{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:PDL2TAUZYAOLO7HV46ZTXPYMBZ","short_pith_number":"pith:PDL2TAUZ","schema_version":"1.0","canonical_sha256":"78d7a98299c01cb77cf5e7b33bbf0c0e47bb8dddc30053eecfb95f1757902948","source":{"kind":"arxiv","id":"2506.07051","version":1},"attestation_state":"computed","paper":{"title":"All-optical control of antiferromagnetic domains via an inverse optical magnetoelectric effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Istv\\'an K\\'ezsm\\'arki, Naoki Ogawa, Shingo Toyoda, Taka-hisa Arima, Vilmos Kocsis, Yasujiro Taguchi, Yoshinori Tokura, Yusuke Tokunaga","submitted_at":"2025-06-08T09:21:47Z","abstract_excerpt":"Antiferromagnets are a promising platform for next-generation spintronics due to their ultrafast spin dynamics and robustness to external fields. All-optical control of antiferromagnetic order is essential to fully exploit their potential in energy-efficient and high-speed spintronic and memory applications. However, optical writing of antiferromagnetic domains remains a fundamental challenge, as conventional magneto-optical techniques rely on net magnetization, which is absent in antiferromagnets. In certain multiferroic antiferromagnets, the magnetic toroidal moment provides an additional de"},"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":"2506.07051","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2025-06-08T09:21:47Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"38c2dedc724b6102dc79065de83020547b0d70e93b4130238aff38d3a917e2f0","abstract_canon_sha256":"d4dcaf50d4d6ff20153abec085673d89833f6848479311442e4c80077de723c4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:18:00.383599Z","signature_b64":"9LYqZPjULkZ9VM8cC8Fy168UN+nV0rYQy29m4OzyJaJR109et9e9sirwRaH8yokH6KqPEeLDaS7qDxF287X9Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"78d7a98299c01cb77cf5e7b33bbf0c0e47bb8dddc30053eecfb95f1757902948","last_reissued_at":"2026-07-05T11:18:00.383090Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:18:00.383090Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"All-optical control of antiferromagnetic domains via an inverse optical magnetoelectric effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Istv\\'an K\\'ezsm\\'arki, Naoki Ogawa, Shingo Toyoda, Taka-hisa Arima, Vilmos Kocsis, Yasujiro Taguchi, Yoshinori Tokura, Yusuke Tokunaga","submitted_at":"2025-06-08T09:21:47Z","abstract_excerpt":"Antiferromagnets are a promising platform for next-generation spintronics due to their ultrafast spin dynamics and robustness to external fields. All-optical control of antiferromagnetic order is essential to fully exploit their potential in energy-efficient and high-speed spintronic and memory applications. However, optical writing of antiferromagnetic domains remains a fundamental challenge, as conventional magneto-optical techniques rely on net magnetization, which is absent in antiferromagnets. In certain multiferroic antiferromagnets, the magnetic toroidal moment provides an additional de"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.07051","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/2506.07051/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":"2506.07051","created_at":"2026-07-05T11:18:00.383146+00:00"},{"alias_kind":"arxiv_version","alias_value":"2506.07051v1","created_at":"2026-07-05T11:18:00.383146+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.07051","created_at":"2026-07-05T11:18:00.383146+00:00"},{"alias_kind":"pith_short_12","alias_value":"PDL2TAUZYAOL","created_at":"2026-07-05T11:18:00.383146+00:00"},{"alias_kind":"pith_short_16","alias_value":"PDL2TAUZYAOLO7HV","created_at":"2026-07-05T11:18:00.383146+00:00"},{"alias_kind":"pith_short_8","alias_value":"PDL2TAUZ","created_at":"2026-07-05T11:18:00.383146+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2601.04811","citing_title":"Switching magnetization of quantum antiferromagnets: Schwinger boson mean-field theory compared to exact diagonalization","ref_index":29,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PDL2TAUZYAOLO7HV46ZTXPYMBZ","json":"https://pith.science/pith/PDL2TAUZYAOLO7HV46ZTXPYMBZ.json","graph_json":"https://pith.science/api/pith-number/PDL2TAUZYAOLO7HV46ZTXPYMBZ/graph.json","events_json":"https://pith.science/api/pith-number/PDL2TAUZYAOLO7HV46ZTXPYMBZ/events.json","paper":"https://pith.science/paper/PDL2TAUZ"},"agent_actions":{"view_html":"https://pith.science/pith/PDL2TAUZYAOLO7HV46ZTXPYMBZ","download_json":"https://pith.science/pith/PDL2TAUZYAOLO7HV46ZTXPYMBZ.json","view_paper":"https://pith.science/paper/PDL2TAUZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2506.07051&json=true","fetch_graph":"https://pith.science/api/pith-number/PDL2TAUZYAOLO7HV46ZTXPYMBZ/graph.json","fetch_events":"https://pith.science/api/pith-number/PDL2TAUZYAOLO7HV46ZTXPYMBZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PDL2TAUZYAOLO7HV46ZTXPYMBZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PDL2TAUZYAOLO7HV46ZTXPYMBZ/action/storage_attestation","attest_author":"https://pith.science/pith/PDL2TAUZYAOLO7HV46ZTXPYMBZ/action/author_attestation","sign_citation":"https://pith.science/pith/PDL2TAUZYAOLO7HV46ZTXPYMBZ/action/citation_signature","submit_replication":"https://pith.science/pith/PDL2TAUZYAOLO7HV46ZTXPYMBZ/action/replication_record"}},"created_at":"2026-07-05T11:18:00.383146+00:00","updated_at":"2026-07-05T11:18:00.383146+00:00"}