{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:N3DWOZW3D74ILCRCRCNZEVYJPV","short_pith_number":"pith:N3DWOZW3","schema_version":"1.0","canonical_sha256":"6ec76766db1ff8858a22889b9257097d6864ffe84f5148f7984a21332847b051","source":{"kind":"arxiv","id":"1805.09574","version":1},"attestation_state":"computed","paper":{"title":"Vortex excitations in the Insulating State of an Oxide Interface","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"D. Graf, E. Maniv, J. -H Park, M. Mograbi, P. K. Rout, Y. Dagan","submitted_at":"2018-05-24T09:46:06Z","abstract_excerpt":"In two-dimensional (2D) superconductors an insulating state can be induced either by applying a magnetic field, $H$, or by increasing disorder. Many scenarios have been put forth to explain the superconductor to insulator transition (SIT): dominating fermionic physics after the breaking of Cooper pairs, loss of phase coherence between superconducting islands embedded in a metallic or insulating matrix and localization of Cooper pairs with concomitant condensation of vortex-type excitations. The difficulty in characterizing the insulating state and its origin stems from the lack of a continuous"},"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":"1805.09574","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2018-05-24T09:46:06Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.str-el"],"title_canon_sha256":"90d4ffd9fd3f219cca1aa6aa1694dda8ea6c2a8432038f785205eba8ffe39655","abstract_canon_sha256":"78df21fb0bdf112602e96e78d99260ea032207f7239f0744f42fcdd3190dba5a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:50:13.623783Z","signature_b64":"rqp7o/x+Kh/q3nkGLYpK0KHWWoHr3g05kE0vBHPFqkvSSdrr1XXRllw4SzLXrBRjCf+irzfmMcUhxci/qtjrBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6ec76766db1ff8858a22889b9257097d6864ffe84f5148f7984a21332847b051","last_reissued_at":"2026-05-17T23:50:13.623230Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:50:13.623230Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Vortex excitations in the Insulating State of an Oxide Interface","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"D. Graf, E. Maniv, J. -H Park, M. Mograbi, P. K. Rout, Y. Dagan","submitted_at":"2018-05-24T09:46:06Z","abstract_excerpt":"In two-dimensional (2D) superconductors an insulating state can be induced either by applying a magnetic field, $H$, or by increasing disorder. Many scenarios have been put forth to explain the superconductor to insulator transition (SIT): dominating fermionic physics after the breaking of Cooper pairs, loss of phase coherence between superconducting islands embedded in a metallic or insulating matrix and localization of Cooper pairs with concomitant condensation of vortex-type excitations. The difficulty in characterizing the insulating state and its origin stems from the lack of a continuous"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.09574","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":"1805.09574","created_at":"2026-05-17T23:50:13.623308+00:00"},{"alias_kind":"arxiv_version","alias_value":"1805.09574v1","created_at":"2026-05-17T23:50:13.623308+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.09574","created_at":"2026-05-17T23:50:13.623308+00:00"},{"alias_kind":"pith_short_12","alias_value":"N3DWOZW3D74I","created_at":"2026-05-18T12:32:40.477152+00:00"},{"alias_kind":"pith_short_16","alias_value":"N3DWOZW3D74ILCRC","created_at":"2026-05-18T12:32:40.477152+00:00"},{"alias_kind":"pith_short_8","alias_value":"N3DWOZW3","created_at":"2026-05-18T12:32:40.477152+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/N3DWOZW3D74ILCRCRCNZEVYJPV","json":"https://pith.science/pith/N3DWOZW3D74ILCRCRCNZEVYJPV.json","graph_json":"https://pith.science/api/pith-number/N3DWOZW3D74ILCRCRCNZEVYJPV/graph.json","events_json":"https://pith.science/api/pith-number/N3DWOZW3D74ILCRCRCNZEVYJPV/events.json","paper":"https://pith.science/paper/N3DWOZW3"},"agent_actions":{"view_html":"https://pith.science/pith/N3DWOZW3D74ILCRCRCNZEVYJPV","download_json":"https://pith.science/pith/N3DWOZW3D74ILCRCRCNZEVYJPV.json","view_paper":"https://pith.science/paper/N3DWOZW3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1805.09574&json=true","fetch_graph":"https://pith.science/api/pith-number/N3DWOZW3D74ILCRCRCNZEVYJPV/graph.json","fetch_events":"https://pith.science/api/pith-number/N3DWOZW3D74ILCRCRCNZEVYJPV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/N3DWOZW3D74ILCRCRCNZEVYJPV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/N3DWOZW3D74ILCRCRCNZEVYJPV/action/storage_attestation","attest_author":"https://pith.science/pith/N3DWOZW3D74ILCRCRCNZEVYJPV/action/author_attestation","sign_citation":"https://pith.science/pith/N3DWOZW3D74ILCRCRCNZEVYJPV/action/citation_signature","submit_replication":"https://pith.science/pith/N3DWOZW3D74ILCRCRCNZEVYJPV/action/replication_record"}},"created_at":"2026-05-17T23:50:13.623308+00:00","updated_at":"2026-05-17T23:50:13.623308+00:00"}