{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:MPTMSDDZU5IL4XSEH76KEPVUSQ","short_pith_number":"pith:MPTMSDDZ","schema_version":"1.0","canonical_sha256":"63e6c90c79a750be5e443ffca23eb494145e9aa3bf743971500d7bc56cec244e","source":{"kind":"arxiv","id":"1201.3790","version":4},"attestation_state":"computed","paper":{"title":"Point-Contact spectroscopy on electron-doped Sr$_{0.88}$La$_{0.12}$CuO$_2$ thin films","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"F. Bouquet, L. Fruchter, Z. Z. Li","submitted_at":"2012-01-18T14:11:02Z","abstract_excerpt":"We report on the spectra of point-contacts made on Sr$_{0.88}$La$_{0.12}$CuO$_2$ thin films. Besides a clear evidence for the superconducting gap, we discuss the origin of specific features, such as resistance peaks at the gap voltage and the occurrence of a two-steps resistance decrease."},"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":"1201.3790","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2012-01-18T14:11:02Z","cross_cats_sorted":[],"title_canon_sha256":"41dea4fb56024242f375512b0694c49c688fcebbd90b8341ea9251a03c5ec2c0","abstract_canon_sha256":"79dd29aa617d1dc174727ad0257b637ae58d2d5fc41bbf629ea36f7311ed0511"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:50:37.410057Z","signature_b64":"roDbiTBGcNyLAdi+8BliYH1KILv3TV0Dl19u4acXXgkudQivlGtYkQDYvL6Q3Artw0IL+FLjW3o/W3UZmn/3Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"63e6c90c79a750be5e443ffca23eb494145e9aa3bf743971500d7bc56cec244e","last_reissued_at":"2026-05-18T03:50:37.409383Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:50:37.409383Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Point-Contact spectroscopy on electron-doped Sr$_{0.88}$La$_{0.12}$CuO$_2$ thin films","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"F. Bouquet, L. Fruchter, Z. Z. Li","submitted_at":"2012-01-18T14:11:02Z","abstract_excerpt":"We report on the spectra of point-contacts made on Sr$_{0.88}$La$_{0.12}$CuO$_2$ thin films. Besides a clear evidence for the superconducting gap, we discuss the origin of specific features, such as resistance peaks at the gap voltage and the occurrence of a two-steps resistance decrease."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.3790","kind":"arxiv","version":4},"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":"1201.3790","created_at":"2026-05-18T03:50:37.409477+00:00"},{"alias_kind":"arxiv_version","alias_value":"1201.3790v4","created_at":"2026-05-18T03:50:37.409477+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.3790","created_at":"2026-05-18T03:50:37.409477+00:00"},{"alias_kind":"pith_short_12","alias_value":"MPTMSDDZU5IL","created_at":"2026-05-18T12:27:14.488303+00:00"},{"alias_kind":"pith_short_16","alias_value":"MPTMSDDZU5IL4XSE","created_at":"2026-05-18T12:27:14.488303+00:00"},{"alias_kind":"pith_short_8","alias_value":"MPTMSDDZ","created_at":"2026-05-18T12:27:14.488303+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/MPTMSDDZU5IL4XSEH76KEPVUSQ","json":"https://pith.science/pith/MPTMSDDZU5IL4XSEH76KEPVUSQ.json","graph_json":"https://pith.science/api/pith-number/MPTMSDDZU5IL4XSEH76KEPVUSQ/graph.json","events_json":"https://pith.science/api/pith-number/MPTMSDDZU5IL4XSEH76KEPVUSQ/events.json","paper":"https://pith.science/paper/MPTMSDDZ"},"agent_actions":{"view_html":"https://pith.science/pith/MPTMSDDZU5IL4XSEH76KEPVUSQ","download_json":"https://pith.science/pith/MPTMSDDZU5IL4XSEH76KEPVUSQ.json","view_paper":"https://pith.science/paper/MPTMSDDZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1201.3790&json=true","fetch_graph":"https://pith.science/api/pith-number/MPTMSDDZU5IL4XSEH76KEPVUSQ/graph.json","fetch_events":"https://pith.science/api/pith-number/MPTMSDDZU5IL4XSEH76KEPVUSQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MPTMSDDZU5IL4XSEH76KEPVUSQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MPTMSDDZU5IL4XSEH76KEPVUSQ/action/storage_attestation","attest_author":"https://pith.science/pith/MPTMSDDZU5IL4XSEH76KEPVUSQ/action/author_attestation","sign_citation":"https://pith.science/pith/MPTMSDDZU5IL4XSEH76KEPVUSQ/action/citation_signature","submit_replication":"https://pith.science/pith/MPTMSDDZU5IL4XSEH76KEPVUSQ/action/replication_record"}},"created_at":"2026-05-18T03:50:37.409477+00:00","updated_at":"2026-05-18T03:50:37.409477+00:00"}