{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:46QM4FO4HPMXSGBR2RV2UWDIXA","short_pith_number":"pith:46QM4FO4","schema_version":"1.0","canonical_sha256":"e7a0ce15dc3bd9791831d46baa5868b8213637134df98bd2fc2aecebd1e579af","source":{"kind":"arxiv","id":"1707.05701","version":2},"attestation_state":"computed","paper":{"title":"Multifractal finite-size scaling at the Anderson transition in the unitary symmetry class","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.dis-nn","authors_text":"Alberto Rodr\\'iguez, Jakob Lindinger","submitted_at":"2017-07-17T10:00:48Z","abstract_excerpt":"We use multifractal finite-size scaling to perform a high-precision numerical study of the critical properties of the Anderson localization-delocalization transition in the unitary symmetry class, considering the Anderson model including a random magnetic flux. We demonstrate the scale invariance of the distribution of wavefunction intensities at the critical point and study its behavior across the transition. Our analysis, involving more than $4\\times10^6$ independently generated wavefunctions of system sizes up to $L^3=150^3$, yields accurate estimates for the critical exponent of the locali"},"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":"1707.05701","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2017-07-17T10:00:48Z","cross_cats_sorted":[],"title_canon_sha256":"e58e3499322f0f085600b5534f45c078264a94d2faa2016ef6fc92370edfde4a","abstract_canon_sha256":"52371b4e636a99d17c1e7644810f6024552331e42a46d917a8d8fc2b4f53ba0c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:33:16.342564Z","signature_b64":"Yvw0xEW26yEBaL+toSU5U4Wy639grU4hIWZ6qSa/4lwihsMYgPAEj6bUOuU535z928n6PD2cuYyyLbQWJzWZCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e7a0ce15dc3bd9791831d46baa5868b8213637134df98bd2fc2aecebd1e579af","last_reissued_at":"2026-05-18T00:33:16.341880Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:33:16.341880Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Multifractal finite-size scaling at the Anderson transition in the unitary symmetry class","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.dis-nn","authors_text":"Alberto Rodr\\'iguez, Jakob Lindinger","submitted_at":"2017-07-17T10:00:48Z","abstract_excerpt":"We use multifractal finite-size scaling to perform a high-precision numerical study of the critical properties of the Anderson localization-delocalization transition in the unitary symmetry class, considering the Anderson model including a random magnetic flux. We demonstrate the scale invariance of the distribution of wavefunction intensities at the critical point and study its behavior across the transition. Our analysis, involving more than $4\\times10^6$ independently generated wavefunctions of system sizes up to $L^3=150^3$, yields accurate estimates for the critical exponent of the locali"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.05701","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":""},"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":"1707.05701","created_at":"2026-05-18T00:33:16.341983+00:00"},{"alias_kind":"arxiv_version","alias_value":"1707.05701v2","created_at":"2026-05-18T00:33:16.341983+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.05701","created_at":"2026-05-18T00:33:16.341983+00:00"},{"alias_kind":"pith_short_12","alias_value":"46QM4FO4HPMX","created_at":"2026-05-18T12:30:58.224056+00:00"},{"alias_kind":"pith_short_16","alias_value":"46QM4FO4HPMXSGBR","created_at":"2026-05-18T12:30:58.224056+00:00"},{"alias_kind":"pith_short_8","alias_value":"46QM4FO4","created_at":"2026-05-18T12:30:58.224056+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/46QM4FO4HPMXSGBR2RV2UWDIXA","json":"https://pith.science/pith/46QM4FO4HPMXSGBR2RV2UWDIXA.json","graph_json":"https://pith.science/api/pith-number/46QM4FO4HPMXSGBR2RV2UWDIXA/graph.json","events_json":"https://pith.science/api/pith-number/46QM4FO4HPMXSGBR2RV2UWDIXA/events.json","paper":"https://pith.science/paper/46QM4FO4"},"agent_actions":{"view_html":"https://pith.science/pith/46QM4FO4HPMXSGBR2RV2UWDIXA","download_json":"https://pith.science/pith/46QM4FO4HPMXSGBR2RV2UWDIXA.json","view_paper":"https://pith.science/paper/46QM4FO4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1707.05701&json=true","fetch_graph":"https://pith.science/api/pith-number/46QM4FO4HPMXSGBR2RV2UWDIXA/graph.json","fetch_events":"https://pith.science/api/pith-number/46QM4FO4HPMXSGBR2RV2UWDIXA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/46QM4FO4HPMXSGBR2RV2UWDIXA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/46QM4FO4HPMXSGBR2RV2UWDIXA/action/storage_attestation","attest_author":"https://pith.science/pith/46QM4FO4HPMXSGBR2RV2UWDIXA/action/author_attestation","sign_citation":"https://pith.science/pith/46QM4FO4HPMXSGBR2RV2UWDIXA/action/citation_signature","submit_replication":"https://pith.science/pith/46QM4FO4HPMXSGBR2RV2UWDIXA/action/replication_record"}},"created_at":"2026-05-18T00:33:16.341983+00:00","updated_at":"2026-05-18T00:33:16.341983+00:00"}