{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:SPA5YQXDEWWMFYWRXWYEGKQJJA","short_pith_number":"pith:SPA5YQXD","schema_version":"1.0","canonical_sha256":"93c1dc42e325acc2e2d1bdb0432a09480cc0a3f7af9ca007e883e489bf5e6b16","source":{"kind":"arxiv","id":"1205.1476","version":1},"attestation_state":"computed","paper":{"title":"Tuning in magnetic modes in Tb(Co_{x}Ni_{1-x})_{2}B_{2}C: from longitudinal spin-density waves to simple ferromagnetism","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.other"],"primary_cat":"cond-mat.str-el","authors_text":"A. M. Gomes, B. Ouladdiaf, H. Takeya, M. ElMassalami, R. Maia Filho, R. R. dos Santos, T. Paiva","submitted_at":"2012-05-07T18:22:35Z","abstract_excerpt":"Neutron diffraction and thermodynamics techniques were used to probe the evolution of the magnetic properties of Tb(Co_{x}Ni_{1-x})_{2}B_{2}C. A succession of magnetic modes was observed as x is varied: the longitudinal modulated k=(0.55,0,0) state at x=0 is transformed into a collinear k=([nicefrac]<LaTeX>\\nicefrac{1}{2}</LaTeX>,0,[nicefrac]<LaTeX>\\nicefrac{1}{2}</LaTeX>) antiferromagnetic state at x= 0.2, 0.4; then into a transverse c-axis modulated k=(0,0,[nicefrac]<LaTeX>\\nicefrac{1}{3}</LaTeX>) mode at x= 0.6, and finally into a simple ferromagnetic structure at x= 0.8 and 1. Concomitantl"},"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":"1205.1476","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2012-05-07T18:22:35Z","cross_cats_sorted":["cond-mat.other"],"title_canon_sha256":"1bae284d3a7843c77722d8a2916ee0f1518603988587e59d3729336c08bd7aa4","abstract_canon_sha256":"9914b53207bb26481b7145a5e7be440cd0206ad85bce57297a96db46a26c30f9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:57:37.155118Z","signature_b64":"FFFbNUKuWqG6IrG7KZ3Gjl1c72G/R/drSsLZQqdwt+PFJMAzBAntVKUFlTa1iiRSbLe1cjhXGmOaq79qV4EuAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"93c1dc42e325acc2e2d1bdb0432a09480cc0a3f7af9ca007e883e489bf5e6b16","last_reissued_at":"2026-05-18T01:57:37.154490Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:57:37.154490Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Tuning in magnetic modes in Tb(Co_{x}Ni_{1-x})_{2}B_{2}C: from longitudinal spin-density waves to simple ferromagnetism","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.other"],"primary_cat":"cond-mat.str-el","authors_text":"A. M. Gomes, B. Ouladdiaf, H. Takeya, M. ElMassalami, R. Maia Filho, R. R. dos Santos, T. Paiva","submitted_at":"2012-05-07T18:22:35Z","abstract_excerpt":"Neutron diffraction and thermodynamics techniques were used to probe the evolution of the magnetic properties of Tb(Co_{x}Ni_{1-x})_{2}B_{2}C. A succession of magnetic modes was observed as x is varied: the longitudinal modulated k=(0.55,0,0) state at x=0 is transformed into a collinear k=([nicefrac]<LaTeX>\\nicefrac{1}{2}</LaTeX>,0,[nicefrac]<LaTeX>\\nicefrac{1}{2}</LaTeX>) antiferromagnetic state at x= 0.2, 0.4; then into a transverse c-axis modulated k=(0,0,[nicefrac]<LaTeX>\\nicefrac{1}{3}</LaTeX>) mode at x= 0.6, and finally into a simple ferromagnetic structure at x= 0.8 and 1. Concomitantl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1205.1476","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":"1205.1476","created_at":"2026-05-18T01:57:37.154579+00:00"},{"alias_kind":"arxiv_version","alias_value":"1205.1476v1","created_at":"2026-05-18T01:57:37.154579+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1205.1476","created_at":"2026-05-18T01:57:37.154579+00:00"},{"alias_kind":"pith_short_12","alias_value":"SPA5YQXDEWWM","created_at":"2026-05-18T12:27:20.899486+00:00"},{"alias_kind":"pith_short_16","alias_value":"SPA5YQXDEWWMFYWR","created_at":"2026-05-18T12:27:20.899486+00:00"},{"alias_kind":"pith_short_8","alias_value":"SPA5YQXD","created_at":"2026-05-18T12:27:20.899486+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/SPA5YQXDEWWMFYWRXWYEGKQJJA","json":"https://pith.science/pith/SPA5YQXDEWWMFYWRXWYEGKQJJA.json","graph_json":"https://pith.science/api/pith-number/SPA5YQXDEWWMFYWRXWYEGKQJJA/graph.json","events_json":"https://pith.science/api/pith-number/SPA5YQXDEWWMFYWRXWYEGKQJJA/events.json","paper":"https://pith.science/paper/SPA5YQXD"},"agent_actions":{"view_html":"https://pith.science/pith/SPA5YQXDEWWMFYWRXWYEGKQJJA","download_json":"https://pith.science/pith/SPA5YQXDEWWMFYWRXWYEGKQJJA.json","view_paper":"https://pith.science/paper/SPA5YQXD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1205.1476&json=true","fetch_graph":"https://pith.science/api/pith-number/SPA5YQXDEWWMFYWRXWYEGKQJJA/graph.json","fetch_events":"https://pith.science/api/pith-number/SPA5YQXDEWWMFYWRXWYEGKQJJA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SPA5YQXDEWWMFYWRXWYEGKQJJA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SPA5YQXDEWWMFYWRXWYEGKQJJA/action/storage_attestation","attest_author":"https://pith.science/pith/SPA5YQXDEWWMFYWRXWYEGKQJJA/action/author_attestation","sign_citation":"https://pith.science/pith/SPA5YQXDEWWMFYWRXWYEGKQJJA/action/citation_signature","submit_replication":"https://pith.science/pith/SPA5YQXDEWWMFYWRXWYEGKQJJA/action/replication_record"}},"created_at":"2026-05-18T01:57:37.154579+00:00","updated_at":"2026-05-18T01:57:37.154579+00:00"}