{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:ZDTZ7QUHTHUEV7FUC2A2DNPW5T","short_pith_number":"pith:ZDTZ7QUH","schema_version":"1.0","canonical_sha256":"c8e79fc28799e84afcb41681a1b5f6ecc05e2cf266c6fa25826dbe7a008a7e0c","source":{"kind":"arxiv","id":"1812.04504","version":1},"attestation_state":"computed","paper":{"title":"Linear Second Order Energy Stable Schemes of Phase Field Model with Nonlocal Constraints for Crystal Growth","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"math.NA","authors_text":"Qi Wang, Xiaobo Jing","submitted_at":"2018-12-10T13:31:49Z","abstract_excerpt":"We present a set of linear, second order, unconditionally energy stable schemes for the Allen-Cahn model with a nonlocal constraint for crystal growth that conserves the mass of each phase. Solvability conditions are established for the linear systems resulting from the linear schemes. Convergence rates are verified numerically. Dynamics obtained using the nonlocal Allen-Cahn model are compared with the one obtained using the classic Allen-Cahn model as well as the Cahn-Hilliard model, demonstrating slower dynamics than that of the Allen-Cahn model but faster dynamics than that of the Cahn-Hil"},"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":"1812.04504","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.NA","submitted_at":"2018-12-10T13:31:49Z","cross_cats_sorted":[],"title_canon_sha256":"b29b0b91f624914a46cdfb976eb3011e9200d1df69993e0aa05402d9a4cca557","abstract_canon_sha256":"a8ffee4149428888524f4d1f299005bd6f75e4f6dfc48822ee0f0b9376f96bd0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:58:31.828444Z","signature_b64":"Foc1RRnQi4cPTIiXvMC8jIBcElz4OhMDzllJBNJ2XjYjIpp5Cx9vvA2PC9sDAAkAdTtCSkimW1l9RnTh5EZBCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c8e79fc28799e84afcb41681a1b5f6ecc05e2cf266c6fa25826dbe7a008a7e0c","last_reissued_at":"2026-05-17T23:58:31.827922Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:58:31.827922Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Linear Second Order Energy Stable Schemes of Phase Field Model with Nonlocal Constraints for Crystal Growth","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"math.NA","authors_text":"Qi Wang, Xiaobo Jing","submitted_at":"2018-12-10T13:31:49Z","abstract_excerpt":"We present a set of linear, second order, unconditionally energy stable schemes for the Allen-Cahn model with a nonlocal constraint for crystal growth that conserves the mass of each phase. Solvability conditions are established for the linear systems resulting from the linear schemes. Convergence rates are verified numerically. Dynamics obtained using the nonlocal Allen-Cahn model are compared with the one obtained using the classic Allen-Cahn model as well as the Cahn-Hilliard model, demonstrating slower dynamics than that of the Allen-Cahn model but faster dynamics than that of the Cahn-Hil"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.04504","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":"1812.04504","created_at":"2026-05-17T23:58:31.827998+00:00"},{"alias_kind":"arxiv_version","alias_value":"1812.04504v1","created_at":"2026-05-17T23:58:31.827998+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.04504","created_at":"2026-05-17T23:58:31.827998+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZDTZ7QUHTHUE","created_at":"2026-05-18T12:33:07.085635+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZDTZ7QUHTHUEV7FU","created_at":"2026-05-18T12:33:07.085635+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZDTZ7QUH","created_at":"2026-05-18T12:33:07.085635+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/ZDTZ7QUHTHUEV7FUC2A2DNPW5T","json":"https://pith.science/pith/ZDTZ7QUHTHUEV7FUC2A2DNPW5T.json","graph_json":"https://pith.science/api/pith-number/ZDTZ7QUHTHUEV7FUC2A2DNPW5T/graph.json","events_json":"https://pith.science/api/pith-number/ZDTZ7QUHTHUEV7FUC2A2DNPW5T/events.json","paper":"https://pith.science/paper/ZDTZ7QUH"},"agent_actions":{"view_html":"https://pith.science/pith/ZDTZ7QUHTHUEV7FUC2A2DNPW5T","download_json":"https://pith.science/pith/ZDTZ7QUHTHUEV7FUC2A2DNPW5T.json","view_paper":"https://pith.science/paper/ZDTZ7QUH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1812.04504&json=true","fetch_graph":"https://pith.science/api/pith-number/ZDTZ7QUHTHUEV7FUC2A2DNPW5T/graph.json","fetch_events":"https://pith.science/api/pith-number/ZDTZ7QUHTHUEV7FUC2A2DNPW5T/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZDTZ7QUHTHUEV7FUC2A2DNPW5T/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZDTZ7QUHTHUEV7FUC2A2DNPW5T/action/storage_attestation","attest_author":"https://pith.science/pith/ZDTZ7QUHTHUEV7FUC2A2DNPW5T/action/author_attestation","sign_citation":"https://pith.science/pith/ZDTZ7QUHTHUEV7FUC2A2DNPW5T/action/citation_signature","submit_replication":"https://pith.science/pith/ZDTZ7QUHTHUEV7FUC2A2DNPW5T/action/replication_record"}},"created_at":"2026-05-17T23:58:31.827998+00:00","updated_at":"2026-05-17T23:58:31.827998+00:00"}