{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:JU7D43VJKI3VLMGGVS2C7CGXG4","short_pith_number":"pith:JU7D43VJ","schema_version":"1.0","canonical_sha256":"4d3e3e6ea9523755b0c6acb42f88d73708d40ec91928fda08aa15490aa6902ee","source":{"kind":"arxiv","id":"cond-mat/0612357","version":2},"attestation_state":"computed","paper":{"title":"Importance of In-Plane Anisotropy in the Quasi Two-Dimensional Antiferromagnet BaNi$_{2}$V$_{2}$O$_{8}$","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"C. Meingast, H. v. L\\\"ohneysen, K. Grube, P. Adelmann, P. Popovich, P. Schweiss, S. Drobnik, Th. Wolf, W. Knafo","submitted_at":"2006-12-14T11:16:30Z","abstract_excerpt":"The phase diagram of the quasi two-dimensional antiferromagnet BaNi$_{2}$V$_{2}$O$_{8}$ is studied by specific heat, thermal expansion, magnetostriction, and magnetization for magnetic fields applied perpendicular to $\\mathbf{c}$. At $\\mu_0H^{*}\\simeq1.5$ T, a crossover to a high-field state, where $T_N(H)$ increases linearly, arises from a competition of intrinsic and field-induced in-plane anisotropies. The pressure dependences of $T_N$ and $H^{*}$ are interpreted using the picture of a pressure-induced in-plane anisotropy. Even at zero field and ambient pressure, in-plane anisotropy cannot "},"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":"cond-mat/0612357","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"cond-mat.str-el","submitted_at":"2006-12-14T11:16:30Z","cross_cats_sorted":[],"title_canon_sha256":"a5c0d4582d74d1530644dfb9abe3559cf4e29b529957dcb2263ba5545f4eed23","abstract_canon_sha256":"40f6946315d0f8c4b28e128f65062b776088d1da1e815b1f82551f324eb22a8f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:04:32.673116Z","signature_b64":"8UhO5KMhLyTVQTqdA/8LF+gmcs5s2G4YXjEBcmCfRFV+lKz/Z+LQ8pDC2rBpUjeqD8fLJVuJ1uBNLmGUmw9XDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4d3e3e6ea9523755b0c6acb42f88d73708d40ec91928fda08aa15490aa6902ee","last_reissued_at":"2026-07-04T15:04:32.672756Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:04:32.672756Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Importance of In-Plane Anisotropy in the Quasi Two-Dimensional Antiferromagnet BaNi$_{2}$V$_{2}$O$_{8}$","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"C. Meingast, H. v. L\\\"ohneysen, K. Grube, P. Adelmann, P. Popovich, P. Schweiss, S. Drobnik, Th. Wolf, W. Knafo","submitted_at":"2006-12-14T11:16:30Z","abstract_excerpt":"The phase diagram of the quasi two-dimensional antiferromagnet BaNi$_{2}$V$_{2}$O$_{8}$ is studied by specific heat, thermal expansion, magnetostriction, and magnetization for magnetic fields applied perpendicular to $\\mathbf{c}$. At $\\mu_0H^{*}\\simeq1.5$ T, a crossover to a high-field state, where $T_N(H)$ increases linearly, arises from a competition of intrinsic and field-induced in-plane anisotropies. The pressure dependences of $T_N$ and $H^{*}$ are interpreted using the picture of a pressure-induced in-plane anisotropy. Even at zero field and ambient pressure, in-plane anisotropy cannot "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0612357","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/cond-mat/0612357/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":"cond-mat/0612357","created_at":"2026-07-04T15:04:32.672817+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0612357v2","created_at":"2026-07-04T15:04:32.672817+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0612357","created_at":"2026-07-04T15:04:32.672817+00:00"},{"alias_kind":"pith_short_12","alias_value":"JU7D43VJKI3V","created_at":"2026-07-04T15:04:32.672817+00:00"},{"alias_kind":"pith_short_16","alias_value":"JU7D43VJKI3VLMGG","created_at":"2026-07-04T15:04:32.672817+00:00"},{"alias_kind":"pith_short_8","alias_value":"JU7D43VJ","created_at":"2026-07-04T15:04:32.672817+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/JU7D43VJKI3VLMGGVS2C7CGXG4","json":"https://pith.science/pith/JU7D43VJKI3VLMGGVS2C7CGXG4.json","graph_json":"https://pith.science/api/pith-number/JU7D43VJKI3VLMGGVS2C7CGXG4/graph.json","events_json":"https://pith.science/api/pith-number/JU7D43VJKI3VLMGGVS2C7CGXG4/events.json","paper":"https://pith.science/paper/JU7D43VJ"},"agent_actions":{"view_html":"https://pith.science/pith/JU7D43VJKI3VLMGGVS2C7CGXG4","download_json":"https://pith.science/pith/JU7D43VJKI3VLMGGVS2C7CGXG4.json","view_paper":"https://pith.science/paper/JU7D43VJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/0612357&json=true","fetch_graph":"https://pith.science/api/pith-number/JU7D43VJKI3VLMGGVS2C7CGXG4/graph.json","fetch_events":"https://pith.science/api/pith-number/JU7D43VJKI3VLMGGVS2C7CGXG4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JU7D43VJKI3VLMGGVS2C7CGXG4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JU7D43VJKI3VLMGGVS2C7CGXG4/action/storage_attestation","attest_author":"https://pith.science/pith/JU7D43VJKI3VLMGGVS2C7CGXG4/action/author_attestation","sign_citation":"https://pith.science/pith/JU7D43VJKI3VLMGGVS2C7CGXG4/action/citation_signature","submit_replication":"https://pith.science/pith/JU7D43VJKI3VLMGGVS2C7CGXG4/action/replication_record"}},"created_at":"2026-07-04T15:04:32.672817+00:00","updated_at":"2026-07-04T15:04:32.672817+00:00"}