{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:RQK355U7ZYXZ6M4ZMO4YPX5SSY","short_pith_number":"pith:RQK355U7","schema_version":"1.0","canonical_sha256":"8c15bef69fce2f9f339963b987dfb296190c41069ded506ab41bdc51761e219d","source":{"kind":"arxiv","id":"1210.8425","version":1},"attestation_state":"computed","paper":{"title":"Edge electrostatics revisited","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"A. Salman, A. Siddiki, M. B. Yucel","submitted_at":"2012-10-31T18:10:31Z","abstract_excerpt":"In this work we investigate in detail, the different regimes of the pioneering work of Chklovskii et al. (1992), which provides an analytical description to model the electrostatics at the edges of a two-dimensional electron gas. We take into account full electrostatics and calculate the charge distribution by solving the 3D Poisson equation self-consistently. The Chklovskii formalism is reintroduced and is employed to determine the widths of the incompressible edge-states also considering the spin degree of freedom. It is shown that, the odd integer filling fractions cannot exist for large ma"},"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":"1210.8425","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2012-10-31T18:10:31Z","cross_cats_sorted":[],"title_canon_sha256":"1c44e274f8fb0a3c1387500e141f08943ff3c7bcaecc64c30b7fbfcb9b31d0e5","abstract_canon_sha256":"6b865ef905a1aca64b84361cb9a0dc159113f9b62ecf1d269be44050c2d2dc91"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:53:28.713511Z","signature_b64":"Gj+u8bZkCZBrIEi77ik/WicMiVMZM6ijzSqy8TH9EwxAHEMvLuzWpslnaNR+2lkCOnQLm9BN5h8IPzOB0ZBhBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8c15bef69fce2f9f339963b987dfb296190c41069ded506ab41bdc51761e219d","last_reissued_at":"2026-05-18T01:53:28.712753Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:53:28.712753Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Edge electrostatics revisited","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"A. Salman, A. Siddiki, M. B. Yucel","submitted_at":"2012-10-31T18:10:31Z","abstract_excerpt":"In this work we investigate in detail, the different regimes of the pioneering work of Chklovskii et al. (1992), which provides an analytical description to model the electrostatics at the edges of a two-dimensional electron gas. We take into account full electrostatics and calculate the charge distribution by solving the 3D Poisson equation self-consistently. The Chklovskii formalism is reintroduced and is employed to determine the widths of the incompressible edge-states also considering the spin degree of freedom. It is shown that, the odd integer filling fractions cannot exist for large ma"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.8425","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":"1210.8425","created_at":"2026-05-18T01:53:28.712886+00:00"},{"alias_kind":"arxiv_version","alias_value":"1210.8425v1","created_at":"2026-05-18T01:53:28.712886+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.8425","created_at":"2026-05-18T01:53:28.712886+00:00"},{"alias_kind":"pith_short_12","alias_value":"RQK355U7ZYXZ","created_at":"2026-05-18T12:27:20.899486+00:00"},{"alias_kind":"pith_short_16","alias_value":"RQK355U7ZYXZ6M4Z","created_at":"2026-05-18T12:27:20.899486+00:00"},{"alias_kind":"pith_short_8","alias_value":"RQK355U7","created_at":"2026-05-18T12:27:20.899486+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/RQK355U7ZYXZ6M4ZMO4YPX5SSY","json":"https://pith.science/pith/RQK355U7ZYXZ6M4ZMO4YPX5SSY.json","graph_json":"https://pith.science/api/pith-number/RQK355U7ZYXZ6M4ZMO4YPX5SSY/graph.json","events_json":"https://pith.science/api/pith-number/RQK355U7ZYXZ6M4ZMO4YPX5SSY/events.json","paper":"https://pith.science/paper/RQK355U7"},"agent_actions":{"view_html":"https://pith.science/pith/RQK355U7ZYXZ6M4ZMO4YPX5SSY","download_json":"https://pith.science/pith/RQK355U7ZYXZ6M4ZMO4YPX5SSY.json","view_paper":"https://pith.science/paper/RQK355U7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1210.8425&json=true","fetch_graph":"https://pith.science/api/pith-number/RQK355U7ZYXZ6M4ZMO4YPX5SSY/graph.json","fetch_events":"https://pith.science/api/pith-number/RQK355U7ZYXZ6M4ZMO4YPX5SSY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RQK355U7ZYXZ6M4ZMO4YPX5SSY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RQK355U7ZYXZ6M4ZMO4YPX5SSY/action/storage_attestation","attest_author":"https://pith.science/pith/RQK355U7ZYXZ6M4ZMO4YPX5SSY/action/author_attestation","sign_citation":"https://pith.science/pith/RQK355U7ZYXZ6M4ZMO4YPX5SSY/action/citation_signature","submit_replication":"https://pith.science/pith/RQK355U7ZYXZ6M4ZMO4YPX5SSY/action/replication_record"}},"created_at":"2026-05-18T01:53:28.712886+00:00","updated_at":"2026-05-18T01:53:28.712886+00:00"}