{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:CIFTNQHVT4XHFJVJJBWOBUFOAI","short_pith_number":"pith:CIFTNQHV","canonical_record":{"source":{"id":"2604.22523","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2026-04-24T13:07:43Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.str-el"],"title_canon_sha256":"d51667f03021dad7cc750c6ff4cf441407e5898574e4bd802f85b7f5b1a8f2ba","abstract_canon_sha256":"70105b2de4dcd27df4d4efd29af140776c36056ad3231edd62d1fb8a4b614e73"},"schema_version":"1.0"},"canonical_sha256":"120b36c0f59f2e72a6a9486ce0d0ae0226e5f0d479914fc317d268a59b5ba77d","source":{"kind":"arxiv","id":"2604.22523","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2604.22523","created_at":"2026-05-26T01:03:31Z"},{"alias_kind":"arxiv_version","alias_value":"2604.22523v2","created_at":"2026-05-26T01:03:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2604.22523","created_at":"2026-05-26T01:03:31Z"},{"alias_kind":"pith_short_12","alias_value":"CIFTNQHVT4XH","created_at":"2026-05-26T01:03:31Z"},{"alias_kind":"pith_short_16","alias_value":"CIFTNQHVT4XHFJVJ","created_at":"2026-05-26T01:03:31Z"},{"alias_kind":"pith_short_8","alias_value":"CIFTNQHV","created_at":"2026-05-26T01:03:31Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:CIFTNQHVT4XHFJVJJBWOBUFOAI","target":"record","payload":{"canonical_record":{"source":{"id":"2604.22523","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2026-04-24T13:07:43Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.str-el"],"title_canon_sha256":"d51667f03021dad7cc750c6ff4cf441407e5898574e4bd802f85b7f5b1a8f2ba","abstract_canon_sha256":"70105b2de4dcd27df4d4efd29af140776c36056ad3231edd62d1fb8a4b614e73"},"schema_version":"1.0"},"canonical_sha256":"120b36c0f59f2e72a6a9486ce0d0ae0226e5f0d479914fc317d268a59b5ba77d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-26T01:03:31.057447Z","signature_b64":"v/1YOqupyBSVa6b1UQ+3YLuIw2pH1vK6m8Oj01c0HhUHL19SKiBNuto4lsbernbVmvCo7FZ7BqHJC2HO5mQiBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"120b36c0f59f2e72a6a9486ce0d0ae0226e5f0d479914fc317d268a59b5ba77d","last_reissued_at":"2026-05-26T01:03:31.056586Z","signature_status":"signed_v1","first_computed_at":"2026-05-26T01:03:31.056586Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2604.22523","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-26T01:03:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Iqyuneq477+P+JhT/LhmVoOHdJpX/zDACDvUlDWgIB1QRSaU8a9YfEvodLHf4FGO7NGKsYLShdsoDM1MVGm2Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T23:30:49.699819Z"},"content_sha256":"00dcea8e59a22d4cbe51fc941c2297c8889b1b0c6621040f18977ea4a1c821e8","schema_version":"1.0","event_id":"sha256:00dcea8e59a22d4cbe51fc941c2297c8889b1b0c6621040f18977ea4a1c821e8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:CIFTNQHVT4XHFJVJJBWOBUFOAI","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Magnetoelastic Waves in Ferromagnetic Thin Films Mediated by Dipolar Interactions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"Dipolar interactions in thin ferromagnetic films hybridize magnetostatic and Lamb waves through coupled elastic and magnetic deformations.","cross_cats":["cond-mat.mes-hall","cond-mat.str-el"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Daiki Hatanaka, Hiroki Yoshida, Kei Yamamoto, Manato Fujimoto, Motoki Asano, Ryohei Kono, Shuichi Murakami","submitted_at":"2026-04-24T13:07:43Z","abstract_excerpt":"Magnetoelastic coupling mediated by magnetic dipolar interactions is theoretically investigated in ferromagnetic thin films under an in-plane magnetic field. We develop a theoretical description that incorporates dipolar fields derived from Maxwell's equations in the presence of elastic deformations. The resulting coupled equations of motion predict hybridization between magnetostatic and Lamb waves. Numerical calculations for a yttrium iron garnet (YIG) film reveal anti-crossings in the dispersion relations, with hybridization gaps ranging from $0.1$ to several MHz."},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"The resulting coupled equations of motion predict hybridization between magnetostatic and Lamb waves. Numerical calculations for a yttrium iron garnet (YIG) film reveal anti-crossings in the dispersion relations, with hybridization gaps ranging from 0.1 to several MHz.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"The theoretical description assumes dipolar fields derived from Maxwell's equations remain valid and accurately coupled to elastic deformations in thin films without additional boundary or approximation details that could alter the hybridization gaps.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"Dipolar interactions mediate magnetoelastic coupling in ferromagnetic thin films, hybridizing magnetostatic and Lamb waves with hybridization gaps of 0.1 to several MHz in YIG.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"Dipolar interactions in thin ferromagnetic films hybridize magnetostatic and Lamb waves through coupled elastic and magnetic deformations.