{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:OL7QSVROGOIUG2NOXS65WNVE22","short_pith_number":"pith:OL7QSVRO","schema_version":"1.0","canonical_sha256":"72ff09562e33914369aebcbddb36a4d68ebc981a7a678c343406fb77bd5ad696","source":{"kind":"arxiv","id":"cond-mat/9607042","version":1},"attestation_state":"computed","paper":{"title":"Statistics of Mesoscopic Fluctuations of Quantum Capacitance","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat","authors_text":"A. M. Jayannavar, N. Kumar","submitted_at":"1996-07-05T07:28:17Z","abstract_excerpt":"The Thouless formula \\(G = (e^2/h)(E_c/\\Delta)\\) for the two-probe dc conductance $G$ of a d-dimensional mesoscopic cube is re-analysed to relate its quantum capacitance $C_Q$ to the reciprocal of the level spacing $\\Delta$. To this end, the escape time-scale $\\tau$ occurring in the Thouless correlation energy \\(E_c = \\hbar/\\tau\\) is interpreted as the {\\em time constant} \\(\\tau = RC_Q\\) with $RG \\equiv$ 1, giving at once \\(C_Q = (e^2/2\\pi \\Delta)\\). Thus, the statistics of the quantum capacitance is directly related to that of the level spacing, which is well known from the Random Matrix Theo"},"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":"cond-mat/9607042","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat","submitted_at":"1996-07-05T07:28:17Z","cross_cats_sorted":[],"title_canon_sha256":"30c0998d0ab80cf6984e1a1aaf3d17d1f5bae8ce2412a9be33c9cad6b1456b93","abstract_canon_sha256":"a9485b0b95fec4c205ba8a2f20061c41aa65bd9292216eba5639e1a2e7dacf28"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:39:34.157785Z","signature_b64":"0VR1vE/W1hKgbtMoCNpg6a1IK2wIgzTaeiW5b9ARC2bCghiaTkkJqQwawSt7eoTOgwzGe8oqdmVFQFeq50tJAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"72ff09562e33914369aebcbddb36a4d68ebc981a7a678c343406fb77bd5ad696","last_reissued_at":"2026-05-18T01:39:34.157214Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:39:34.157214Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Statistics of Mesoscopic Fluctuations of Quantum Capacitance","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat","authors_text":"A. M. Jayannavar, N. Kumar","submitted_at":"1996-07-05T07:28:17Z","abstract_excerpt":"The Thouless formula \\(G = (e^2/h)(E_c/\\Delta)\\) for the two-probe dc conductance $G$ of a d-dimensional mesoscopic cube is re-analysed to relate its quantum capacitance $C_Q$ to the reciprocal of the level spacing $\\Delta$. To this end, the escape time-scale $\\tau$ occurring in the Thouless correlation energy \\(E_c = \\hbar/\\tau\\) is interpreted as the {\\em time constant} \\(\\tau = RC_Q\\) with $RG \\equiv$ 1, giving at once \\(C_Q = (e^2/2\\pi \\Delta)\\). Thus, the statistics of the quantum capacitance is directly related to that of the level spacing, which is well known from the Random Matrix Theo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9607042","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":"cond-mat/9607042","created_at":"2026-05-18T01:39:34.157305+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9607042v1","created_at":"2026-05-18T01:39:34.157305+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9607042","created_at":"2026-05-18T01:39:34.157305+00:00"},{"alias_kind":"pith_short_12","alias_value":"OL7QSVROGOIU","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_16","alias_value":"OL7QSVROGOIUG2NO","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_8","alias_value":"OL7QSVRO","created_at":"2026-05-18T12:25:48.327863+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/OL7QSVROGOIUG2NOXS65WNVE22","json":"https://pith.science/pith/OL7QSVROGOIUG2NOXS65WNVE22.json","graph_json":"https://pith.science/api/pith-number/OL7QSVROGOIUG2NOXS65WNVE22/graph.json","events_json":"https://pith.science/api/pith-number/OL7QSVROGOIUG2NOXS65WNVE22/events.json","paper":"https://pith.science/paper/OL7QSVRO"},"agent_actions":{"view_html":"https://pith.science/pith/OL7QSVROGOIUG2NOXS65WNVE22","download_json":"https://pith.science/pith/OL7QSVROGOIUG2NOXS65WNVE22.json","view_paper":"https://pith.science/paper/OL7QSVRO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/9607042&json=true","fetch_graph":"https://pith.science/api/pith-number/OL7QSVROGOIUG2NOXS65WNVE22/graph.json","fetch_events":"https://pith.science/api/pith-number/OL7QSVROGOIUG2NOXS65WNVE22/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OL7QSVROGOIUG2NOXS65WNVE22/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OL7QSVROGOIUG2NOXS65WNVE22/action/storage_attestation","attest_author":"https://pith.science/pith/OL7QSVROGOIUG2NOXS65WNVE22/action/author_attestation","sign_citation":"https://pith.science/pith/OL7QSVROGOIUG2NOXS65WNVE22/action/citation_signature","submit_replication":"https://pith.science/pith/OL7QSVROGOIUG2NOXS65WNVE22/action/replication_record"}},"created_at":"2026-05-18T01:39:34.157305+00:00","updated_at":"2026-05-18T01:39:34.157305+00:00"}