{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:BZEEEZZOLLI7AOEIATX5OQVREI","short_pith_number":"pith:BZEEEZZO","schema_version":"1.0","canonical_sha256":"0e4842672e5ad1f0388804efd742b1221c3b7213daccb185462e9fefb3702441","source":{"kind":"arxiv","id":"2410.16034","version":1},"attestation_state":"computed","paper":{"title":"Amorphization-induced topological and insulator-metal transitions in bidimensional Bi$_x$Sb$_{1-x}$ alloys","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.dis-nn","authors_text":"A. J. Ur\\'ia-\\'Alvarez, J. J. Palacios","submitted_at":"2024-10-21T14:08:49Z","abstract_excerpt":"Bismuth has been shown to be topological in its different allotropes and compounds, with one of the most notable examples being the Bi-Sb alloy, the first 3D topological insulator ever discovered. In this paper we explore two-dimensional alloys of Bi and Sb, both crystalline and amorphous, to determine the critical concentrations that render the alloys topological. For the amorphous alloy, we determine the effect of structural disorder on its topological properties, remarkably observing a trivial to topological transition as disorder increases. The alloys are modelled using a Slater-Koster tig"},"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":"2410.16034","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2024-10-21T14:08:49Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"b052b2922356c0d4409cc3ba1137f476b0566a8c5edecb188482f4a787ab350a","abstract_canon_sha256":"4940d8f95750696e52a6e99374d9d0da6ad0e4e2a1c3b8556431364aead0824b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:23:28.296223Z","signature_b64":"PLpErmqNBgfkq5PqkUb+oy6GOlAlvI9Vd61rksFieo80An9wv5zwl1nHDECYPRE6EhATTPiQubW4dYEhOWU4DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0e4842672e5ad1f0388804efd742b1221c3b7213daccb185462e9fefb3702441","last_reissued_at":"2026-07-05T09:23:28.295718Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:23:28.295718Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Amorphization-induced topological and insulator-metal transitions in bidimensional Bi$_x$Sb$_{1-x}$ alloys","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.dis-nn","authors_text":"A. J. Ur\\'ia-\\'Alvarez, J. J. Palacios","submitted_at":"2024-10-21T14:08:49Z","abstract_excerpt":"Bismuth has been shown to be topological in its different allotropes and compounds, with one of the most notable examples being the Bi-Sb alloy, the first 3D topological insulator ever discovered. In this paper we explore two-dimensional alloys of Bi and Sb, both crystalline and amorphous, to determine the critical concentrations that render the alloys topological. For the amorphous alloy, we determine the effect of structural disorder on its topological properties, remarkably observing a trivial to topological transition as disorder increases. The alloys are modelled using a Slater-Koster tig"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2410.16034","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2410.16034/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":"2410.16034","created_at":"2026-07-05T09:23:28.295777+00:00"},{"alias_kind":"arxiv_version","alias_value":"2410.16034v1","created_at":"2026-07-05T09:23:28.295777+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2410.16034","created_at":"2026-07-05T09:23:28.295777+00:00"},{"alias_kind":"pith_short_12","alias_value":"BZEEEZZOLLI7","created_at":"2026-07-05T09:23:28.295777+00:00"},{"alias_kind":"pith_short_16","alias_value":"BZEEEZZOLLI7AOEI","created_at":"2026-07-05T09:23:28.295777+00:00"},{"alias_kind":"pith_short_8","alias_value":"BZEEEZZO","created_at":"2026-07-05T09:23:28.295777+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2509.03632","citing_title":"One-Particle Density Matrix Framework for Mode-Shell Correspondence: Characterizing Topology in Amorphous Higher-Order Topological Insulators","ref_index":83,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BZEEEZZOLLI7AOEIATX5OQVREI","json":"https://pith.science/pith/BZEEEZZOLLI7AOEIATX5OQVREI.json","graph_json":"https://pith.science/api/pith-number/BZEEEZZOLLI7AOEIATX5OQVREI/graph.json","events_json":"https://pith.science/api/pith-number/BZEEEZZOLLI7AOEIATX5OQVREI/events.json","paper":"https://pith.science/paper/BZEEEZZO"},"agent_actions":{"view_html":"https://pith.science/pith/BZEEEZZOLLI7AOEIATX5OQVREI","download_json":"https://pith.science/pith/BZEEEZZOLLI7AOEIATX5OQVREI.json","view_paper":"https://pith.science/paper/BZEEEZZO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2410.16034&json=true","fetch_graph":"https://pith.science/api/pith-number/BZEEEZZOLLI7AOEIATX5OQVREI/graph.json","fetch_events":"https://pith.science/api/pith-number/BZEEEZZOLLI7AOEIATX5OQVREI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BZEEEZZOLLI7AOEIATX5OQVREI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BZEEEZZOLLI7AOEIATX5OQVREI/action/storage_attestation","attest_author":"https://pith.science/pith/BZEEEZZOLLI7AOEIATX5OQVREI/action/author_attestation","sign_citation":"https://pith.science/pith/BZEEEZZOLLI7AOEIATX5OQVREI/action/citation_signature","submit_replication":"https://pith.science/pith/BZEEEZZOLLI7AOEIATX5OQVREI/action/replication_record"}},"created_at":"2026-07-05T09:23:28.295777+00:00","updated_at":"2026-07-05T09:23:28.295777+00:00"}