{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:K25AADL5TI75OERFI4LJHJ3IDW","short_pith_number":"pith:K25AADL5","canonical_record":{"source":{"id":"1809.07663","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"math.NA","submitted_at":"2018-09-20T15:00:36Z","cross_cats_sorted":["cs.CE","physics.comp-ph"],"title_canon_sha256":"8ddf11413ce995e158efe4cde76aa432c676a7621d2625f61c87fb164cf80d47","abstract_canon_sha256":"eed5e1a0612c4cbd2e6eb79c8f7354f25144ee754319b9ce09aef9a31068bf07"},"schema_version":"1.0"},"canonical_sha256":"56ba000d7d9a3fd71225471693a7681dad6f0659f4b3b186de55a15c210685f3","source":{"kind":"arxiv","id":"1809.07663","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1809.07663","created_at":"2026-05-18T00:04:54Z"},{"alias_kind":"arxiv_version","alias_value":"1809.07663v2","created_at":"2026-05-18T00:04:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1809.07663","created_at":"2026-05-18T00:04:54Z"},{"alias_kind":"pith_short_12","alias_value":"K25AADL5TI75","created_at":"2026-05-18T12:32:33Z"},{"alias_kind":"pith_short_16","alias_value":"K25AADL5TI75OERF","created_at":"2026-05-18T12:32:33Z"},{"alias_kind":"pith_short_8","alias_value":"K25AADL5","created_at":"2026-05-18T12:32:33Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:K25AADL5TI75OERFI4LJHJ3IDW","target":"record","payload":{"canonical_record":{"source":{"id":"1809.07663","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"math.NA","submitted_at":"2018-09-20T15:00:36Z","cross_cats_sorted":["cs.CE","physics.comp-ph"],"title_canon_sha256":"8ddf11413ce995e158efe4cde76aa432c676a7621d2625f61c87fb164cf80d47","abstract_canon_sha256":"eed5e1a0612c4cbd2e6eb79c8f7354f25144ee754319b9ce09aef9a31068bf07"},"schema_version":"1.0"},"canonical_sha256":"56ba000d7d9a3fd71225471693a7681dad6f0659f4b3b186de55a15c210685f3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:04:54.361545Z","signature_b64":"LwitoZogo49Gv2WEpydqKcsg3jaGPItxPAcQKEukNT+m3pbDRrY6ET9Y4FF6oJFpp/3jdqrB71mIu81L7ts9CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"56ba000d7d9a3fd71225471693a7681dad6f0659f4b3b186de55a15c210685f3","last_reissued_at":"2026-05-18T00:04:54.360921Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:04:54.360921Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1809.07663","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":"2026-05-18T00:04:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"V7L2WV7jx6OWW/gbtSCjqu1yoFq1KHbA8LV3W9JCKgU+2CHDDreHQRFUSHEvL3UiF93jfNukiGXjuq7GGCRYBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T23:06:26.183064Z"},"content_sha256":"68734b620b43c1a6eea3472a0aa61c826e0f92e31b0a68350a27ac7b2f6fa326","schema_version":"1.0","event_id":"sha256:68734b620b43c1a6eea3472a0aa61c826e0f92e31b0a68350a27ac7b2f6fa326"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:K25AADL5TI75OERFI4LJHJ3IDW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Residual stresses in metal deposition modeling: discretizations of higher order","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cs.CE","physics.comp-ph"],"primary_cat":"math.NA","authors_text":"Ali \\\"Ozcan, Ernst Rank, John N. Jomo, Stefan Kollmannsberger","submitted_at":"2018-09-20T15:00:36Z","abstract_excerpt":"This article addresses the research question if and how the finite cell method, an embedded domain finite element method of high order, may be used in the simulation of metal deposition to harvest its computational efficiency. This application demands for the solution of a coupled thermo-elasto-plastic problem on transient meshes within which history variables need to be managed dynamically on non-boundary conforming discretizations. To this end, we propose to combine the multi-level hp-method and the finite cell method. The former was specifically designed to treat high-order finite element d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1809.07663","kind":"arxiv","version":2},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:04:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ltDoI7IhxMpoRrMjRyYoxXk+YXOiRZtpETATYfRAsOoYOx2sN1wAFtksgc/r7yv+haQ+kySZIM8RgHGmKpdFAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T23:06:26.183779Z"},"content_sha256":"cb82c0eef694fd03afd03af7f5931ffc468364740fddd5adb0fa33b0b27754af","schema_version":"1.0","event_id":"sha256:cb82c0eef694fd03afd03af7f5931ffc468364740fddd5adb0fa33b0b27754af"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/K25AADL5TI75OERFI4LJHJ3IDW/bundle.json","state_url":"https://pith.science/pith/K25AADL5TI75OERFI4LJHJ3IDW