{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:AUXPJCM23K357T24EIHM6EWPNH","short_pith_number":"pith:AUXPJCM2","schema_version":"1.0","canonical_sha256":"052ef4899adab7dfcf5c220ecf12cf69f4744d036532c37280c5a0761f4e7986","source":{"kind":"arxiv","id":"1507.08955","version":1},"attestation_state":"computed","paper":{"title":"Confinement of superconducting fluctuations due to emergent electronic inhomogeneities","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"B. Leridon, B. Vignolle, C. Brun, C. Carbillet, D. Demaille, D. Roditchev, F. Debontridder, K. Ilin, L. Largeau, M. Grilli, M. Siegel, S. Caprara, T. Cren, W. Tabis","submitted_at":"2015-07-31T17:39:35Z","abstract_excerpt":"The microscopic nature of an insulating state in the vicinity of a superconducting state, in the presence of disorder, is a hotly debated question. While the simplest scenario proposes that Coulomb interactions destroy the Cooper pairs at the transition, leading to localization of single electrons, an alternate possibility supported by experimental observations suggests that Cooper pairs instead directly localize. The question of the homogeneity, granularity, or possibly glassiness of the material on the verge of this transition is intimately related to this fundamental issue. Here, by combini"},"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":"1507.08955","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2015-07-31T17:39:35Z","cross_cats_sorted":[],"title_canon_sha256":"2876ca8beac74df64d7223a45cd14a83d0bd749cfe47ad161bb5294461cc906f","abstract_canon_sha256":"a38ceeb8f046a1ae7ae4abd728ca19b604a9f2b188a1eed10c191ec035f9cda1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:16:49.610803Z","signature_b64":"j4SpBZ/f4rHrz1z67YnvEzkDO/f1tFH5dX140AqSBZjqdD/qfK8sZ7Xm18O/WL4lXOMlRjFnAZtvaoU8Gr5wBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"052ef4899adab7dfcf5c220ecf12cf69f4744d036532c37280c5a0761f4e7986","last_reissued_at":"2026-05-18T01:16:49.610078Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:16:49.610078Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Confinement of superconducting fluctuations due to emergent electronic inhomogeneities","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"B. Leridon, B. Vignolle, C. Brun, C. Carbillet, D. Demaille, D. Roditchev, F. Debontridder, K. Ilin, L. Largeau, M. Grilli, M. Siegel, S. Caprara, T. Cren, W. Tabis","submitted_at":"2015-07-31T17:39:35Z","abstract_excerpt":"The microscopic nature of an insulating state in the vicinity of a superconducting state, in the presence of disorder, is a hotly debated question. While the simplest scenario proposes that Coulomb interactions destroy the Cooper pairs at the transition, leading to localization of single electrons, an alternate possibility supported by experimental observations suggests that Cooper pairs instead directly localize. The question of the homogeneity, granularity, or possibly glassiness of the material on the verge of this transition is intimately related to this fundamental issue. Here, by combini"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.08955","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":"1507.08955","created_at":"2026-05-18T01:16:49.610192+00:00"},{"alias_kind":"arxiv_version","alias_value":"1507.08955v1","created_at":"2026-05-18T01:16:49.610192+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.08955","created_at":"2026-05-18T01:16:49.610192+00:00"},{"alias_kind":"pith_short_12","alias_value":"AUXPJCM23K35","created_at":"2026-05-18T12:29:10.953037+00:00"},{"alias_kind":"pith_short_16","alias_value":"AUXPJCM23K357T24","created_at":"2026-05-18T12:29:10.953037+00:00"},{"alias_kind":"pith_short_8","alias_value":"AUXPJCM2","created_at":"2026-05-18T12:29:10.953037+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/AUXPJCM23K357T24EIHM6EWPNH","json":"https://pith.science/pith/AUXPJCM23K357T24EIHM6EWPNH.json","graph_json":"https://pith.science/api/pith-number/AUXPJCM23K357T24EIHM6EWPNH/graph.json","events_json":"https://pith.science/api/pith-number/AUXPJCM23K357T24EIHM6EWPNH/events.json","paper":"https://pith.science/paper/AUXPJCM2"},"agent_actions":{"view_html":"https://pith.science/pith/AUXPJCM23K357T24EIHM6EWPNH","download_json":"https://pith.science/pith/AUXPJCM23K357T24EIHM6EWPNH.json","view_paper":"https://pith.science/paper/AUXPJCM2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1507.08955&json=true","fetch_graph":"https://pith.science/api/pith-number/AUXPJCM23K357T24EIHM6EWPNH/graph.json","fetch_events":"https://pith.science/api/pith-number/AUXPJCM23K357T24EIHM6EWPNH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AUXPJCM23K357T24EIHM6EWPNH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AUXPJCM23K357T24EIHM6EWPNH/action/storage_attestation","attest_author":"https://pith.science/pith/AUXPJCM23K357T24EIHM6EWPNH/action/author_attestation","sign_citation":"https://pith.science/pith/AUXPJCM23K357T24EIHM6EWPNH/action/citation_signature","submit_replication":"https://pith.science/pith/AUXPJCM23K357T24EIHM6EWPNH/action/replication_record"}},"created_at":"2026-05-18T01:16:49.610192+00:00","updated_at":"2026-05-18T01:16:49.610192+00:00"}