{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:TX7QTMMJYIXWUTSRSLSAHH6S2M","short_pith_number":"pith:TX7QTMMJ","schema_version":"1.0","canonical_sha256":"9dff09b189c22f6a4e5192e4039fd2d3323697642afc1eb2997624f2cc6e7b1e","source":{"kind":"arxiv","id":"1206.6786","version":2},"attestation_state":"computed","paper":{"title":"Type-1.5 superconductivity in muliband and other multicomponent systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Egor Babaev, Mihail Silaev","submitted_at":"2012-06-28T18:22:24Z","abstract_excerpt":"Usual superconductors are classified into two categories as follows: type-1 when the ratio of the magnetic field penetration length (\\lambda) to coherence length (\\xi) with Ginzburg-Landau parameter \\kappa=\\lambda/\\xi <1/\\sqrt{2} and type-2 when \\kappa >1/\\sqrt{2}. The boundary case \\kappa =1/\\sqrt{2} is also considered to be a special situation, frequently termed as \"Bogomolnyi limit\". Here we discuss multicomponent systems which can possess three or more fundamental length scales and allow a separate superconducting state, which was recently termed \"type-1.5\". In that state a system has 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":"1206.6786","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2012-06-28T18:22:24Z","cross_cats_sorted":[],"title_canon_sha256":"d9ebf2fbbe96687e469dc836fc86ba1588b52078b93a4236423f58858b30f6f9","abstract_canon_sha256":"977210cd2397c79a8bae79f28138e3cb42f9b174544d94cb6bcd221f9464d674"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:27:34.436061Z","signature_b64":"NNqesaOPXenjrNo6+BGR0GTBuEMLGZovEqZg8sgO0IdbHKM7MQUfziHSTmpfhE9GeJLx/on47e6RbqWt7Kw5Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9dff09b189c22f6a4e5192e4039fd2d3323697642afc1eb2997624f2cc6e7b1e","last_reissued_at":"2026-05-18T03:27:34.435533Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:27:34.435533Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Type-1.5 superconductivity in muliband and other multicomponent systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Egor Babaev, Mihail Silaev","submitted_at":"2012-06-28T18:22:24Z","abstract_excerpt":"Usual superconductors are classified into two categories as follows: type-1 when the ratio of the magnetic field penetration length (\\lambda) to coherence length (\\xi) with Ginzburg-Landau parameter \\kappa=\\lambda/\\xi <1/\\sqrt{2} and type-2 when \\kappa >1/\\sqrt{2}. The boundary case \\kappa =1/\\sqrt{2} is also considered to be a special situation, frequently termed as \"Bogomolnyi limit\". Here we discuss multicomponent systems which can possess three or more fundamental length scales and allow a separate superconducting state, which was recently termed \"type-1.5\". In that state a system has the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1206.6786","kind":"arxiv","version":2},"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":"1206.6786","created_at":"2026-05-18T03:27:34.435587+00:00"},{"alias_kind":"arxiv_version","alias_value":"1206.6786v2","created_at":"2026-05-18T03:27:34.435587+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1206.6786","created_at":"2026-05-18T03:27:34.435587+00:00"},{"alias_kind":"pith_short_12","alias_value":"TX7QTMMJYIXW","created_at":"2026-05-18T12:27:23.164592+00:00"},{"alias_kind":"pith_short_16","alias_value":"TX7QTMMJYIXWUTSR","created_at":"2026-05-18T12:27:23.164592+00:00"},{"alias_kind":"pith_short_8","alias_value":"TX7QTMMJ","created_at":"2026-05-18T12:27:23.164592+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/TX7QTMMJYIXWUTSRSLSAHH6S2M","json":"https://pith.science/pith/TX7QTMMJYIXWUTSRSLSAHH6S2M.json","graph_json":"https://pith.science/api/pith-number/TX7QTMMJYIXWUTSRSLSAHH6S2M/graph.json","events_json":"https://pith.science/api/pith-number/TX7QTMMJYIXWUTSRSLSAHH6S2M/events.json","paper":"https://pith.science/paper/TX7QTMMJ"},"agent_actions":{"view_html":"https://pith.science/pith/TX7QTMMJYIXWUTSRSLSAHH6S2M","download_json":"https://pith.science/pith/TX7QTMMJYIXWUTSRSLSAHH6S2M.json","view_paper":"https://pith.science/paper/TX7QTMMJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1206.6786&json=true","fetch_graph":"https://pith.science/api/pith-number/TX7QTMMJYIXWUTSRSLSAHH6S2M/graph.json","fetch_events":"https://pith.science/api/pith-number/TX7QTMMJYIXWUTSRSLSAHH6S2M/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TX7QTMMJYIXWUTSRSLSAHH6S2M/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TX7QTMMJYIXWUTSRSLSAHH6S2M/action/storage_attestation","attest_author":"https://pith.science/pith/TX7QTMMJYIXWUTSRSLSAHH6S2M/action/author_attestation","sign_citation":"https://pith.science/pith/TX7QTMMJYIXWUTSRSLSAHH6S2M/action/citation_signature","submit_replication":"https://pith.science/pith/TX7QTMMJYIXWUTSRSLSAHH6S2M/action/replication_record"}},"created_at":"2026-05-18T03:27:34.435587+00:00","updated_at":"2026-05-18T03:27:34.435587+00:00"}