{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:O6C4KYWGPSABZ4S7FXWZEPS4ZD","short_pith_number":"pith:O6C4KYWG","schema_version":"1.0","canonical_sha256":"7785c562c67c801cf25f2ded923e5cc8d4499e39184c578ae8feb64fb4d23869","source":{"kind":"arxiv","id":"2504.20225","version":1},"attestation_state":"computed","paper":{"title":"Magnons in the strained Heisenberg-Kitaev magnet","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Miguel Letelier, Nicolas Vidal-Silva, Roberto E. Troncoso","submitted_at":"2025-04-28T19:49:02Z","abstract_excerpt":"The properties of magnons hosted in strained Heisenberg-Kitaev magnets are investigated using numerical and analytical calculations. Considering that deformation fields modulate the coupling parameters, we find a general expression for the weakly strained magnon Hamiltonian that depends on the (symmetric) strain tensor. We numerically tested our results in finite nanoribbon structures. We found that uniaxial deformations make the bulk bands more dispersive while topologically protected in-gap edge modes become nonreciprocal at the boundary of the Brillouin Zone. On the other hand, when applyin"},"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":"2504.20225","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2025-04-28T19:49:02Z","cross_cats_sorted":[],"title_canon_sha256":"fb1ba63a28c0508fa151d60a31177bb566a0657eb635e3729cceb3ea19734b75","abstract_canon_sha256":"4b623a834467435ed8f892e4d6d58cd76459c64c5f6183d401f2b38043c512e8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:55:38.792523Z","signature_b64":"yZxWqweeKVkiEDRIwpGl3go9yQfm+7kaQHctIXxW9zTC7l8aKglv8EEFAmzJ7rqnsj+zeWWVQI/s5pGjQzwhCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7785c562c67c801cf25f2ded923e5cc8d4499e39184c578ae8feb64fb4d23869","last_reissued_at":"2026-07-05T10:55:38.791973Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:55:38.791973Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Magnons in the strained Heisenberg-Kitaev magnet","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Miguel Letelier, Nicolas Vidal-Silva, Roberto E. Troncoso","submitted_at":"2025-04-28T19:49:02Z","abstract_excerpt":"The properties of magnons hosted in strained Heisenberg-Kitaev magnets are investigated using numerical and analytical calculations. Considering that deformation fields modulate the coupling parameters, we find a general expression for the weakly strained magnon Hamiltonian that depends on the (symmetric) strain tensor. We numerically tested our results in finite nanoribbon structures. We found that uniaxial deformations make the bulk bands more dispersive while topologically protected in-gap edge modes become nonreciprocal at the boundary of the Brillouin Zone. On the other hand, when applyin"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2504.20225","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/2504.20225/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":"2504.20225","created_at":"2026-07-05T10:55:38.792028+00:00"},{"alias_kind":"arxiv_version","alias_value":"2504.20225v1","created_at":"2026-07-05T10:55:38.792028+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2504.20225","created_at":"2026-07-05T10:55:38.792028+00:00"},{"alias_kind":"pith_short_12","alias_value":"O6C4KYWGPSAB","created_at":"2026-07-05T10:55:38.792028+00:00"},{"alias_kind":"pith_short_16","alias_value":"O6C4KYWGPSABZ4S7","created_at":"2026-07-05T10:55:38.792028+00:00"},{"alias_kind":"pith_short_8","alias_value":"O6C4KYWG","created_at":"2026-07-05T10:55:38.792028+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/O6C4KYWGPSABZ4S7FXWZEPS4ZD","json":"https://pith.science/pith/O6C4KYWGPSABZ4S7FXWZEPS4ZD.json","graph_json":"https://pith.science/api/pith-number/O6C4KYWGPSABZ4S7FXWZEPS4ZD/graph.json","events_json":"https://pith.science/api/pith-number/O6C4KYWGPSABZ4S7FXWZEPS4ZD/events.json","paper":"https://pith.science/paper/O6C4KYWG"},"agent_actions":{"view_html":"https://pith.science/pith/O6C4KYWGPSABZ4S7FXWZEPS4ZD","download_json":"https://pith.science/pith/O6C4KYWGPSABZ4S7FXWZEPS4ZD.json","view_paper":"https://pith.science/paper/O6C4KYWG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2504.20225&json=true","fetch_graph":"https://pith.science/api/pith-number/O6C4KYWGPSABZ4S7FXWZEPS4ZD/graph.json","fetch_events":"https://pith.science/api/pith-number/O6C4KYWGPSABZ4S7FXWZEPS4ZD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/O6C4KYWGPSABZ4S7FXWZEPS4ZD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/O6C4KYWGPSABZ4S7FXWZEPS4ZD/action/storage_attestation","attest_author":"https://pith.science/pith/O6C4KYWGPSABZ4S7FXWZEPS4ZD/action/author_attestation","sign_citation":"https://pith.science/pith/O6C4KYWGPSABZ4S7FXWZEPS4ZD/action/citation_signature","submit_replication":"https://pith.science/pith/O6C4KYWGPSABZ4S7FXWZEPS4ZD/action/replication_record"}},"created_at":"2026-07-05T10:55:38.792028+00:00","updated_at":"2026-07-05T10:55:38.792028+00:00"}