{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:N3UH6CFSNLNTEGVQZY5AWGITSG","short_pith_number":"pith:N3UH6CFS","schema_version":"1.0","canonical_sha256":"6ee87f08b26adb321ab0ce3a0b19139192db9414184b54fd00e74fb4d5b5ffa5","source":{"kind":"arxiv","id":"1301.2025","version":1},"attestation_state":"computed","paper":{"title":"Phase Diagram and Magnetic Excitations of Anisotropic Spin-One Magnets","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Cristian D. Batista, Ian Yap, Keola Wierschem, Pinaki Sengupta, Yasuyuki Kato, Zhifeng Zhang","submitted_at":"2013-01-10T04:05:58Z","abstract_excerpt":"We use a generalized spin wave approach and large scale quantum Monte Carlo (QMC) simulations to study the quantum phase diagram and quasiparticle excitations of the S=1 Heisenberg model with an easy-plane single-ion anisotropy in dimensions d=2 and 3. We consider two alternative approximations for describing the quantum paramagnetic state: the standard Holstein-Primakoff approximation and a modified treatment in which the local constraint (finite dimension of the local Hilbert space) is enforced by introducing a Lagrange multiplier. While both approximations produce qualitatively similar resu"},"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":"1301.2025","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2013-01-10T04:05:58Z","cross_cats_sorted":[],"title_canon_sha256":"eceb204e49f25605f741cbe6fd794302eb79786a7385abb47612758746e45ac8","abstract_canon_sha256":"4053b79264c2de9bd78361d939a978dd5446d616d1648a2a0307b8853a64204c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:18:49.667724Z","signature_b64":"4txX7is5RXAIOfABoCio9PhwHlcQKKj+gbkJfK0GYkrQ1gS5gtWF+E32sDGoncEGGXOS1DrB0ZIq7bGFBoiFDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6ee87f08b26adb321ab0ce3a0b19139192db9414184b54fd00e74fb4d5b5ffa5","last_reissued_at":"2026-05-18T03:18:49.667100Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:18:49.667100Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phase Diagram and Magnetic Excitations of Anisotropic Spin-One Magnets","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Cristian D. Batista, Ian Yap, Keola Wierschem, Pinaki Sengupta, Yasuyuki Kato, Zhifeng Zhang","submitted_at":"2013-01-10T04:05:58Z","abstract_excerpt":"We use a generalized spin wave approach and large scale quantum Monte Carlo (QMC) simulations to study the quantum phase diagram and quasiparticle excitations of the S=1 Heisenberg model with an easy-plane single-ion anisotropy in dimensions d=2 and 3. We consider two alternative approximations for describing the quantum paramagnetic state: the standard Holstein-Primakoff approximation and a modified treatment in which the local constraint (finite dimension of the local Hilbert space) is enforced by introducing a Lagrange multiplier. While both approximations produce qualitatively similar resu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1301.2025","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":"1301.2025","created_at":"2026-05-18T03:18:49.667196+00:00"},{"alias_kind":"arxiv_version","alias_value":"1301.2025v1","created_at":"2026-05-18T03:18:49.667196+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1301.2025","created_at":"2026-05-18T03:18:49.667196+00:00"},{"alias_kind":"pith_short_12","alias_value":"N3UH6CFSNLNT","created_at":"2026-05-18T12:27:52.871228+00:00"},{"alias_kind":"pith_short_16","alias_value":"N3UH6CFSNLNTEGVQ","created_at":"2026-05-18T12:27:52.871228+00:00"},{"alias_kind":"pith_short_8","alias_value":"N3UH6CFS","created_at":"2026-05-18T12:27:52.871228+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.18705","citing_title":"Conformal Data for the $O(2)$ Wilson-Fisher CFT in $(2+1)$-Dimensional Spacetime from Exact Diagonalization and Matrix Product States on the Fuzzy Sphere","ref_index":65,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/N3UH6CFSNLNTEGVQZY5AWGITSG","json":"https://pith.science/pith/N3UH6CFSNLNTEGVQZY5AWGITSG.json","graph_json":"https://pith.science/api/pith-number/N3UH6CFSNLNTEGVQZY5AWGITSG/graph.json","events_json":"https://pith.science/api/pith-number/N3UH6CFSNLNTEGVQZY5AWGITSG/events.json","paper":"https://pith.science/paper/N3UH6CFS"},"agent_actions":{"view_html":"https://pith.science/pith/N3UH6CFSNLNTEGVQZY5AWGITSG","download_json":"https://pith.science/pith/N3UH6CFSNLNTEGVQZY5AWGITSG.json","view_paper":"https://pith.science/paper/N3UH6CFS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1301.2025&json=true","fetch_graph":"https://pith.science/api/pith-number/N3UH6CFSNLNTEGVQZY5AWGITSG/graph.json","fetch_events":"https://pith.science/api/pith-number/N3UH6CFSNLNTEGVQZY5AWGITSG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/N3UH6CFSNLNTEGVQZY5AWGITSG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/N3UH6CFSNLNTEGVQZY5AWGITSG/action/storage_attestation","attest_author":"https://pith.science/pith/N3UH6CFSNLNTEGVQZY5AWGITSG/action/author_attestation","sign_citation":"https://pith.science/pith/N3UH6CFSNLNTEGVQZY5AWGITSG/action/citation_signature","submit_replication":"https://pith.science/pith/N3UH6CFSNLNTEGVQZY5AWGITSG/action/replication_record"}},"created_at":"2026-05-18T03:18:49.667196+00:00","updated_at":"2026-05-18T03:18:49.667196+00:00"}