{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:ZIRIYO7Q33NAVDUL6F4XTGTQ5G","short_pith_number":"pith:ZIRIYO7Q","schema_version":"1.0","canonical_sha256":"ca228c3bf0deda0a8e8bf179799a70e98c2ed227a98f55424d406057012bf143","source":{"kind":"arxiv","id":"1503.06737","version":3},"attestation_state":"computed","paper":{"title":"Neutron spin resonance as a probe of superconducting gap anisotropy in partially detwinned electron underdoped NaFe$_{0.985}$Co$_{0.015}$As","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Chenglin Zhang, J. T. Park, J. W. Lynn, Pengcheng Dai, Qimiao Si, Rong Yu, Wenliang Zhang, Xingye Lu, Yang Zhao, Yu Li","submitted_at":"2015-03-23T17:28:46Z","abstract_excerpt":"We use inelastic neutron scattering (INS) to study the spin excitations in partially detwinned NaFe$_{0.985}$Co$_{0.015}$As which has coexisting static antiferromagnetic (AF) order and superconductivity ($T_c=15$ K, $T_N=30$ K). In previous INS work on a twinned sample, spin excitations form a dispersive sharp resonance near $E_{r1}=3.25$ meV and a broad dispersionless mode at $E_{r1}=6$ meV at the AF ordering wave vector ${\\bf Q}_{\\rm AF}={\\bf Q}_1=(1,0)$ and its twinned domain ${\\bf Q}_2=(0,1)$. For partially detwinned NaFe$_{0.985}$Co$_{0.015}$As with the static AF order mostly occurring at"},"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":"1503.06737","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2015-03-23T17:28:46Z","cross_cats_sorted":[],"title_canon_sha256":"d8b60624389abfe7930811c712637e41721a09dc3eb00de6f9eab374b0550a7a","abstract_canon_sha256":"0d2c6ce6d7251bee9314a1aef338312ebcf556a1e9c70e56ace5dfb67d6b6135"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:40:50.074725Z","signature_b64":"F5N0xcimzg8PgX/HuLT/uKnK8aKq1PH3iMiMQwHYsy/aJqDUNc1b2KTriN3NHMNVZkv2i9Jrk0xotKZeCysADw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ca228c3bf0deda0a8e8bf179799a70e98c2ed227a98f55424d406057012bf143","last_reissued_at":"2026-05-18T01:40:50.074098Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:40:50.074098Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Neutron spin resonance as a probe of superconducting gap anisotropy in partially detwinned electron underdoped NaFe$_{0.985}$Co$_{0.015}$As","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Chenglin Zhang, J. T. Park, J. W. Lynn, Pengcheng Dai, Qimiao Si, Rong Yu, Wenliang Zhang, Xingye Lu, Yang Zhao, Yu Li","submitted_at":"2015-03-23T17:28:46Z","abstract_excerpt":"We use inelastic neutron scattering (INS) to study the spin excitations in partially detwinned NaFe$_{0.985}$Co$_{0.015}$As which has coexisting static antiferromagnetic (AF) order and superconductivity ($T_c=15$ K, $T_N=30$ K). In previous INS work on a twinned sample, spin excitations form a dispersive sharp resonance near $E_{r1}=3.25$ meV and a broad dispersionless mode at $E_{r1}=6$ meV at the AF ordering wave vector ${\\bf Q}_{\\rm AF}={\\bf Q}_1=(1,0)$ and its twinned domain ${\\bf Q}_2=(0,1)$. For partially detwinned NaFe$_{0.985}$Co$_{0.015}$As with the static AF order mostly occurring at"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1503.06737","kind":"arxiv","version":3},"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":"1503.06737","created_at":"2026-05-18T01:40:50.074195+00:00"},{"alias_kind":"arxiv_version","alias_value":"1503.06737v3","created_at":"2026-05-18T01:40:50.074195+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1503.06737","created_at":"2026-05-18T01:40:50.074195+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZIRIYO7Q33NA","created_at":"2026-05-18T12:29:52.810259+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZIRIYO7Q33NAVDUL","created_at":"2026-05-18T12:29:52.810259+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZIRIYO7Q","created_at":"2026-05-18T12:29:52.810259+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/ZIRIYO7Q33NAVDUL6F4XTGTQ5G","json":"https://pith.science/pith/ZIRIYO7Q33NAVDUL6F4XTGTQ5G.json","graph_json":"https://pith.science/api/pith-number/ZIRIYO7Q33NAVDUL6F4XTGTQ5G/graph.json","events_json":"https://pith.science/api/pith-number/ZIRIYO7Q33NAVDUL6F4XTGTQ5G/events.json","paper":"https://pith.science/paper/ZIRIYO7Q"},"agent_actions":{"view_html":"https://pith.science/pith/ZIRIYO7Q33NAVDUL6F4XTGTQ5G","download_json":"https://pith.science/pith/ZIRIYO7Q33NAVDUL6F4XTGTQ5G.json","view_paper":"https://pith.science/paper/ZIRIYO7Q","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1503.06737&json=true","fetch_graph":"https://pith.science/api/pith-number/ZIRIYO7Q33NAVDUL6F4XTGTQ5G/graph.json","fetch_events":"https://pith.science/api/pith-number/ZIRIYO7Q33NAVDUL6F4XTGTQ5G/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZIRIYO7Q33NAVDUL6F4XTGTQ5G/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZIRIYO7Q33NAVDUL6F4XTGTQ5G/action/storage_attestation","attest_author":"https://pith.science/pith/ZIRIYO7Q33NAVDUL6F4XTGTQ5G/action/author_attestation","sign_citation":"https://pith.science/pith/ZIRIYO7Q33NAVDUL6F4XTGTQ5G/action/citation_signature","submit_replication":"https://pith.science/pith/ZIRIYO7Q33NAVDUL6F4XTGTQ5G/action/replication_record"}},"created_at":"2026-05-18T01:40:50.074195+00:00","updated_at":"2026-05-18T01:40:50.074195+00:00"}