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/K25AADL5TI75OERFI4LJHJ3IDW/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":"2026-06-04T23:06:26Z","links":{"resolver":"https://pith.science/pith/K25AADL5TI75OERFI4LJHJ3IDW","bundle":"https://pith.science/pith/K25AADL5TI75OERFI4LJHJ3IDW/bundle.json","state":"https://pith.science/pith/K25AADL5TI75OERFI4LJHJ3IDW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/K25AADL5TI75OERFI4LJHJ3IDW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:K25AADL5TI75OERFI4LJHJ3IDW","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":"eed5e1a0612c4cbd2e6eb79c8f7354f25144ee754319b9ce09aef9a31068bf07","cross_cats_sorted":["cs.CE","physics.comp-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"math.NA","submitted_at":"2018-09-20T15:00:36Z","title_canon_sha256":"8ddf11413ce995e158efe4cde76aa432c676a7621d2625f61c87fb164cf80d47"},"schema_version":"1.0","source":{"id":"1809.07663","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1809.07663","created_at":"2026-05-18T00:04:54Z"},{"alias_kind":"arxiv_version","alias_value":"1809.07663v2","created_at":"2026-05-18T00:04:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1809.07663","created_at":"2026-05-18T00:04:54Z"},{"alias_kind":"pith_short_12","alias_value":"K25AADL5TI75","created_at":"2026-05-18T12:32:33Z"},{"alias_kind":"pith_short_16","alias_value":"K25AADL5TI75OERF","created_at":"2026-05-18T12:32:33Z"},{"alias_kind":"pith_short_8","alias_value":"K25AADL5","created_at":"2026-05-18T12:32:33Z"}],"graph_snapshots":[{"event_id":"sha256:cb82c0eef694fd03afd03af7f5931ffc468364740fddd5adb0fa33b0b27754af","target":"graph","created_at":"2026-05-18T00:04:54Z","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":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"This article addresses the research question if and how the finite cell method, an embedded domain finite element method of high order, may be used in the simulation of metal deposition to harvest its computational efficiency. This application demands for the solution of a coupled thermo-elasto-plastic problem on transient meshes within which history variables need to be managed dynamically on non-boundary conforming discretizations. To this end, we propose to combine the multi-level hp-method and the finite cell method. The former was specifically designed to treat high-order finite element d","authors_text":"Ali \\\"Ozcan, Ernst Rank, John N. Jomo, Stefan Kollmannsberger","cross_cats":["cs.CE","physics.comp-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"math.NA","submitted_at":"2018-09-20T15:00:36Z","title":"Residual stresses in metal deposition modeling: discretizations of higher order"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1809.07663","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:68734b620b43c1a6eea3472a0aa61c826e0f92e31b0a68350a27ac7b2f6fa326","target":"record","created_at":"2026-05-18T00:04:54Z","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":"eed5e1a0612c4cbd2e6eb79c8f7354f25144ee754319b9ce09aef9a31068bf07","cross_cats_sorted":["cs.CE","physics.comp-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"math.NA","submitted_at":"2018-09-20T15:00:36Z","title_canon_sha256":"8ddf11413ce995e158efe4cde76aa432c676a7621d2625f61c87fb164cf80d47"},"schema_version":"1.0","source":{"id":"1809.07663","kind":"arxiv","version":2}},"canonical_sha256":"56ba000d7d9a3fd71225471693a7681dad6f0659f4b3b186de55a15c210685f3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"56ba000d7d9a3fd71225471693a7681dad6f0659f4b3b186de55a15c210685f3","first_computed_at":"2026-05-18T00:04:54.360921Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:04:54.360921Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"LwitoZogo49Gv2WEpydqKcsg3jaGPItxPAcQKEukNT+m3pbDRrY6ET9Y4FF6oJFpp/3jdqrB71mIu81L7ts9CA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:04:54.361545Z","signed_message":"canonical_sha256_bytes"},"source_id":"1809.07663","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:68734b620b43c1a6eea3472a0aa61c826e0f92e31b0a68350a27ac7b2f6fa326","sha256:cb82c0eef694fd03afd03af7f5931ffc468364740fddd5adb0fa33b0b27754af"],"state_sha256":"91c49264da54a9db17973aff85432e57c0558c2d9e05a796646406afd98a43eb"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4oyE5xX5iC4bkO1mI9HyTp6dbmCjAHmtZbfEDQMRSEcWbxoSrcuihzafAkQoXXmOMKDDMaUL17iAD744nGIoCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-04T23:06:26.187464Z","bundle_sha256":"e4c610102dc03a0a5f8a27be85d85592b2e37fc27eee96802a4b08bd8ab9da05"}}