{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:UHY6Z75XO6SFP2RPNVHSC6XVE5","short_pith_number":"pith:UHY6Z75X","schema_version":"1.0","canonical_sha256":"a1f1ecffb777a457ea2f6d4f217af5276046ae0a3c104f2e7ec02d44b0ecbc52","source":{"kind":"arxiv","id":"2309.02355","version":1},"attestation_state":"computed","paper":{"title":"Induced Monolayer Altermagnetism in MnP(S,Se)$_3$ and FeSe","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"Igor Mazin, Libor \\v{S}mejkal, Rafael Gonz\\'alez-Hern\\'andez","submitted_at":"2023-09-05T16:11:45Z","abstract_excerpt":"Altermagnets (AM) are a recently discovered third class of collinear magnets, distinctly different from conventional ferromagnets (FM) and antiferromagnets (AF). AM have been actively researched in the last few years, but two aspects so far remain unaddressed: (1) Are there realistic 2D single-layer altermagnets? And (2) is it possible to functionalize a conventional AF into AM by external stimuli? In this paper we address both issues by demonstrating how a well-known 2D AF, MnP(S,Se)$_3$ can be functionalized into strong AM by applying out-of-plane electric field. Of particular interest is th"},"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":"2309.02355","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2023-09-05T16:11:45Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"8f3f6e03046737cfee717d5aee269cbd1c51fcfbd78e85d0a2caf105de67fe9c","abstract_canon_sha256":"bc692e17acf7d7db610077a1fef4cacff2f40e722621a8112a296408bba6a1ba"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:47:59.105238Z","signature_b64":"wXwGNabqI/WiLyGb1WiW1VnKC2meDBHSoHrZq8DxSNfTZZm+WhmW2LPpu5Y3NWP2MEQyP2QYwEzUKt9u1ueVBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a1f1ecffb777a457ea2f6d4f217af5276046ae0a3c104f2e7ec02d44b0ecbc52","last_reissued_at":"2026-07-05T06:47:59.104786Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:47:59.104786Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Induced Monolayer Altermagnetism in MnP(S,Se)$_3$ and FeSe","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"Igor Mazin, Libor \\v{S}mejkal, Rafael Gonz\\'alez-Hern\\'andez","submitted_at":"2023-09-05T16:11:45Z","abstract_excerpt":"Altermagnets (AM) are a recently discovered third class of collinear magnets, distinctly different from conventional ferromagnets (FM) and antiferromagnets (AF). AM have been actively researched in the last few years, but two aspects so far remain unaddressed: (1) Are there realistic 2D single-layer altermagnets? And (2) is it possible to functionalize a conventional AF into AM by external stimuli? In this paper we address both issues by demonstrating how a well-known 2D AF, MnP(S,Se)$_3$ can be functionalized into strong AM by applying out-of-plane electric field. Of particular interest is th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2309.02355","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/2309.02355/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":"2309.02355","created_at":"2026-07-05T06:47:59.104840+00:00"},{"alias_kind":"arxiv_version","alias_value":"2309.02355v1","created_at":"2026-07-05T06:47:59.104840+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2309.02355","created_at":"2026-07-05T06:47:59.104840+00:00"},{"alias_kind":"pith_short_12","alias_value":"UHY6Z75XO6SF","created_at":"2026-07-05T06:47:59.104840+00:00"},{"alias_kind":"pith_short_16","alias_value":"UHY6Z75XO6SFP2RP","created_at":"2026-07-05T06:47:59.104840+00:00"},{"alias_kind":"pith_short_8","alias_value":"UHY6Z75X","created_at":"2026-07-05T06:47:59.104840+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":17,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.26239","citing_title":"Anomalous Hall viscosity of altermagnets","ref_index":71,"is_internal_anchor":false},{"citing_arxiv_id":"2606.19903","citing_title":"Symmetry