{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:AHACEHNLM6FQ5OPXJ2FF2KOSDN","short_pith_number":"pith:AHACEHNL","schema_version":"1.0","canonical_sha256":"01c0221dab678b0eb9f74e8a5d29d21b7a21fb880a469604262d77dd6eb8f319","source":{"kind":"arxiv","id":"1503.04403","version":1},"attestation_state":"computed","paper":{"title":"Numerical simulation of Faraday waves oscillated by two-frequency forcing","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"Kentaro Takagi, Takeshi Matsumoto","submitted_at":"2015-03-15T09:32:04Z","abstract_excerpt":"We perform a numerical simulation of Faraday waves forced with two-frequency oscillations using a level-set method with Lagrangian-particle corrections (particle level-set method). After validating the simulation with the linear stability analysis, we show that square, hexagonal and rhomboidal patterns are reproduced in agreement with the laboratory experiments [Arbell and Fineberg, Phys. Rev. Lett. 84, 654 (2000) and Phys. Rev. Lett. 85, 756 (2000)]. We also show that the particle level-set's high degree of conservation of volume is necessary in the simulations. The numerical results of the r"},"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":"1503.04403","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2015-03-15T09:32:04Z","cross_cats_sorted":[],"title_canon_sha256":"6bd290128a7a689309a17c157c75c39405edf2bb79a135511c02e6cba400b47d","abstract_canon_sha256":"e256b9a0c348f17816f571ebc30ce692d5e2d3d999156a2a58457c5ab2474875"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:20:12.133782Z","signature_b64":"vqIrI1zTulx8sQYSBEU0MlumwZCNI7EfpejbpzN8uKdHP+OHxc9WXh2iS3EqdlmIksDsE1MhZ0YIgdCQnJj1Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"01c0221dab678b0eb9f74e8a5d29d21b7a21fb880a469604262d77dd6eb8f319","last_reissued_at":"2026-05-18T02:20:12.133278Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:20:12.133278Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Numerical simulation of Faraday waves oscillated by two-frequency forcing","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"Kentaro Takagi, Takeshi Matsumoto","submitted_at":"2015-03-15T09:32:04Z","abstract_excerpt":"We perform a numerical simulation of Faraday waves forced with two-frequency oscillations using a level-set method with Lagrangian-particle corrections (particle level-set method). After validating the simulation with the linear stability analysis, we show that square, hexagonal and rhomboidal patterns are reproduced in agreement with the laboratory experiments [Arbell and Fineberg, Phys. Rev. Lett. 84, 654 (2000) and Phys. Rev. Lett. 85, 756 (2000)]. We also show that the particle level-set's high degree of conservation of volume is necessary in the simulations. The numerical results of the r"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1503.04403","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":""},"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":"1503.04403","created_at":"2026-05-18T02:20:12.133370+00:00"},{"alias_kind":"arxiv_version","alias_value":"1503.04403v1","created_at":"2026-05-18T02:20:12.133370+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1503.04403","created_at":"2026-05-18T02:20:12.133370+00:00"},{"alias_kind":"pith_short_12","alias_value":"AHACEHNLM6FQ","created_at":"2026-05-18T12:29:10.953037+00:00"},{"alias_kind":"pith_short_16","alias_value":"AHACEHNLM6FQ5OPX","created_at":"2026-05-18T12:29:10.953037+00:00"},{"alias_kind":"pith_short_8","alias_value":"AHACEHNL","created_at":"2026-05-18T12:29:10.953037+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/AHACEHNLM6FQ5OPXJ2FF2KOSDN","json":"https://pith.science/pith/AHACEHNLM6FQ5OPXJ2FF2KOSDN.json","graph_json":"https://pith.science/api/pith-number/AHACEHNLM6FQ5OPXJ2FF2KOSDN/graph.json","events_json":"https://pith.science/api/pith-number/AHACEHNLM6FQ5OPXJ2FF2KOSDN/events.json","paper":"https://pith.science/paper/AHACEHNL"},"agent_actions":{"view_html":"https://pith.science/pith/AHACEHNLM6FQ5OPXJ2FF2KOSDN","download_json":"https://pith.science/pith/AHACEHNLM6FQ5OPXJ2FF2KOSDN.json","view_paper":"https://pith.science/paper/AHACEHNL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1503.04403&json=true","fetch_graph":"https://pith.science/api/pith-number/AHACEHNLM6FQ5OPXJ2FF2KOSDN/graph.json","fetch_events":"https://pith.science/api/pith-number/AHACEHNLM6FQ5OPXJ2FF2KOSDN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AHACEHNLM6FQ5OPXJ2FF2KOSDN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AHACEHNLM6FQ5OPXJ2FF2KOSDN/action/storage_attestation","attest_author":"https://pith.science/pith/AHACEHNLM6FQ5OPXJ2FF2KOSDN/action/author_attestation","sign_citation":"https://pith.science/pith/AHACEHNLM6FQ5OPXJ2FF2KOSDN/action/citation_signature","submit_replication":"https://pith.science/pith/AHACEHNLM6FQ5OPXJ2FF2KOSDN/action/replication_record"}},"created_at":"2026-05-18T02:20:12.133370+00:00","updated_at":"2026-05-18T02:20:12.133370+00:00"}