{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:LBBW23MZ3FFF2MYN2UB6DQCAWS","short_pith_number":"pith:LBBW23MZ","schema_version":"1.0","canonical_sha256":"58436d6d99d94a5d330dd503e1c040b4937548383bd744f1edceb04f0e1ae8e7","source":{"kind":"arxiv","id":"1412.1678","version":5},"attestation_state":"computed","paper":{"title":"Acoustomagnetoelectric Effect in Graphene Nanoribbon in the Presence of External Electric and Magnetic Field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"H. A. Quaye, K. A. Dompreh, N. G. Mensah, R. Edziah, S. S. Abukari, S. Y. Mensah","submitted_at":"2014-12-04T14:30:16Z","abstract_excerpt":"The Acoustomagnetoelectric Effect (AME) in Graphene Nanoribbon (GNR) was theoretically studied using the Boltzmann kinetic equation. On open circuit, the general formular for Surface Acoustomagnetoelectric field ($\\vec{E}_{SAME}$) in GNR with energy dispersion $\\varepsilon(p)$ near the Fermi point was calculated. The $E_{SAME}$ was found to depend on the magnetic strength ($\\eta$), $\\alpha$ = ${\\hbar \\omega_q}/{E_g}$ and the energy gap ($E_g$). The expression for $\\vec{E}_{SAME}$ was analyzed numerically for varying width of GNR, magnetic strength ($\\eta$) and $\\alpha$ at different sub-bands i"},"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":"1412.1678","kind":"arxiv","version":5},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2014-12-04T14:30:16Z","cross_cats_sorted":[],"title_canon_sha256":"2034efa5b6dab7b0b6585b28ac89af45d6286ea4885c680cca268a94b1503bfb","abstract_canon_sha256":"971796d053d67fe302b6bf785cb8f569572d739a186f2e80ff26ee8a35587957"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:05:24.044830Z","signature_b64":"5HpgzEiI4V/lIkc4ifgrKQ7ET5s2BPMlSdRHA/jFohQ2jG4ABds8mmGbQk2IUnY4xftddMR3uqhDxaTajI94Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"58436d6d99d94a5d330dd503e1c040b4937548383bd744f1edceb04f0e1ae8e7","last_reissued_at":"2026-05-18T02:05:24.044121Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:05:24.044121Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Acoustomagnetoelectric Effect in Graphene Nanoribbon in the Presence of External Electric and Magnetic Field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"H. A. Quaye, K. A. Dompreh, N. G. Mensah, R. Edziah, S. S. Abukari, S. Y. Mensah","submitted_at":"2014-12-04T14:30:16Z","abstract_excerpt":"The Acoustomagnetoelectric Effect (AME) in Graphene Nanoribbon (GNR) was theoretically studied using the Boltzmann kinetic equation. On open circuit, the general formular for Surface Acoustomagnetoelectric field ($\\vec{E}_{SAME}$) in GNR with energy dispersion $\\varepsilon(p)$ near the Fermi point was calculated. The $E_{SAME}$ was found to depend on the magnetic strength ($\\eta$), $\\alpha$ = ${\\hbar \\omega_q}/{E_g}$ and the energy gap ($E_g$). The expression for $\\vec{E}_{SAME}$ was analyzed numerically for varying width of GNR, magnetic strength ($\\eta$) and $\\alpha$ at different sub-bands i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.1678","kind":"arxiv","version":5},"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":"1412.1678","created_at":"2026-05-18T02:05:24.044208+00:00"},{"alias_kind":"arxiv_version","alias_value":"1412.1678v5","created_at":"2026-05-18T02:05:24.044208+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.1678","created_at":"2026-05-18T02:05:24.044208+00:00"},{"alias_kind":"pith_short_12","alias_value":"LBBW23MZ3FFF","created_at":"2026-05-18T12:28:35.611951+00:00"},{"alias_kind":"pith_short_16","alias_value":"LBBW23MZ3FFF2MYN","created_at":"2026-05-18T12:28:35.611951+00:00"},{"alias_kind":"pith_short_8","alias_value":"LBBW23MZ","created_at":"2026-05-18T12:28:35.611951+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/LBBW23MZ3FFF2MYN2UB6DQCAWS","json":"https://pith.science/pith/LBBW23MZ3FFF2MYN2UB6DQCAWS.json","graph_json":"https://pith.science/api/pith-number/LBBW23MZ3FFF2MYN2UB6DQCAWS/graph.json","events_json":"https://pith.science/api/pith-number/LBBW23MZ3FFF2MYN2UB6DQCAWS/events.json","paper":"https://pith.science/paper/LBBW23MZ"},"agent_actions":{"view_html":"https://pith.science/pith/LBBW23MZ3FFF2MYN2UB6DQCAWS","download_json":"https://pith.science/pith/LBBW23MZ3FFF2MYN2UB6DQCAWS.json","view_paper":"https://pith.science/paper/LBBW23MZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1412.1678&json=true","fetch_graph":"https://pith.science/api/pith-number/LBBW23MZ3FFF2MYN2UB6DQCAWS/graph.json","fetch_events":"https://pith.science/api/pith-number/LBBW23MZ3FFF2MYN2UB6DQCAWS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LBBW23MZ3FFF2MYN2UB6DQCAWS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LBBW23MZ3FFF2MYN2UB6DQCAWS/action/storage_attestation","attest_author":"https://pith.science/pith/LBBW23MZ3FFF2MYN2UB6DQCAWS/action/author_attestation","sign_citation":"https://pith.science/pith/LBBW23MZ3FFF2MYN2UB6DQCAWS/action/citation_signature","submit_replication":"https://pith.science/pith/LBBW23MZ3FFF2MYN2UB6DQCAWS/action/replication_record"}},"created_at":"2026-05-18T02:05:24.044208+00:00","updated_at":"2026-05-18T02:05:24.044208+00:00"}