{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:VKAZ44WTM7H5JYCFAFXREVJSHF","short_pith_number":"pith:VKAZ44WT","schema_version":"1.0","canonical_sha256":"aa819e72d367cfd4e045016f1255323958f0b6cdfc8d15c1c4dd202887d75967","source":{"kind":"arxiv","id":"cond-mat/0111189","version":1},"attestation_state":"computed","paper":{"title":"Current transport in a superconducting superlattice system","license":"","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"Bor-Luen Huang, Chung-Yu Mou","submitted_at":"2001-11-10T06:49:34Z","abstract_excerpt":"We investigate the effect of the superlattice structure on the single particle transport along the c-axis of high temperature superconductors. In particular, superlattice systems that consists of metals/insulators and d-wave superconductors (NS/IS superlattice) are considered. We find that for the NS superlattice in the large mass anisotropy limit of the metal, the density of state in the low energy section is bulk d-wave like except that the position of the quasi-particle peak can be considerably smaller than the gap value, while for the IS superlattice, the quasi-particle peak remains at the"},"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/0111189","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.supr-con","submitted_at":"2001-11-10T06:49:34Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"4c4df7a8f155974333fd4589fc23e19e47a8c2570d675ad3a8143a089142b7e5","abstract_canon_sha256":"f2e05d29ceb2f80a5e9795fb3b13db98be7061fecf8f8742f1d437df6dc18ccb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:18:49.293176Z","signature_b64":"yQHonfky4hsojiI6uPgB4L1GOtW6nZKpg615Ljri72eJ7/exb7cHJS8KW9gaskenUt1pQqhQh2AJeGKmATiBBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aa819e72d367cfd4e045016f1255323958f0b6cdfc8d15c1c4dd202887d75967","last_reissued_at":"2026-07-04T14:18:49.292782Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:18:49.292782Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Current transport in a superconducting superlattice system","license":"","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"Bor-Luen Huang, Chung-Yu Mou","submitted_at":"2001-11-10T06:49:34Z","abstract_excerpt":"We investigate the effect of the superlattice structure on the single particle transport along the c-axis of high temperature superconductors. In particular, superlattice systems that consists of metals/insulators and d-wave superconductors (NS/IS superlattice) are considered. We find that for the NS superlattice in the large mass anisotropy limit of the metal, the density of state in the low energy section is bulk d-wave like except that the position of the quasi-particle peak can be considerably smaller than the gap value, while for the IS superlattice, the quasi-particle peak remains at the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0111189","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/cond-mat/0111189/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":"cond-mat/0111189","created_at":"2026-07-04T14:18:49.292838+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0111189v1","created_at":"2026-07-04T14:18:49.292838+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0111189","created_at":"2026-07-04T14:18:49.292838+00:00"},{"alias_kind":"pith_short_12","alias_value":"VKAZ44WTM7H5","created_at":"2026-07-04T14:18:49.292838+00:00"},{"alias_kind":"pith_short_16","alias_value":"VKAZ44WTM7H5JYCF","created_at":"2026-07-04T14:18:49.292838+00:00"},{"alias_kind":"pith_short_8","alias_value":"VKAZ44WT","created_at":"2026-07-04T14:18:49.292838+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/VKAZ44WTM7H5JYCFAFXREVJSHF","json":"https://pith.science/pith/VKAZ44WTM7H5JYCFAFXREVJSHF.json","graph_json":"https://pith.science/api/pith-number/VKAZ44WTM7H5JYCFAFXREVJSHF/graph.json","events_json":"https://pith.science/api/pith-number/VKAZ44WTM7H5JYCFAFXREVJSHF/events.json","paper":"https://pith.science/paper/VKAZ44WT"},"agent_actions":{"view_html":"https://pith.science/pith/VKAZ44WTM7H5JYCFAFXREVJSHF","download_json":"https://pith.science/pith/VKAZ44WTM7H5JYCFAFXREVJSHF.json","view_paper":"https://pith.science/paper/VKAZ44WT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/0111189&json=true","fetch_graph":"https://pith.science/api/pith-number/VKAZ44WTM7H5JYCFAFXREVJSHF/graph.json","fetch_events":"https://pith.science/api/pith-number/VKAZ44WTM7H5JYCFAFXREVJSHF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VKAZ44WTM7H5JYCFAFXREVJSHF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VKAZ44WTM7H5JYCFAFXREVJSHF/action/storage_attestation","attest_author":"https://pith.science/pith/VKAZ44WTM7H5JYCFAFXREVJSHF/action/author_attestation","sign_citation":"https://pith.science/pith/VKAZ44WTM7H5JYCFAFXREVJSHF/action/citation_signature","submit_replication":"https://pith.science/pith/VKAZ44WTM7H5JYCFAFXREVJSHF/action/replication_record"}},"created_at":"2026-07-04T14:18:49.292838+00:00","updated_at":"2026-07-04T14:18:49.292838+00:00"}