{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:A7D43NWZHAHIXKHXDSGIOHZFM3","short_pith_number":"pith:A7D43NWZ","schema_version":"1.0","canonical_sha256":"07c7cdb6d9380e8ba8f71c8c871f2566d151170c5e196c99922ada831f589cbe","source":{"kind":"arxiv","id":"2503.00119","version":2},"attestation_state":"computed","paper":{"title":"Universality in the Anticoncentration of Chaotic Quantum Circuits","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Arman Sauliere, Beatrice Magni, Guglielmo Lami, Jacopo De Nardis, Xhek Turkeshi","submitted_at":"2025-02-28T19:00:26Z","abstract_excerpt":"We identify a \\emph{universal functional form} that governs anticoncentration in random quantum circuits-one that holds across diverse circuit architectures and depths, and crucially remains valid even at finite system sizes and shallow depth. We support this claim through analytical results for ensembles of random tensor-network states and random-phase models. This compact, universal expression for the output bitstring probability distribution is fully characterized by just two fitting parameters, as validated through extensive numerical simulations. Our findings underscore the pivotal role o"},"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":"2503.00119","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2025-02-28T19:00:26Z","cross_cats_sorted":[],"title_canon_sha256":"5f9b65438b9c06b140adfec6dbed85d9ca17a4145889902168cd2420e566d450","abstract_canon_sha256":"83d86c2a5f368bd7d1283e33d4c413458436155aba74013729d76162b0718dda"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:33:04.131665Z","signature_b64":"L75Ro96dbOOkG0qrE+GKAnzBGijqUy5+eHWVgb+cO01S/tQ63tU22QNDwqGCbeuF2gWlpar9dtnUlaxRwPaGBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"07c7cdb6d9380e8ba8f71c8c871f2566d151170c5e196c99922ada831f589cbe","last_reissued_at":"2026-07-05T11:33:04.131181Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:33:04.131181Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Universality in the Anticoncentration of Chaotic Quantum Circuits","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Arman Sauliere, Beatrice Magni, Guglielmo Lami, Jacopo De Nardis, Xhek Turkeshi","submitted_at":"2025-02-28T19:00:26Z","abstract_excerpt":"We identify a \\emph{universal functional form} that governs anticoncentration in random quantum circuits-one that holds across diverse circuit architectures and depths, and crucially remains valid even at finite system sizes and shallow depth. We support this claim through analytical results for ensembles of random tensor-network states and random-phase models. This compact, universal expression for the output bitstring probability distribution is fully characterized by just two fitting parameters, as validated through extensive numerical simulations. Our findings underscore the pivotal role o"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2503.00119","kind":"arxiv","version":2},"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/2503.00119/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":"2503.00119","created_at":"2026-07-05T11:33:04.131240+00:00"},{"alias_kind":"arxiv_version","alias_value":"2503.00119v2","created_at":"2026-07-05T11:33:04.131240+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2503.00119","created_at":"2026-07-05T11:33:04.131240+00:00"},{"alias_kind":"pith_short_12","alias_value":"A7D43NWZHAHI","created_at":"2026-07-05T11:33:04.131240+00:00"},{"alias_kind":"pith_short_16","alias_value":"A7D43NWZHAHIXKHX","created_at":"2026-07-05T11:33:04.131240+00:00"},{"alias_kind":"pith_short_8","alias_value":"A7D43NWZ","created_at":"2026-07-05T11:33:04.131240+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.07556","citing_title":"Entanglement Asymmetry in Random Quantum Automata","ref_index":58,"is_internal_anchor":true},{"citing_arxiv_id":"2603.28870","citing_title":"Non-stabilizerness and U(1) symmetry in chaotic many-body quantum systems","ref_index":111,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/A7D43NWZHAHIXKHXDSGIOHZFM3","json":"https://pith.science/pith/A7D43NWZHAHIXKHXDSGIOHZFM3.json","graph_json":"https://pith.science/api/pith-number/A7D43NWZHAHIXKHXDSGIOHZFM3/graph.json","events_json":"https://pith.science/api/pith-number/A7D43NWZHAHIXKHXDSGIOHZFM3/events.json","paper":"https://pith.science/paper/A7D43NWZ"},"agent_actions":{"view_html":"https://pith.science/pith/A7D43NWZHAHIXKHXDSGIOHZFM3","download_json":"https://pith.science/pith/A7D43NWZHAHIXKHXDSGIOHZFM3.json","view_paper":"https://pith.science/paper/A7D43NWZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2503.00119&json=true","fetch_graph":"https://pith.science/api/pith-number/A7D43NWZHAHIXKHXDSGIOHZFM3/graph.json","fetch_events":"https://pith.science/api/pith-number/A7D43NWZHAHIXKHXDSGIOHZFM3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/A7D43NWZHAHIXKHXDSGIOHZFM3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/A7D43NWZHAHIXKHXDSGIOHZFM3/action/storage_attestation","attest_author":"https://pith.science/pith/A7D43NWZHAHIXKHXDSGIOHZFM3/action/author_attestation","sign_citation":"https://pith.science/pith/A7D43NWZHAHIXKHXDSGIOHZFM3/action/citation_signature","submit_replication":"https://pith.science/pith/A7D43NWZHAHIXKHXDSGIOHZFM3/action/replication_record"}},"created_at":"2026-07-05T11:33:04.131240+00:00","updated_at":"2026-07-05T11:33:04.131240+00:00"}