{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2019:IYNXEHSTO2TBUV636YJUJKXV54","short_pith_number":"pith:IYNXEHST","canonical_record":{"source":{"id":"1901.01792","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.NA","submitted_at":"2019-01-07T13:22:57Z","cross_cats_sorted":["cs.NA"],"title_canon_sha256":"9f2c6483b0ce1778271f3350a9c726a552151123fb16eeec4c5bb890bd82f6d9","abstract_canon_sha256":"a3e9a264fc603ad0c849d9aa082728304af439c8feeeaa6560e372d81d678f33"},"schema_version":"1.0"},"canonical_sha256":"461b721e5376a61a57dbf61344aaf5ef31d18efa1446b251b15d9ad1b8c4bd48","source":{"kind":"arxiv","id":"1901.01792","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1901.01792","created_at":"2026-05-17T23:42:08Z"},{"alias_kind":"arxiv_version","alias_value":"1901.01792v2","created_at":"2026-05-17T23:42:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1901.01792","created_at":"2026-05-17T23:42:08Z"},{"alias_kind":"pith_short_12","alias_value":"IYNXEHSTO2TB","created_at":"2026-05-18T12:33:18Z"},{"alias_kind":"pith_short_16","alias_value":"IYNXEHSTO2TBUV63","created_at":"2026-05-18T12:33:18Z"},{"alias_kind":"pith_short_8","alias_value":"IYNXEHST","created_at":"2026-05-18T12:33:18Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2019:IYNXEHSTO2TBUV636YJUJKXV54","target":"record","payload":{"canonical_record":{"source":{"id":"1901.01792","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.NA","submitted_at":"2019-01-07T13:22:57Z","cross_cats_sorted":["cs.NA"],"title_canon_sha256":"9f2c6483b0ce1778271f3350a9c726a552151123fb16eeec4c5bb890bd82f6d9","abstract_canon_sha256":"a3e9a264fc603ad0c849d9aa082728304af439c8feeeaa6560e372d81d678f33"},"schema_version":"1.0"},"canonical_sha256":"461b721e5376a61a57dbf61344aaf5ef31d18efa1446b251b15d9ad1b8c4bd48","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:42:08.448169Z","signature_b64":"mNN+JWqMiY0UhJjQVuHNmoEzRmFOxqN14wqx1A5NfZhK7NEVgvvDpl7URahhJps5QzmQtbiqPZ4BUgFa+t8wCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"461b721e5376a61a57dbf61344aaf5ef31d18efa1446b251b15d9ad1b8c4bd48","last_reissued_at":"2026-05-17T23:42:08.447517Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:42:08.447517Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1901.01792","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":"2026-05-17T23:42:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9IeWzhdb4pxv+wG6QAEr9s885fa4dNji3nqV3KVEded7qbA1NJaMaWDUkVGgUUQI5Uxa4eSxQet0kTi/IL2IBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T05:46:22.261096Z"},"content_sha256":"d9a9b56b6eafd78bf41cd9a9c354f2b504539ab20b27160412eef9d1b69f7722","schema_version":"1.0","event_id":"sha256:d9a9b56b6eafd78bf41cd9a9c354f2b504539ab20b27160412eef9d1b69f7722"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2019:IYNXEHSTO2TBUV636YJUJKXV54","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Finite element error analysis of wave equations with dynamic boundary conditions: $L^2$ estimates","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cs.NA"],"primary_cat":"math.NA","authors_text":"Bal\\'azs Kov\\'acs, David Hipp","submitted_at":"2019-01-07T13:22:57Z","abstract_excerpt":"$L^2$ norm error estimates of semi- and full discretisations, using bulk--surface finite elements and Runge--Kutta methods, of wave equations with dynamic boundary conditions are studied. The analysis resides on an abstract formulation and error estimates, via energy techniques, within this abstract setting. Four prototypical linear wave equations with dynamic boundary conditions are analysed which fit into the abstract framework. For problems with velocity terms, or with acoustic boundary conditions we prove surprising results: for such problems the spatial convergence order is shown to be le"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1901.01792","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":"2026-05-17T23:42:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Hx6ik2VAVQwjvePwU3oN+IEpsYIka/fLVAoqgZw+TOOMp4JNP48/5tSQq/FstNd3A4YgGsBe+SGgluNh8tRhCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T05:46:22.261848Z"},"content_sha256":"32d3673b22b14c87aa9c7988ed088a9165e5076ce8317d14c8c9a2afbe208fe9","schema_version":"1.0","event_id":"sha256:32d3673b22b14c87aa9c7988ed088a9165e5076ce8317d14c8c9a2afbe208fe9"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/IYNXEHSTO2TBUV636YJUJKXV54/bundle.json","state_url":"https://pith.science/pith/IYNXEHSTO2TBUV636