{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:5WXPUMGTAIHW6FJVFTP3RE6LAQ","short_pith_number":"pith:5WXPUMGT","schema_version":"1.0","canonical_sha256":"edaefa30d3020f6f15352cdfb893cb041a76a326215da161d6fe2a5c11bb85bf","source":{"kind":"arxiv","id":"1509.05541","version":1},"attestation_state":"computed","paper":{"title":"Simulation of Stacks of High Temperature Superconducting Coated Conductors Magnetized by Pulsed Field Magnetization Using Controlled Magnetic Density Distribution Coils","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Francesco Grilli, Shengnan Zou, Victor Manuel Rodriguez Zermeno","submitted_at":"2015-09-18T08:31:43Z","abstract_excerpt":"High temperature superconducting (HTS) stacks of coated conductors (CCs) can work as strong trapped field magnets (TFMs) and show potential in electrical applications. Pulsed field magnetization (PFM) is a practical method to magnetize such TFMs, but due to heat generation during the dynamic process, it cannot achieve a trapped field as high as field cooling can. In this work, we construct a 2D electromagnetic-thermal coupled model to simulate stacks of HTS CCs with realistic laminated structures magnetized by PFM. The model considers temperature and anisotropic magnetic field dependent Jc of "},"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":"1509.05541","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2015-09-18T08:31:43Z","cross_cats_sorted":[],"title_canon_sha256":"cb179c717afda7a91af7acd4110b75010d9f271c130749d2a751f5fcafde4b2b","abstract_canon_sha256":"a578b5519c7bd4db452855f63466af0e54f9b9f1f36e36f45b61eba3fd0ca127"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:11:44.270878Z","signature_b64":"3cVg5z46szpzUfafCJjFZgi07cIbUR5wgkZxq6COc19lEQtRSdf5bWZ6onZmS8orqx9sf8M3myDmI1K0QWLwDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"edaefa30d3020f6f15352cdfb893cb041a76a326215da161d6fe2a5c11bb85bf","last_reissued_at":"2026-05-18T00:11:44.270153Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:11:44.270153Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Simulation of Stacks of High Temperature Superconducting Coated Conductors Magnetized by Pulsed Field Magnetization Using Controlled Magnetic Density Distribution Coils","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Francesco Grilli, Shengnan Zou, Victor Manuel Rodriguez Zermeno","submitted_at":"2015-09-18T08:31:43Z","abstract_excerpt":"High temperature superconducting (HTS) stacks of coated conductors (CCs) can work as strong trapped field magnets (TFMs) and show potential in electrical applications. Pulsed field magnetization (PFM) is a practical method to magnetize such TFMs, but due to heat generation during the dynamic process, it cannot achieve a trapped field as high as field cooling can. In this work, we construct a 2D electromagnetic-thermal coupled model to simulate stacks of HTS CCs with realistic laminated structures magnetized by PFM. The model considers temperature and anisotropic magnetic field dependent Jc of "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.05541","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":"1509.05541","created_at":"2026-05-18T00:11:44.270265+00:00"},{"alias_kind":"arxiv_version","alias_value":"1509.05541v1","created_at":"2026-05-18T00:11:44.270265+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.05541","created_at":"2026-05-18T00:11:44.270265+00:00"},{"alias_kind":"pith_short_12","alias_value":"5WXPUMGTAIHW","created_at":"2026-05-18T12:29:07.941421+00:00"},{"alias_kind":"pith_short_16","alias_value":"5WXPUMGTAIHW6FJV","created_at":"2026-05-18T12:29:07.941421+00:00"},{"alias_kind":"pith_short_8","alias_value":"5WXPUMGT","created_at":"2026-05-18T12:29:07.941421+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/5WXPUMGTAIHW6FJVFTP3RE6LAQ","json":"https://pith.science/pith/5WXPUMGTAIHW6FJVFTP3RE6LAQ.json","graph_json":"https://pith.science/api/pith-number/5WXPUMGTAIHW6FJVFTP3RE6LAQ/graph.json","events_json":"https://pith.science/api/pith-number/5WXPUMGTAIHW6FJVFTP3RE6LAQ/events.json","paper":"https://pith.science/paper/5WXPUMGT"},"agent_actions":{"view_html":"https://pith.science/pith/5WXPUMGTAIHW6FJVFTP3RE6LAQ","download_json":"https://pith.science/pith/5WXPUMGTAIHW6FJVFTP3RE6LAQ.json","view_paper":"https://pith.science/paper/5WXPUMGT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1509.05541&json=true","fetch_graph":"https://pith.science/api/pith-number/5WXPUMGTAIHW6FJVFTP3RE6LAQ/graph.json","fetch_events":"https://pith.science/api/pith-number/5WXPUMGTAIHW6FJVFTP3RE6LAQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5WXPUMGTAIHW6FJVFTP3RE6LAQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5WXPUMGTAIHW6FJVFTP3RE6LAQ/action/storage_attestation","attest_author":"https://pith.science/pith/5WXPUMGTAIHW6FJVFTP3RE6LAQ/action/author_attestation","sign_citation":"https://pith.science/pith/5WXPUMGTAIHW6FJVFTP3RE6LAQ/action/citation_signature","submit_replication":"https://pith.science/pith/5WXPUMGTAIHW6FJVFTP3RE6LAQ/action/replication_record"}},"created_at":"2026-05-18T00:11:44.270265+00:00","updated_at":"2026-05-18T00:11:44.270265+00:00"}