{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:J2XDWZGASWGLXMXITU7NMKXS32","short_pith_number":"pith:J2XDWZGA","schema_version":"1.0","canonical_sha256":"4eae3b64c0958cbbb2e89d3ed62af2de9bd76dca3ada82bd15c86794a236b1fb","source":{"kind":"arxiv","id":"1211.6606","version":1},"attestation_state":"computed","paper":{"title":"Analytical and numerical study of uncorrelated disorder on a honeycomb lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","quant-ph"],"primary_cat":"cond-mat.dis-nn","authors_text":"Beno\\^it Gr\\'emaud, Christian Miniatura, Dominique Delande, Kean Loon Lee","submitted_at":"2012-11-28T14:05:08Z","abstract_excerpt":"We consider a tight-binding model on the regular honeycomb lattice with uncorrelated on-site disorder. We use two independent methods (recursive Green's function and self-consistent Born approximation) to extract the scattering mean free path, the scattering mean free time, the density of states and the localization length as a function of the disorder strength. The two methods give excellent quantitative agreement for these single-particle properties. Furthermore, a finite-size scaling analysis reveals that all localization lengths for different lattice sizes and different energies (including"},"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":"1211.6606","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2012-11-28T14:05:08Z","cross_cats_sorted":["cond-mat.quant-gas","quant-ph"],"title_canon_sha256":"6c6ace616c46b910efb8dc3ac05f117c7cb6e2f03c306b705e8ec6a862788ab9","abstract_canon_sha256":"c5b33a228b8fe0eb809d7793778c27c474bc2534275f2c2cc60b570c81beec5d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:28:29.263176Z","signature_b64":"OiUtrUthMrtx89x5ychbG4KCaKZfJnjDUVHOqjTR5168kP+6pY2P+bs0aEDcMvIldEt4QTAuvKi0Rm1y3b9oDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4eae3b64c0958cbbb2e89d3ed62af2de9bd76dca3ada82bd15c86794a236b1fb","last_reissued_at":"2026-05-18T03:28:29.262576Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:28:29.262576Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Analytical and numerical study of uncorrelated disorder on a honeycomb lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","quant-ph"],"primary_cat":"cond-mat.dis-nn","authors_text":"Beno\\^it Gr\\'emaud, Christian Miniatura, Dominique Delande, Kean Loon Lee","submitted_at":"2012-11-28T14:05:08Z","abstract_excerpt":"We consider a tight-binding model on the regular honeycomb lattice with uncorrelated on-site disorder. We use two independent methods (recursive Green's function and self-consistent Born approximation) to extract the scattering mean free path, the scattering mean free time, the density of states and the localization length as a function of the disorder strength. The two methods give excellent quantitative agreement for these single-particle properties. Furthermore, a finite-size scaling analysis reveals that all localization lengths for different lattice sizes and different energies (including"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.6606","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":"1211.6606","created_at":"2026-05-18T03:28:29.262669+00:00"},{"alias_kind":"arxiv_version","alias_value":"1211.6606v1","created_at":"2026-05-18T03:28:29.262669+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.6606","created_at":"2026-05-18T03:28:29.262669+00:00"},{"alias_kind":"pith_short_12","alias_value":"J2XDWZGASWGL","created_at":"2026-05-18T12:27:09.501522+00:00"},{"alias_kind":"pith_short_16","alias_value":"J2XDWZGASWGLXMXI","created_at":"2026-05-18T12:27:09.501522+00:00"},{"alias_kind":"pith_short_8","alias_value":"J2XDWZGA","created_at":"2026-05-18T12:27:09.501522+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/J2XDWZGASWGLXMXITU7NMKXS32","json":"https://pith.science/pith/J2XDWZGASWGLXMXITU7NMKXS32.json","graph_json":"https://pith.science/api/pith-number/J2XDWZGASWGLXMXITU7NMKXS32/graph.json","events_json":"https://pith.science/api/pith-number/J2XDWZGASWGLXMXITU7NMKXS32/events.json","paper":"https://pith.science/paper/J2XDWZGA"},"agent_actions":{"view_html":"https://pith.science/pith/J2XDWZGASWGLXMXITU7NMKXS32","download_json":"https://pith.science/pith/J2XDWZGASWGLXMXITU7NMKXS32.json","view_paper":"https://pith.science/paper/J2XDWZGA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1211.6606&json=true","fetch_graph":"https://pith.science/api/pith-number/J2XDWZGASWGLXMXITU7NMKXS32/graph.json","fetch_events":"https://pith.science/api/pith-number/J2XDWZGASWGLXMXITU7NMKXS32/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/J2XDWZGASWGLXMXITU7NMKXS32/action/timestamp_anchor","attest_storage":"https://pith.science/pith/J2XDWZGASWGLXMXITU7NMKXS32/action/storage_attestation","attest_author":"https://pith.science/pith/J2XDWZGASWGLXMXITU7NMKXS32/action/author_attestation","sign_citation":"https://pith.science/pith/J2XDWZGASWGLXMXITU7NMKXS32/action/citation_signature","submit_replication":"https://pith.science/pith/J2XDWZGASWGLXMXITU7NMKXS32/action/replication_record"}},"created_at":"2026-05-18T03:28:29.262669+00:00","updated_at":"2026-05-18T03:28:29.262669+00:00"}