YJUJKXV54/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/IYNXEHSTO2TBUV636YJUJKXV54/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":"2026-06-05T05:46:22Z","links":{"resolver":"https://pith.science/pith/IYNXEHSTO2TBUV636YJUJKXV54","bundle":"https://pith.science/pith/IYNXEHSTO2TBUV636YJUJKXV54/bundle.json","state":"https://pith.science/pith/IYNXEHSTO2TBUV636YJUJKXV54/state.json","well_known_bundle":"https://pith.science/.well-known/pith/IYNXEHSTO2TBUV636YJUJKXV54/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:IYNXEHSTO2TBUV636YJUJKXV54","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":"a3e9a264fc603ad0c849d9aa082728304af439c8feeeaa6560e372d81d678f33","cross_cats_sorted":["cs.NA"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.NA","submitted_at":"2019-01-07T13:22:57Z","title_canon_sha256":"9f2c6483b0ce1778271f3350a9c726a552151123fb16eeec4c5bb890bd82f6d9"},"schema_version":"1.0","source":{"id":"1901.01792","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1901.01792","created_at":"2026-05-17T23:42:08Z"},{"alias_kind":"arxiv_version","alias_value":"1901.01792v2","created_at":"2026-05-17T23:42:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1901.01792","created_at":"2026-05-17T23:42:08Z"},{"alias_kind":"pith_short_12","alias_value":"IYNXEHSTO2TB","created_at":"2026-05-18T12:33:18Z"},{"alias_kind":"pith_short_16","alias_value":"IYNXEHSTO2TBUV63","created_at":"2026-05-18T12:33:18Z"},{"alias_kind":"pith_short_8","alias_value":"IYNXEHST","created_at":"2026-05-18T12:33:18Z"}],"graph_snapshots":[{"event_id":"sha256:32d3673b22b14c87aa9c7988ed088a9165e5076ce8317d14c8c9a2afbe208fe9","target":"graph","created_at":"2026-05-17T23:42:08Z","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":"$L^2$ norm error estimates of semi- and full discretisations, using bulk--surface finite elements and Runge--Kutta methods, of wave equations with dynamic boundary conditions are studied. The analysis resides on an abstract formulation and error estimates, via energy techniques, within this abstract setting. Four prototypical linear wave equations with dynamic boundary conditions are analysed which fit into the abstract framework. For problems with velocity terms, or with acoustic boundary conditions we prove surprising results: for such problems the spatial convergence order is shown to be le","authors_text":"Bal\\'azs Kov\\'acs, David Hipp","cross_cats":["cs.NA"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.NA","submitted_at":"2019-01-07T13:22:57Z","title":"Finite element error analysis of wave equations with dynamic boundary conditions: $L^2$ estimates"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1901.01792","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:d9a9b56b6eafd78bf41cd9a9c354f2b504539ab20b27160412eef9d1b69f7722","target":"record","created_at":"2026-05-17T23:42:08Z","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":"a3e9a264fc603ad0c849d9aa082728304af439c8feeeaa6560e372d81d678f33","cross_cats_sorted":["cs.NA"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.NA","submitted_at":"2019-01-07T13:22:57Z","title_canon_sha256":"9f2c6483b0ce1778271f3350a9c726a552151123fb16eeec4c5bb890bd82f6d9"},"schema_version":"1.0","source":{"id":"1901.01792","kind":"arxiv","version":2}},"canonical_sha256":"461b721e5376a61a57dbf61344aaf5ef31d18efa1446b251b15d9ad1b8c4bd48","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"461b721e5376a61a57dbf61344aaf5ef31d18efa1446b251b15d9ad1b8c4bd48","first_computed_at":"2026-05-17T23:42:08.447517Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:42:08.447517Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"mNN+JWqMiY0UhJjQVuHNmoEzRmFOxqN14wqx1A5NfZhK7NEVgvvDpl7URahhJps5QzmQtbiqPZ4BUgFa+t8wCQ==","signature_status":"signed_v1","signed_at":"2026-05-17T23:42:08.448169Z","signed_message":"canonical_sha256_bytes"},"source_id":"1901.01792","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d9a9b56b6eafd78bf41cd9a9c354f2b504539ab20b27160412eef9d1b69f7722","sha256:32d3673b22b14c87aa9c7988ed088a9165e5076ce8317d14c8c9a2afbe208fe9"],"state_sha256":"cd1d2a4b76e755d54d71813d85f9c1c8ec1c08254e29667a869c9cc6555aa71a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Y5BuqNW3g2pmFygbR+x0IofK7i8AlPbfqXEZxi85ClaboQPUS5wgqdTDWdXlDYb0WJLj0mjX/8l+MBFuGjriBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-05T05:46:22.265580Z","bundle_sha256":"6b7db94ca4a8ec86759ac87dfe1d3ccae461921769b93de1af47a358dde33814"}}