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"20e1d6cc8721ba67316e307b540fc484b2fa653136b8e1a976fe78ceadfef370"},"source":{"id":"2604.22523","kind":"arxiv","version":2},"verdict":{"id":"e43196a5-edb9-4dd4-97ce-0cefddb24ac6","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-08T11:09:42.566387Z","strongest_claim":"The resulting coupled equations of motion predict hybridization between magnetostatic and Lamb waves. Numerical calculations for a yttrium iron garnet (YIG) film reveal anti-crossings in the dispersion relations, with hybridization gaps ranging from 0.1 to several MHz.","one_line_summary":"Dipolar interactions mediate magnetoelastic coupling in ferromagnetic thin films, hybridizing magnetostatic and Lamb waves with hybridization gaps of 0.1 to several MHz in YIG.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"The theoretical description assumes dipolar fields derived from Maxwell's equations remain valid and accurately coupled to elastic deformations in thin films without additional boundary or approximation details that could alter the hybridization gaps.","pith_extraction_headline":"Dipolar interactions in thin ferromagnetic films hybridize magnetostatic and Lamb waves through coupled elastic and magnetic deformations."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2604.22523/integrity.json","findings":[],"available":true,"detectors_run":[{"name":"ai_meta_artifact","ran_at":"2026-05-21T10:38:42.087421Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"doi_compliance","ran_at":"2026-05-19T23:54:57.742747Z","status":"completed","version":"1.0.0","findings_count":0}],"snapshot_sha256":"d396d4abe9031a5a7e3bd5739ac2789eae6e6f94126506614cb9077c95307d86"},"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"},"verdict_id":"e43196a5-edb9-4dd4-97ce-0cefddb24ac6"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-26T01:03:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"e8O2jTO80OMOUJWwuZR/tiv05dbcXuPN2WwgjukUvy8mwNrOiQUwsb7DcXQZtANqIq5CL0EmVSasFe3VEQsDAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T23:30:49.700369Z"},"content_sha256":"8d73cf1215e0fa93e7155dc985a44a896bcd03ec5ad6362b93858dbff51f8520","schema_version":"1.0","event_id":"sha256:8d73cf1215e0fa93e7155dc985a44a896bcd03ec5ad6362b93858dbff51f8520"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/CIFTNQHVT4XHFJVJJBWOBUFOAI/bundle.json","state_url":"https://pith.science/pith/CIFTNQHVT4XHFJVJJBWOBUFOAI/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/CIFTNQHVT4XHFJVJJBWOBUFOAI/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-01T23:30:49Z","links":{"resolver":"https://pith.science/pith/CIFTNQHVT4XHFJVJJBWOBUFOAI","bundle":"https://pith.science/pith/CIFTNQHVT4XHFJVJJBWOBUFOAI/bundle.json","state":"https://pith.science/pith/CIFTNQHVT4XHFJVJJBWOBUFOAI/state.json","well_known_bundle":"https://pith.science/.well-known/pith/CIFTNQHVT4XHFJVJJBWOBUFOAI/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:CIFTNQHVT4XHFJVJJBWOBUFOAI","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"70105b2de4dcd27df4d4efd29af140776c36056ad3231edd62d1fb8a4b614e73","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.str-el"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2026-04-24T13:07:43Z","title_canon_sha256":"d51667f03021dad7cc750c6ff4cf441407e5898574e4bd802f85b7f5b1a8f2ba"},"schema_version":"1.0","source":{"id":"2604.22523","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2604.22523","created_at":"2026-05-26T01:03:31Z"},{"alias_kind":"arxiv_version","alias_value":"2604.22523v2","created_at":"2026-05-26T01:03:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2604.22523","created_at":"2026-05-26T01:03:31Z"},{"alias_kind":"pith_short_12","alias_value":"CIFTNQHVT4XH","created_at":"2026-05-26T01:03:31Z"},{"alias_kind":"pith_short_16","alias_value":"CIFTNQHVT4XHFJVJ","created_at":"2026-05-26T01:03:31Z"},{"alias_kind":"pith_short_8","alias_value":"CIFTNQHV","created_at":"2026-05-26T01:03:31Z"}],"graph_snapshots":[{"event_id":"sha256:8d73cf1215e0fa93e7155dc985a44a896bcd03ec5ad6362b93858dbff51f8520","target":"graph","created_at":"2026-05-26T01:03:31Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":4,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","text":"The resulting coupled equations of motion predict hybridization between magnetostatic and Lamb waves. Numerical calculations for a yttrium iron garnet (YIG) film reveal anti-crossings in the dispersion relations, with hybridization gaps ranging from 0.1 to several MHz."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"The theoretical description assumes dipolar fields derived from Maxwell's equations remain valid and accurately coupled to elastic deformations in thin films without additional boundary or approximation details that could alter the hybridization gaps."