{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2000:6D5APC7V44BJQ65NXE2FRKY5RA","short_pith_number":"pith:6D5APC7V","canonical_record":{"source":{"id":"physics/0009031","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"physics.acc-ph","submitted_at":"2000-09-08T21:16:56Z","cross_cats_sorted":[],"title_canon_sha256":"c6d293d087589d52a6c443a7032321182ebb5cc855e33d5dc710158d30a1844d","abstract_canon_sha256":"c2b47ce4a0e4af81aeab2e9e5af662f0a59db2761add84a1056083b38eb39e7d"},"schema_version":"1.0"},"canonical_sha256":"f0fa078bf5e702987badb93458ab1d881529a295d467f6fa12555dea95a069b2","source":{"kind":"arxiv","id":"physics/0009031","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"physics/0009031","created_at":"2026-07-04T14:43:21Z"},{"alias_kind":"arxiv_version","alias_value":"physics/0009031v1","created_at":"2026-07-04T14:43:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.physics/0009031","created_at":"2026-07-04T14:43:21Z"},{"alias_kind":"pith_short_12","alias_value":"6D5APC7V44BJ","created_at":"2026-07-04T14:43:21Z"},{"alias_kind":"pith_short_16","alias_value":"6D5APC7V44BJQ65N","created_at":"2026-07-04T14:43:21Z"},{"alias_kind":"pith_short_8","alias_value":"6D5APC7V","created_at":"2026-07-04T14:43:21Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2000:6D5APC7V44BJQ65NXE2FRKY5RA","target":"record","payload":{"canonical_record":{"source":{"id":"physics/0009031","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"physics.acc-ph","submitted_at":"2000-09-08T21:16:56Z","cross_cats_sorted":[],"title_canon_sha256":"c6d293d087589d52a6c443a7032321182ebb5cc855e33d5dc710158d30a1844d","abstract_canon_sha256":"c2b47ce4a0e4af81aeab2e9e5af662f0a59db2761add84a1056083b38eb39e7d"},"schema_version":"1.0"},"canonical_sha256":"f0fa078bf5e702987badb93458ab1d881529a295d467f6fa12555dea95a069b2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:43:21.166072Z","signature_b64":"f0m1z0jJzuUxohTuxPc9VOefeaPutOMmTn0MKKKWMc+UGFNEO7dG9POuM2PTusm439Wkh5ZzUFgo6rbfIBO0CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f0fa078bf5e702987badb93458ab1d881529a295d467f6fa12555dea95a069b2","last_reissued_at":"2026-07-04T14:43:21.165655Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:43:21.165655Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"physics/0009031","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T14:43:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"B1sfci9J8f9iGNe5OxnCvV0fpQoJPXgysHl88lzRRgb64Tu+ekX0io4Lt8nMOQd46mIWJFJzxSXTK2Ik1BoYAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-07T09:30:14.175385Z"},"content_sha256":"dd751a6af7ce851f6da202e9059ecc8a1b4bbae30f1f7908414ad3ecf1fbcd2d","schema_version":"1.0","event_id":"sha256:dd751a6af7ce851f6da202e9059ecc8a1b4bbae30f1f7908414ad3ecf1fbcd2d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2000:6D5APC7V44BJQ65NXE2FRKY5RA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Design of the JLC/NLC RDDS Structure Using Parallel Eigensolver Omega3p","license":"","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"B. McCandless, E.W. Lundahl, J.W. Wang (SLAC), K. Ko, M.D. Starkey, N.T. Folwell, R.D. Ruth, R.H. Miller, R.J. Loewen, T. Higo (KEK), Y. Sun, Z. Li","submitted_at":"2000-09-08T21:16:56Z","abstract_excerpt":"The complexity of the Round Damped Detuned Structue (RDDS) for the JLC/NLC main linac is driven by the considerations of rf efficiency and dipole wakefield suppression. As a time and cost saving measure for the JLC/NLC, the dimensions of the 3D RDDS cell are being determined through computer modeling to within fabrication precision so that no tuning may be needed once the structures are assembled. The tolerances on the frequency errors for the RDDS structure are about one MHz for the fundamental mode and a few MHz for the dipole modes. At the X-band frequency, these correspond to errors of a m"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"physics/0009031","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/physics/0009031/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T14:43:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PStklt0SBkSrFk1aqakR35H4ngKdEoRKxR3n9ntadifybm0RPLP2biWMzSKlYA3ddpNpmIoO/vAbcL3GAe5pCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-07T09:30:14.176317Z"},"content_sha256":"a4e77fd3d29d19159bfafbd8dc4637e582b97b0fa1066bc56fb0efead581aa0f","schema_version":"1.0","event_id":"sha256:a4e77fd3d29d19159bfafbd8dc4637e582b97b0fa1066bc56fb0efead581aa0f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6D5APC7V44BJQ65NXE2FRKY5RA/bundle.json","state_url":"https://pith.science/pith/6D5APC7V44BJQ65NXE2FRKY5RA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6D5APC7V44BJQ65NXE2FRKY5RA/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":"2026-08-07T09:30:14Z","links":{"resolver":"https://pith.science/pith/6D5APC7V44BJQ65NXE2FRKY5RA","bundle":"https://pith.science/pith/6D5APC7V44BJQ65NXE2FRKY5RA/bundle.json","state":"https://pith.science/pith/6D5APC7V44BJQ65NXE2FRKY5RA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6D5APC7V44BJQ65NXE2FRKY5RA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2000:6D5APC7V44BJQ65NXE2FRKY5RA","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":"c2b47ce4a0e4af81aeab2e9e5af662f0a59db2761add84a1056083b38eb39e7d","cross_cats_sorted":[],"license":"","primary_cat":"physics.acc-ph","submitted_at":"2000-09-08T21:16:56Z","title_canon_sha256":"c6d293d087589d52a6c443a7032321182ebb5cc855e33d5dc710158d30a1844d"},"schema_version":"1.0","source":{"id":"physics/0009031","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"physics/0009031","created_at":"2026-07-04T14:43:21Z"},{"alias_kind":"arxiv_version","alias_value":"physics/0009031v1","created_at":"2026-07-04T14:43:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.physics/0009031","created_at":"2026-07-04T14:43:21Z"},{"alias_kind":"pith_short_12","alias_value":"6D5APC7V44BJ","created_at":"2026-07-04T14:43:21Z"},{"alias_kind":"pith_short_16","alias_value":"6D5APC7V44BJQ65N","created_at":"2026-07-04T14:43:21Z"},{"alias_kind":"pith_short_8","alias_value":"6D5APC7V","created_at":"2026-07-04T14:43:21Z"}],"graph_snapshots":[{"event_id":"sha256:a4e77fd3d29d19159bfafbd8dc4637e582b97b0fa1066bc56fb0efead581aa0f","target":"graph","created_at":"2026-07-04T14:43:21Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/physics/0009031/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The complexity of the Round Damped Detuned Structue (RDDS) for the JLC/NLC main linac is driven by the considerations of rf efficiency and dipole wakefield suppression. As a time and cost saving measure for the JLC/NLC, the dimensions of the 3D RDDS cell are being determined through computer modeling to within fabrication precision so that no tuning may be needed once the structures are assembled. The tolerances on the frequency errors for the RDDS structure are about one MHz for the fundamental mode and a few MHz for the dipole modes. At the X-band frequency, these correspond to errors of a m","authors_text":"B. McCandless, E.W. Lundahl, J.W. Wang (SLAC), K. Ko, M.D. Starkey, N.T. Folwell, R.D. Ruth, R.H. Miller, R.J. Loewen, T. Higo (KEK), Y. Sun, Z. Li","cross_cats":[],"headline":"","license":"","primary_cat":"physics.acc-ph","submitted_at":"2000-09-08T21:16:56Z","title":"Design of the JLC/NLC RDDS Structure Using Parallel Eigensolver Omega3p"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"physics/0009031","kind":"arxiv","version":1},"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:dd751a6af7ce851f6da202e9059ecc8a1b4bbae30f1f7908414ad3ecf1fbcd2d","target":"record","created_at":"2026-07-04T14:43:21Z","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":"c2b47ce4a0e4af81aeab2e9e5af662f0a59db2761add84a1056083b38eb39e7d","cross_cats_sorted":[],"license":"","primary_cat":"physics.acc-ph","submitted_at":"2000-09-08T21:16:56Z","title_canon_sha256":"c6d293d087589d52a6c443a7032321182ebb5cc855e33d5dc710158d30a1844d"},"schema_version":"1.0","source":{"id":"physics/0009031","kind":"arxiv","version":1}},"canonical_sha256":"f0fa078bf5e702987badb93458ab1d881529a295d467f6fa12555dea95a069b2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f0fa078bf5e702987badb93458ab1d881529a295d467f6fa12555dea95a069b2","first_computed_at":"2026-07-04T14:43:21.165655Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T14:43:21.165655Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"f0m1z0jJzuUxohTuxPc9VOefeaPutOMmTn0MKKKWMc+UGFNEO7dG9POuM2PTusm439Wkh5ZzUFgo6rbfIBO0CQ==","signature_status":"signed_v1","signed_at":"2026-07-04T14:43:21.166072Z","signed_message":"canonical_sha256_bytes"},"source_id":"physics/0009031","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:dd751a6af7ce851f6da202e9059ecc8a1b4bbae30f1f7908414ad3ecf1fbcd2d","sha256:a4e77fd3d29d19159bfafbd8dc4637e582b97b0fa1066bc56fb0efead581aa0f"],"state_sha256":"43b127f73570eedee5cda72169508df1ccfd7b7dd6288cf7248a6629e36eed62"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wv+DSlR5VlkQ8LNL0dW7LYqTn+dIHiV7CW2WZIGw2LthrQXjBSUlLf2MwiUs+DmG3ECPs3QbjN8xSAX6nL5rCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-07T09:30:14.182128Z","bundle_sha256":"f76c9879a5ee03a21779244d95b4156e1e0619b092c47917471c1ea983de090c"}}