enforced quantum spin Hall effect in Altermagnets","ref_index":54,"is_internal_anchor":false},{"citing_arxiv_id":"2606.11128","citing_title":"Roughness-robust surface altermagnetism in $PT$ antiferromagnets","ref_index":32,"is_internal_anchor":false},{"citing_arxiv_id":"2605.26075","citing_title":"Observation of the Optical Phonons in {\\alpha}-MnTe films","ref_index":19,"is_internal_anchor":false},{"citing_arxiv_id":"2510.00509","citing_title":"Orbital Altermagnetism in Two Dimensions","ref_index":98,"is_internal_anchor":false},{"citing_arxiv_id":"2309.01607","citing_title":"P-wave magnets","ref_index":28,"is_internal_anchor":false},{"citing_arxiv_id":"2508.01564","citing_title":"Unconventional Altermagnetism in Quasicrystals: A Hyperspatial Projective Construction","ref_index":85,"is_internal_anchor":false},{"citing_arxiv_id":"2508.04788","citing_title":"Quantum-impurity sensing of altermagnetic order","ref_index":9,"is_internal_anchor":false},{"citing_arxiv_id":"2510.02451","citing_title":"Slow-phonon control of spin Edelstein effect in Rashba $d$-wave altermagnets","ref_index":43,"is_internal_anchor":false},{"citing_arxiv_id":"2601.10183","citing_title":"Classification and design of two-dimensional altermagnets","ref_index":110,"is_internal_anchor":false},{"citing_arxiv_id":"2604.02790","citing_title":"A Route to Nonrelativistic Altermagnetic Spin Splitting via Ultrafast Light","ref_index":26,"is_internal_anchor":false},{"citing_arxiv_id":"2604.26239","citing_title":"Coexistence of d-Wave Altermagnetism and Topological States in Janus FeSeX (X = S, Te) Monolayers","ref_index":15,"is_internal_anchor":false},{"citing_arxiv_id":"2604.10768","citing_title":"Vacancy-driven inverse Lieb geometry: A general route to $d$-wave altermagnetism in two dimensions","ref_index":23,"is_internal_anchor":false},{"citing_arxiv_id":"2605.03026","citing_title":"Tunable Odd-Parity Spin Splittings in Altermagnets","ref_index":35,"is_internal_anchor":false},{"citing_arxiv_id":"2604.10768","citing_title":"Vacancy-driven inverse Lieb geometry: A general route to $d$-wave altermagnetism in two dimensions","ref_index":23,"is_internal_anchor":false},{"citing_arxiv_id":"2605.07656","citing_title":"Finite temperature pair density wave superconductivity in $d$-wave altermagnets","ref_index":64,"is_internal_anchor":false},{"citing_arxiv_id":"2604.19661","citing_title":"Intrinsic i-wave altermagnetism in 2D graphene superlattices","ref_index":21,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UHY6Z75XO6SFP2RPNVHSC6XVE5","json":"https://pith.science/pith/UHY6Z75XO6SFP2RPNVHSC6XVE5.json","graph_json":"https://pith.science/api/pith-number/UHY6Z75XO6SFP2RPNVHSC6XVE5/graph.json","events_json":"https://pith.science/api/pith-number/UHY6Z75XO6SFP2RPNVHSC6XVE5/events.json","paper":"https://pith.science/paper/UHY6Z75X"},"agent_actions":{"view_html":"https://pith.science/pith/UHY6Z75XO6SFP2RPNVHSC6XVE5","download_json":"https://pith.science/pith/UHY6Z75XO6SFP2RPNVHSC6XVE5.json","view_paper":"https://pith.science/paper/UHY6Z75X","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2309.02355&json=true","fetch_graph":"https://pith.science/api/pith-number/UHY6Z75XO6SFP2RPNVHSC6XVE5/graph.json","fetch_events":"https://pith.science/api/pith-number/UHY6Z75XO6SFP2RPNVHSC6XVE5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UHY6Z75XO6SFP2RPNVHSC6XVE5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UHY6Z75XO6SFP2RPNVHSC6XVE5/action/storage_attestation","attest_author":"https://pith.science/pith/UHY6Z75XO6SFP2RPNVHSC6XVE5/action/author_attestation","sign_citation":"https://pith.science/pith/UHY6Z75XO6SFP2RPNVHSC6XVE5/action/citation_signature","submit_replication":"https://pith.science/pith/UHY6Z75XO6SFP2RPNVHSC6XVE5/action/replication_record"}},"created_at":"2026-07-05T06:47:59.104840+00:00","updated_at":"2026-07-05T06:47:59.104840+00:00"}