting many-body disordered systems. We put forward a simple, general, and intuitive argument that allows one to unveil the multifractal structure of the mini-bands in the local spectrum when hybridization is due to anomalously large transition amplitudes in the tails of the distribution. The idea is that the ","authors_text":"Giulio Biroli, Marco Tarzia","cross_cats":["cond-mat.quant-gas","cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2020-12-23T18:09:21Z","title":"The L\\'evy-Rosenzweig-Porter random matrix ensemble"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2012.12841","kind":"arxiv","version":2},"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:a3fb3ee9b533b57f52034a66eba910d2a9646de5eaf41e698ad9c9f972fc6805","target":"record","created_at":"2026-07-05T02:27:35Z","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":"f7f5cd6952aa794714a1851d149f44b81d7c6195e9c526b02804b9088fb1b667","cross_cats_sorted":["cond-mat.quant-gas","cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2020-12-23T18:09:21Z","title_canon_sha256":"04239b47614c94c4786e23f6c6d3e99282e606de643b1085165688143a4793f3"},"schema_version":"1.0","source":{"id":"2012.12841","kind":"arxiv","version":2}},"canonical_sha256":"9eef20914b1125e60d084df55281a1e64d91c85572bca4f2025f5de6964ab265","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9eef20914b1125e60d084df55281a1e64d91c85572bca4f2025f5de6964ab265","first_computed_at":"2026-07-05T02:27:35.412025Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T02:27:35.412025Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"sSF3ExdtU5dgD4BGMUD9gNWHAkAz73T7OXxFY74V97Ty/gLlcS+bbyy5tgkX8q8XzFttPLk9Iyla/RANYx6KDw==","signature_status":"signed_v1","signed_at":"2026-07-05T02:27:35.412410Z","signed_message":"canonical_sha256_bytes"},"source_id":"2012.12841","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a3fb3ee9b533b57f52034a66eba910d2a9646de5eaf41e698ad9c9f972fc6805","sha256:2c610d0f29244f12eeefa0afdba81db85fe25c289d3ddb79fbdd365a995896e4"],"state_sha256":"f40638eea594954b38fdb44d24ba70943b2adf9994c34b562c86d03d4e757dc0"}