{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:RT47PQV5OJMLB36QUUAUNCUXPV","short_pith_number":"pith:RT47PQV5","schema_version":"1.0","canonical_sha256":"8cf9f7c2bd7258b0efd0a501468a977d52123ddd60848f7af7f3106dfba2e471","source":{"kind":"arxiv","id":"1710.09863","version":2},"attestation_state":"computed","paper":{"title":"Growth and structural characterization of large superconducting crystals of La$_{2-x}$Ca$_{1+x}$Cu$_2$O$_{6}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"G. D. Gu, Guangyong Xu, J. A. Schneeloch, J. M. Tranquada, K. M. Mohanty, M. B. Stone, Ruidan Zhong, Wei Tian, Z. Guguchia","submitted_at":"2017-10-26T18:42:52Z","abstract_excerpt":"Large crystals of La$_{2-x}$Ca$_{1+x}$Cu$_2$O$_{6}$ (La-Ca-2126) with $x=0.10$ and 0.15 have been grown and converted to bulk superconductors by high-pressure oxygen annealing. The superconducting transition temperature, $T_c$, is as high as 55~K; this can be raised to 60~K by post-annealing in air. Here we present structural and magnetic characterizations of these crystals using neutron scattering and muon spin rotation techniques. While the as-grown, non-superconducting crystals are single phase, we find that the superconducting crystals contain 3 phases forming coherent domains stacked alon"},"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":"1710.09863","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2017-10-26T18:42:52Z","cross_cats_sorted":[],"title_canon_sha256":"29587b109e3924a504c78a79171cc2c0d9d704c21e916b50d6e53ee6accdf401","abstract_canon_sha256":"79925cb9432370dc49db3d09a5a82902dade36b534768e0e0da1983a67266a09"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:28:40.254034Z","signature_b64":"JmNqmxMGGsxuacjdfvoKA8ZF5pLKYt5WjVP1c38a34eIZzGDcg1VRvaIxcDDLEYuKSgptCGLhtmE4hYCF0vPCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8cf9f7c2bd7258b0efd0a501468a977d52123ddd60848f7af7f3106dfba2e471","last_reissued_at":"2026-05-18T00:28:40.253252Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:28:40.253252Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Growth and structural characterization of large superconducting crystals of La$_{2-x}$Ca$_{1+x}$Cu$_2$O$_{6}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"G. D. Gu, Guangyong Xu, J. A. Schneeloch, J. M. Tranquada, K. M. Mohanty, M. B. Stone, Ruidan Zhong, Wei Tian, Z. Guguchia","submitted_at":"2017-10-26T18:42:52Z","abstract_excerpt":"Large crystals of La$_{2-x}$Ca$_{1+x}$Cu$_2$O$_{6}$ (La-Ca-2126) with $x=0.10$ and 0.15 have been grown and converted to bulk superconductors by high-pressure oxygen annealing. The superconducting transition temperature, $T_c$, is as high as 55~K; this can be raised to 60~K by post-annealing in air. Here we present structural and magnetic characterizations of these crystals using neutron scattering and muon spin rotation techniques. While the as-grown, non-superconducting crystals are single phase, we find that the superconducting crystals contain 3 phases forming coherent domains stacked alon"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.09863","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":"1710.09863","created_at":"2026-05-18T00:28:40.253395+00:00"},{"alias_kind":"arxiv_version","alias_value":"1710.09863v2","created_at":"2026-05-18T00:28:40.253395+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.09863","created_at":"2026-05-18T00:28:40.253395+00:00"},{"alias_kind":"pith_short_12","alias_value":"RT47PQV5OJML","created_at":"2026-05-18T12:31:39.905425+00:00"},{"alias_kind":"pith_short_16","alias_value":"RT47PQV5OJMLB36Q","created_at":"2026-05-18T12:31:39.905425+00:00"},{"alias_kind":"pith_short_8","alias_value":"RT47PQV5","created_at":"2026-05-18T12:31:39.905425+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/RT47PQV5OJMLB36QUUAUNCUXPV","json":"https://pith.science/pith/RT47PQV5OJMLB36QUUAUNCUXPV.json","graph_json":"https://pith.science/api/pith-number/RT47PQV5OJMLB36QUUAUNCUXPV/graph.json","events_json":"https://pith.science/api/pith-number/RT47PQV5OJMLB36QUUAUNCUXPV/events.json","paper":"https://pith.science/paper/RT47PQV5"},"agent_actions":{"view_html":"https://pith.science/pith/RT47PQV5OJMLB36QUUAUNCUXPV","download_json":"https://pith.science/pith/RT47PQV5OJMLB36QUUAUNCUXPV.json","view_paper":"https://pith.science/paper/RT47PQV5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1710.09863&json=true","fetch_graph":"https://pith.science/api/pith-number/RT47PQV5OJMLB36QUUAUNCUXPV/graph.json","fetch_events":"https://pith.science/api/pith-number/RT47PQV5OJMLB36QUUAUNCUXPV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RT47PQV5OJMLB36QUUAUNCUXPV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RT47PQV5OJMLB36QUUAUNCUXPV/action/storage_attestation","attest_author":"https://pith.science/pith/RT47PQV5OJMLB36QUUAUNCUXPV/action/author_attestation","sign_citation":"https://pith.science/pith/RT47PQV5OJMLB36QUUAUNCUXPV/action/citation_signature","submit_replication":"https://pith.science/pith/RT47PQV5OJMLB36QUUAUNCUXPV/action/replication_record"}},"created_at":"2026-05-18T00:28:40.253395+00:00","updated_at":"2026-05-18T00:28:40.253395+00:00"}