{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:G3IYVQ57OBV7BC74I5BOYIOJXK","short_pith_number":"pith:G3IYVQ57","schema_version":"1.0","canonical_sha256":"36d18ac3bf706bf08bfc4742ec21c9bab8b7fa42013edb4a5759c1c48f7d5450","source":{"kind":"arxiv","id":"2106.11402","version":1},"attestation_state":"computed","paper":{"title":"Large exchange bias and low temperature glassy state in frustrated triangular-lattice antiferromagnet Ba$_3$NiIr$_2$O$_9$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.str-el","authors_text":"A. K. Pramanik, Kranti Kumar, Manju Mishra Patidar, M. P. Saravanan, Shobha Gondh, V. Ganesan","submitted_at":"2021-06-21T20:34:21Z","abstract_excerpt":"Here, we report both ac and dc magnetization, thermodynamic and electric properties of hexagonal Ba$_3$NiIr$_2$O$_9$. The Ni$^{2+}$ (spin-1) forms layered triangular-lattice and interacts antiferromagnetically while Ir$^{5+}$ is believed to act as magnetic link between the layers. This complex magnetic interaction results in magnetic frustration leading to a spin-glass transition at $T_f$ $\\sim$ 8.5 K. The observed magnetic relaxation and aging effect also confirms the nonequilibrium ground state. The system further shows large exchange bias which is tunable with cooling field. Below the Curie"},"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":"2106.11402","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2021-06-21T20:34:21Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"98ab9cb2cf024e70727359dcfbd6d58cd6ab1d3814e2e22a93818dd8b81764b9","abstract_canon_sha256":"17d3a23434c7b7701bd992aa19cd3282faa4ca988fd2499d37578fc52ebc9b85"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:57:24.107296Z","signature_b64":"k23KbRj1qeyCcCO6jh6us0IhTB/EttSLm3B6bUeDmY3jcNpGk+AaJpCHKdoyoXuCi4BO0BWaAw00tzuEV+8YAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"36d18ac3bf706bf08bfc4742ec21c9bab8b7fa42013edb4a5759c1c48f7d5450","last_reissued_at":"2026-07-05T02:57:24.106835Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:57:24.106835Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Large exchange bias and low temperature glassy state in frustrated triangular-lattice antiferromagnet Ba$_3$NiIr$_2$O$_9$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.str-el","authors_text":"A. K. Pramanik, Kranti Kumar, Manju Mishra Patidar, M. P. Saravanan, Shobha Gondh, V. Ganesan","submitted_at":"2021-06-21T20:34:21Z","abstract_excerpt":"Here, we report both ac and dc magnetization, thermodynamic and electric properties of hexagonal Ba$_3$NiIr$_2$O$_9$. The Ni$^{2+}$ (spin-1) forms layered triangular-lattice and interacts antiferromagnetically while Ir$^{5+}$ is believed to act as magnetic link between the layers. This complex magnetic interaction results in magnetic frustration leading to a spin-glass transition at $T_f$ $\\sim$ 8.5 K. The observed magnetic relaxation and aging effect also confirms the nonequilibrium ground state. The system further shows large exchange bias which is tunable with cooling field. Below the Curie"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2106.11402","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2106.11402/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2106.11402","created_at":"2026-07-05T02:57:24.106893+00:00"},{"alias_kind":"arxiv_version","alias_value":"2106.11402v1","created_at":"2026-07-05T02:57:24.106893+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2106.11402","created_at":"2026-07-05T02:57:24.106893+00:00"},{"alias_kind":"pith_short_12","alias_value":"G3IYVQ57OBV7","created_at":"2026-07-05T02:57:24.106893+00:00"},{"alias_kind":"pith_short_16","alias_value":"G3IYVQ57OBV7BC74","created_at":"2026-07-05T02:57:24.106893+00:00"},{"alias_kind":"pith_short_8","alias_value":"G3IYVQ57","created_at":"2026-07-05T02:57:24.106893+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/G3IYVQ57OBV7BC74I5BOYIOJXK","json":"https://pith.science/pith/G3IYVQ57OBV7BC74I5BOYIOJXK.json","graph_json":"https://pith.science/api/pith-number/G3IYVQ57OBV7BC74I5BOYIOJXK/graph.json","events_json":"https://pith.science/api/pith-number/G3IYVQ57OBV7BC74I5BOYIOJXK/events.json","paper":"https://pith.science/paper/G3IYVQ57"},"agent_actions":{"view_html":"https://pith.science/pith/G3IYVQ57OBV7BC74I5BOYIOJXK","download_json":"https://pith.science/pith/G3IYVQ57OBV7BC74I5BOYIOJXK.json","view_paper":"https://pith.science/paper/G3IYVQ57","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2106.11402&json=true","fetch_graph":"https://pith.science/api/pith-number/G3IYVQ57OBV7BC74I5BOYIOJXK/graph.json","fetch_events":"https://pith.science/api/pith-number/G3IYVQ57OBV7BC74I5BOYIOJXK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/G3IYVQ57OBV7BC74I5BOYIOJXK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/G3IYVQ57OBV7BC74I5BOYIOJXK/action/storage_attestation","attest_author":"https://pith.science/pith/G3IYVQ57OBV7BC74I5BOYIOJXK/action/author_attestation","sign_citation":"https://pith.science/pith/G3IYVQ57OBV7BC74I5BOYIOJXK/action/citation_signature","submit_replication":"https://pith.science/pith/G3IYVQ57OBV7BC74I5BOYIOJXK/action/replication_record"}},"created_at":"2026-07-05T02:57:24.106893+00:00","updated_at":"2026-07-05T02:57:24.106893+00:00"}