{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:X46HK7YJM4ESDCSPGXMCOJ23AI","short_pith_number":"pith:X46HK7YJ","schema_version":"1.0","canonical_sha256":"bf3c757f096709218a4f35d827275b0205c317f62344981a7c1facae660abe62","source":{"kind":"arxiv","id":"2503.23351","version":1},"attestation_state":"computed","paper":{"title":"Weak scattering formulation for flexural waves in thin elastic plates with point-like resonators","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.app-ph","authors_text":"Marc Mart\\'i-Sabat\\'e, Mario L\\'azaro, Richard V. Craster, Vicent Romero-Garc\\'ia","submitted_at":"2025-03-30T08:15:44Z","abstract_excerpt":"A theoretical study on the weak scattering formulation for flexural waves in thin elastic plates loaded by point-like resonators is reported. Our approach employs the Born approximation and far-field asymptotics of the Green function to characterize multiple scattering effects in this system. The response of the system to an incident wave can be expressed as a power series expansion, where each term introduces higher-order scattering components. The behavior of this series is governed by the spectral properties of a specific matrix, which dictates the convergence and accuracy of the weak scatt"},"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":"2503.23351","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.app-ph","submitted_at":"2025-03-30T08:15:44Z","cross_cats_sorted":[],"title_canon_sha256":"e33eb1839c4cb60aa0a0cb4cfd93d81f50f4eb5a201bc4d1fa2f6893c4d2c7de","abstract_canon_sha256":"765040f2c86899658fe96c32a021c4872b60f16deb97795da53f29124d31ebf0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:41:34.844602Z","signature_b64":"nIlzKBJKj8ovg4RCBTOFoZDmZyv7Q8UvexOLZbBPBLrHaArmA86Z4GT+bPPJ/7UsZpE8j3k5tcW1/FUqwwVvAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bf3c757f096709218a4f35d827275b0205c317f62344981a7c1facae660abe62","last_reissued_at":"2026-07-05T10:41:34.844104Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:41:34.844104Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Weak scattering formulation for flexural waves in thin elastic plates with point-like resonators","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.app-ph","authors_text":"Marc Mart\\'i-Sabat\\'e, Mario L\\'azaro, Richard V. Craster, Vicent Romero-Garc\\'ia","submitted_at":"2025-03-30T08:15:44Z","abstract_excerpt":"A theoretical study on the weak scattering formulation for flexural waves in thin elastic plates loaded by point-like resonators is reported. Our approach employs the Born approximation and far-field asymptotics of the Green function to characterize multiple scattering effects in this system. The response of the system to an incident wave can be expressed as a power series expansion, where each term introduces higher-order scattering components. The behavior of this series is governed by the spectral properties of a specific matrix, which dictates the convergence and accuracy of the weak scatt"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2503.23351","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/2503.23351/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":"2503.23351","created_at":"2026-07-05T10:41:34.844170+00:00"},{"alias_kind":"arxiv_version","alias_value":"2503.23351v1","created_at":"2026-07-05T10:41:34.844170+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2503.23351","created_at":"2026-07-05T10:41:34.844170+00:00"},{"alias_kind":"pith_short_12","alias_value":"X46HK7YJM4ES","created_at":"2026-07-05T10:41:34.844170+00:00"},{"alias_kind":"pith_short_16","alias_value":"X46HK7YJM4ESDCSP","created_at":"2026-07-05T10:41:34.844170+00:00"},{"alias_kind":"pith_short_8","alias_value":"X46HK7YJ","created_at":"2026-07-05T10:41:34.844170+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.18768","citing_title":"Scattering of Antiplane Shear Waves by Fractals in Strain Gradient Elasticity","ref_index":17,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/X46HK7YJM4ESDCSPGXMCOJ23AI","json":"https://pith.science/pith/X46HK7YJM4ESDCSPGXMCOJ23AI.json","graph_json":"https://pith.science/api/pith-number/X46HK7YJM4ESDCSPGXMCOJ23AI/graph.json","events_json":"https://pith.science/api/pith-number/X46HK7YJM4ESDCSPGXMCOJ23AI/events.json","paper":"https://pith.science/paper/X46HK7YJ"},"agent_actions":{"view_html":"https://pith.science/pith/X46HK7YJM4ESDCSPGXMCOJ23AI","download_json":"https://pith.science/pith/X46HK7YJM4ESDCSPGXMCOJ23AI.json","view_paper":"https://pith.science/paper/X46HK7YJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2503.23351&json=true","fetch_graph":"https://pith.science/api/pith-number/X46HK7YJM4ESDCSPGXMCOJ23AI/graph.json","fetch_events":"https://pith.science/api/pith-number/X46HK7YJM4ESDCSPGXMCOJ23AI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/X46HK7YJM4ESDCSPGXMCOJ23AI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/X46HK7YJM4ESDCSPGXMCOJ23AI/action/storage_attestation","attest_author":"https://pith.science/pith/X46HK7YJM4ESDCSPGXMCOJ23AI/action/author_attestation","sign_citation":"https://pith.science/pith/X46HK7YJM4ESDCSPGXMCOJ23AI/action/citation_signature","submit_replication":"https://pith.science/pith/X46HK7YJM4ESDCSPGXMCOJ23AI/action/replication_record"}},"created_at":"2026-07-05T10:41:34.844170+00:00","updated_at":"2026-07-05T10:41:34.844170+00:00"}