{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:K3VZKPJWF7ZDFSP3T4GJNMUA3N","short_pith_number":"pith:K3VZKPJW","schema_version":"1.0","canonical_sha256":"56eb953d362ff232c9fb9f0c96b280db69fdef3bfb6d12367b2046ffab5d75eb","source":{"kind":"arxiv","id":"2511.08179","version":2},"attestation_state":"computed","paper":{"title":"Non-linear spin wave theory in the strong easy-axis limit of the triangular XXZ model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Achille Mauri, Fr\\'ed\\'eric Mila, Siebe Roose","submitted_at":"2025-11-11T12:42:47Z","abstract_excerpt":"Motivated by recent experimental studies, we investigate the spectrum of the nearest-neighbour triangular XXZ model within the $1/S$ expansion, in the limit in which the exchange couplings present a strong easy-axis anisotropy $J_{xy}/J_{zz} \\ll 1$. We show that in the limit in which $1/S \\to 0$ and $J_{xy} \\to 0$ at fixed $V = J_{zz}/(S J_{xy})$, the triangular spin model can be reduced to an effective boson model with quartic interactions on the honeycomb lattice. This effective model interpolates between a spin-wave ($V \\to 0$) and a strong-coupling limit ($V \\to \\infty$) and encodes in a s"},"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":"2511.08179","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-11-11T12:42:47Z","cross_cats_sorted":[],"title_canon_sha256":"3f70c88d5dbe43d19db4fc988eddc4db3f6c305b4e057b106e46b882b7ebdece","abstract_canon_sha256":"ee80c44b6f0b05e0e063547b4438128f9d94e22baa2af0bba0047c7f27cb48f6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-27T01:05:39.822368Z","signature_b64":"j4c0dd3E6dPtBiH/EewZVLA7lHQ006oF2Z/5AA/ly2xZf5x4/nLn8BbOC3BVzkxjZzQOuSjAaW/fWT8Kir40AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"56eb953d362ff232c9fb9f0c96b280db69fdef3bfb6d12367b2046ffab5d75eb","last_reissued_at":"2026-05-27T01:05:39.821770Z","signature_status":"signed_v1","first_computed_at":"2026-05-27T01:05:39.821770Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-linear spin wave theory in the strong easy-axis limit of the triangular XXZ model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Achille Mauri, Fr\\'ed\\'eric Mila, Siebe Roose","submitted_at":"2025-11-11T12:42:47Z","abstract_excerpt":"Motivated by recent experimental studies, we investigate the spectrum of the nearest-neighbour triangular XXZ model within the $1/S$ expansion, in the limit in which the exchange couplings present a strong easy-axis anisotropy $J_{xy}/J_{zz} \\ll 1$. We show that in the limit in which $1/S \\to 0$ and $J_{xy} \\to 0$ at fixed $V = J_{zz}/(S J_{xy})$, the triangular spin model can be reduced to an effective boson model with quartic interactions on the honeycomb lattice. This effective model interpolates between a spin-wave ($V \\to 0$) and a strong-coupling limit ($V \\to \\infty$) and encodes in a s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2511.08179","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/2511.08179/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":"2511.08179","created_at":"2026-05-27T01:05:39.821852+00:00"},{"alias_kind":"arxiv_version","alias_value":"2511.08179v2","created_at":"2026-05-27T01:05:39.821852+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2511.08179","created_at":"2026-05-27T01:05:39.821852+00:00"},{"alias_kind":"pith_short_12","alias_value":"K3VZKPJWF7ZD","created_at":"2026-05-27T01:05:39.821852+00:00"},{"alias_kind":"pith_short_16","alias_value":"K3VZKPJWF7ZDFSP3","created_at":"2026-05-27T01:05:39.821852+00:00"},{"alias_kind":"pith_short_8","alias_value":"K3VZKPJW","created_at":"2026-05-27T01:05:39.821852+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2601.01890","citing_title":"Emergent Spin Supersolids in Frustrated Quantum Materials","ref_index":122,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/K3VZKPJWF7ZDFSP3T4GJNMUA3N","json":"https://pith.science/pith/K3VZKPJWF7ZDFSP3T4GJNMUA3N.json","graph_json":"https://pith.science/api/pith-number/K3VZKPJWF7ZDFSP3T4GJNMUA3N/graph.json","events_json":"https://pith.science/api/pith-number/K3VZKPJWF7ZDFSP3T4GJNMUA3N/events.json","paper":"https://pith.science/paper/K3VZKPJW"},"agent_actions":{"view_html":"https://pith.science/pith/K3VZKPJWF7ZDFSP3T4GJNMUA3N","download_json":"https://pith.science/pith/K3VZKPJWF7ZDFSP3T4GJNMUA3N.json","view_paper":"https://pith.science/paper/K3VZKPJW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2511.08179&json=true","fetch_graph":"https://pith.science/api/pith-number/K3VZKPJWF7ZDFSP3T4GJNMUA3N/graph.json","fetch_events":"https://pith.science/api/pith-number/K3VZKPJWF7ZDFSP3T4GJNMUA3N/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/K3VZKPJWF7ZDFSP3T4GJNMUA3N/action/timestamp_anchor","attest_storage":"https://pith.science/pith/K3VZKPJWF7ZDFSP3T4GJNMUA3N/action/storage_attestation","attest_author":"https://pith.science/pith/K3VZKPJWF7ZDFSP3T4GJNMUA3N/action/author_attestation","sign_citation":"https://pith.science/pith/K3VZKPJWF7ZDFSP3T4GJNMUA3N/action/citation_signature","submit_replication":"https://pith.science/pith/K3VZKPJWF7ZDFSP3T4GJNMUA3N/action/replication_record"}},"created_at":"2026-05-27T01:05:39.821852+00:00","updated_at":"2026-05-27T01:05:39.821852+00:00"}