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"Dipolar interactions mediate magnetoelastic coupling in ferromagnetic thin films, hybridizing magnetostatic and Lamb waves with hybridization gaps of 0.1 to several MHz in YIG."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"Dipolar interactions in thin ferromagnetic films hybridize magnetostatic and Lamb waves through coupled elastic and magnetic deformations."}],"snapshot_sha256":"20e1d6cc8721ba67316e307b540fc484b2fa653136b8e1a976fe78ceadfef370"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[{"findings_count":0,"name":"ai_meta_artifact","ran_at":"2026-05-21T10:38:42.087421Z","status":"completed","version":"1.0.0"},{"findings_count":0,"name":"doi_compliance","ran_at":"2026-05-19T23:54:57.742747Z","status":"completed","version":"1.0.0"}],"endpoint":"/pith/2604.22523/integrity.json","findings":[],"snapshot_sha256":"d396d4abe9031a5a7e3bd5739ac2789eae6e6f94126506614cb9077c95307d86","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Magnetoelastic coupling mediated by magnetic dipolar interactions is theoretically investigated in ferromagnetic thin films under an in-plane magnetic field. We develop a theoretical description that incorporates dipolar fields derived from Maxwell's equations in the presence of elastic deformations. The resulting coupled equations of motion predict hybridization between magnetostatic and Lamb waves. Numerical calculations for a yttrium iron garnet (YIG) film reveal anti-crossings in the dispersion relations, with hybridization gaps ranging from $0.1$ to several MHz.","authors_text":"Daiki Hatanaka, Hiroki Yoshida, Kei Yamamoto, Manato Fujimoto, Motoki Asano, Ryohei Kono, Shuichi Murakami","cross_cats":["cond-mat.mes-hall","cond-mat.str-el"],"headline":"Dipolar interactions in thin ferromagnetic films hybridize magnetostatic and Lamb waves through coupled elastic and magnetic deformations.","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2026-04-24T13:07:43Z","title":"Magnetoelastic Waves in Ferromagnetic Thin Films Mediated by Dipolar Interactions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2604.22523","kind":"arxiv","version":2},"verdict":{"created_at":"2026-05-08T11:09:42.566387Z","id":"e43196a5-edb9-4dd4-97ce-0cefddb24ac6","model_set":{"reader":"grok-4.3"},"one_line_summary":"Dipolar interactions mediate magnetoelastic coupling in ferromagnetic thin films, hybridizing magnetostatic and Lamb waves with hybridization gaps of 0.1 to several MHz in YIG.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"Dipolar interactions in thin ferromagnetic films hybridize magnetostatic and Lamb waves through coupled elastic and magnetic deformations.","strongest_claim":"The resulting coupled equations of motion predict hybridization between magnetostatic and Lamb waves. Numerical calculations for a yttrium iron garnet (YIG) film reveal anti-crossings in the dispersion relations, with hybridization gaps ranging from 0.1 to several MHz.","weakest_assumption":"The theoretical description assumes dipolar fields derived from Maxwell's equations remain valid and accurately coupled to elastic deformations in thin films without additional boundary or approximation details that could alter the hybridization gaps."}},"verdict_id":"e43196a5-edb9-4dd4-97ce-0cefddb24ac6"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:00dcea8e59a22d4cbe51fc941c2297c8889b1b0c6621040f18977ea4a1c821e8","target":"record","created_at":"2026-05-26T01:03:31Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"70105b2de4dcd27df4d4efd29af140776c36056ad3231edd62d1fb8a4b614e73","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.str-el"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2026-04-24T13:07:43Z","title_canon_sha256":"d51667f03021dad7cc750c6ff4cf441407e5898574e4bd802f85b7f5b1a8f2ba"},"schema_version":"1.0","source":{"id":"2604.22523","kind":"arxiv","version":2}},"canonical_sha256":"120b36c0f59f2e72a6a9486ce0d0ae0226e5f0d479914fc317d268a59b5ba77d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"120b36c0f59f2e72a6a9486ce0d0ae0226e5f0d479914fc317d268a59b5ba77d","first_computed_at":"2026-05-26T01:03:31.056586Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-26T01:03:31.056586Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"v/1YOqupyBSVa6b1UQ+3YLuIw2pH1vK6m8Oj01c0HhUHL19SKiBNuto4lsbernbVmvCo7FZ7BqHJC2HO5mQiBg==","signature_status":"signed_v1","signed_at":"2026-05-26T01:03:31.057447Z","signed_message":"canonical_sha256_bytes"},"source_id":"2604.22523","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:00dcea8e59a22d4cbe51fc941c2297c8889b1b0c6621040f18977ea4a1c821e8","sha256:8d73cf1215e0fa93e7155dc985a44a896bcd03ec5ad6362b93858dbff51f8520"],"state_sha256":"324af11c78e72a805b3ebc378a9c47d21342cb9013ac063d8d009e3fc673d473"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"of3PuO5ehrivoosG7AW7HSExVlkIwV4l3Rr0nbCmhVCu4Ox3H0G29GB7NoeZQdbZEYHbJyaHcUEozlZef/+FDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T23:30:49.702892Z","bundle_sha256":"8bbed3e2a74f1f0e78fec77ed1596bf8fbe80e6cc4995acb969743ff28202a15"}}