{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:LRAUTX6NJQ5HMYKENYRDA3XHZP","short_pith_number":"pith:LRAUTX6N","canonical_record":{"source":{"id":"1303.6514","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.acc-ph","submitted_at":"2013-03-26T14:46:59Z","cross_cats_sorted":[],"title_canon_sha256":"102d42a6c08ea088ece9fa66cf563b626b22d3276eb9d54050015e209c609fc8","abstract_canon_sha256":"cb788b5bfa043b7422a1897b2a7016feed0607a46ccd589dbdc77c6657ee4252"},"schema_version":"1.0"},"canonical_sha256":"5c4149dfcd4c3a7661446e22306ee7cbcef2d58ff54152a033752e9cbf0e5b97","source":{"kind":"arxiv","id":"1303.6514","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.6514","created_at":"2026-05-18T03:29:49Z"},{"alias_kind":"arxiv_version","alias_value":"1303.6514v1","created_at":"2026-05-18T03:29:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.6514","created_at":"2026-05-18T03:29:49Z"},{"alias_kind":"pith_short_12","alias_value":"LRAUTX6NJQ5H","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_16","alias_value":"LRAUTX6NJQ5HMYKE","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_8","alias_value":"LRAUTX6N","created_at":"2026-05-18T12:27:51Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:LRAUTX6NJQ5HMYKENYRDA3XHZP","target":"record","payload":{"canonical_record":{"source":{"id":"1303.6514","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.acc-ph","submitted_at":"2013-03-26T14:46:59Z","cross_cats_sorted":[],"title_canon_sha256":"102d42a6c08ea088ece9fa66cf563b626b22d3276eb9d54050015e209c609fc8","abstract_canon_sha256":"cb788b5bfa043b7422a1897b2a7016feed0607a46ccd589dbdc77c6657ee4252"},"schema_version":"1.0"},"canonical_sha256":"5c4149dfcd4c3a7661446e22306ee7cbcef2d58ff54152a033752e9cbf0e5b97","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:29:49.217192Z","signature_b64":"DkUnPnLpQzCEaDGn1nw6kFJlru+SZ25ntwBl2MEwjG7kEQbMtHZpoGwIZkBn9dA8pGTuV0VQ8jwR3Xko1RCCBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5c4149dfcd4c3a7661446e22306ee7cbcef2d58ff54152a033752e9cbf0e5b97","last_reissued_at":"2026-05-18T03:29:49.216381Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:29:49.216381Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1303.6514","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":"2026-05-18T03:29:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cZFlWe53sXHPp1o+ZXnLRFTKuawYOIHN/KMsqBzH6MtvEcht2ZiVmsFjxfoH+qkQoAC3PrtDgqtaV89xdpvcAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T08:22:39.808154Z"},"content_sha256":"e8d9936cf7ef0af9ab109f438bc2dac10acf4167778802407e8ce5b5312f56d0","schema_version":"1.0","event_id":"sha256:e8d9936cf7ef0af9ab109f438bc2dac10acf4167778802407e8ce5b5312f56d0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:LRAUTX6NJQ5HMYKENYRDA3XHZP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Beam optics and lattice design for particle accelerators","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":[],"primary_cat":"physics.acc-ph","authors_text":"Bernhard J. Holzer (CERN)","submitted_at":"2013-03-26T14:46:59Z","abstract_excerpt":"The goal of this manuscript is to give an introduction into the design of the magnet lattice and as a consequence into the transverse dynamics of the particles in a synchrotron or storage ring. Starting from the basic principles of how to design the geometry of the ring we will briefly review the transverse motion of the particles and apply this knowledge to study the layout and optimization of the principal elements, namely the lattice cells. The detailed arrangement of the accelerator magnets within the cells is explained and will be used to calculate well defined and predictable beam parame"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.6514","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:29:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NNPTIH0H+soxI3+lj1pqmgYbJX+wI7ajQKrgNcQ9oiKE02N2zdCahbgMkDMJyWiTPMFmQs2hPHvJvlNWBrCkAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-10T08:22:39.808902Z"},"content_sha256":"cdb278247c8a6cbb6f41ddc26e3fae2a735cd35e0bf5240063ce04e2711003f0","schema_version":"1.0","event_id":"sha256:cdb278247c8a6cbb6f41ddc26e3fae2a735cd35e0bf5240063ce04e2711003f0"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LRAUTX6NJQ5HMYKENYRDA3XHZP/bundle.json","state_url":"https://pith.science/pith/LRAUTX6NJQ5HMYKENYRDA3XHZP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LRAUTX6NJQ5HMYKENYRDA3XHZP/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":"2026-06-10T08:22:39Z","links":{"resolver":"https://pith.science/pith/LRAUTX6NJQ5HMYKENYRDA3XHZP","bundle":"https://pith.science/pith/LRAUTX6NJQ5HMYKENYRDA3XHZP/bundle.json","state":"https://pith.science/pith/LRAUTX6NJQ5HMYKENYRDA3XHZP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LRAUTX6NJQ5HMYKENYRDA3XHZP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:LRAUTX6NJQ5HMYKENYRDA3XHZP","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":"cb788b5bfa043b7422a1897b2a7016feed0607a46ccd589dbdc77c6657ee4252","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.acc-ph","submitted_at":"2013-03-26T14:46:59Z","title_canon_sha256":"102d42a6c08ea088ece9fa66cf563b626b22d3276eb9d54050015e209c609fc8"},"schema_version":"1.0","source":{"id":"1303.6514","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.6514","created_at":"2026-05-18T03:29:49Z"},{"alias_kind":"arxiv_version","alias_value":"1303.6514v1","created_at":"2026-05-18T03:29:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.6514","created_at":"2026-05-18T03:29:49Z"},{"alias_kind":"pith_short_12","alias_value":"LRAUTX6NJQ5H","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_16","alias_value":"LRAUTX6NJQ5HMYKE","created_at":"2026-05-18T12:27:51Z"},{"alias_kind":"pith_short_8","alias_value":"LRAUTX6N","created_at":"2026-05-18T12:27:51Z"}],"graph_snapshots":[{"event_id":"sha256:cdb278247c8a6cbb6f41ddc26e3fae2a735cd35e0bf5240063ce04e2711003f0","target":"graph","created_at":"2026-05-18T03:29:49Z","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":"The goal of this manuscript is to give an introduction into the design of the magnet lattice and as a consequence into the transverse dynamics of the particles in a synchrotron or storage ring. Starting from the basic principles of how to design the geometry of the ring we will briefly review the transverse motion of the particles and apply this knowledge to study the layout and optimization of the principal elements, namely the lattice cells. The detailed arrangement of the accelerator magnets within the cells is explained and will be used to calculate well defined and predictable beam parame","authors_text":"Bernhard J. Holzer (CERN)","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.acc-ph","submitted_at":"2013-03-26T14:46:59Z","title":"Beam optics and lattice design for particle accelerators"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.6514","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:e8d9936cf7ef0af9ab109f438bc2dac10acf4167778802407e8ce5b5312f56d0","target":"record","created_at":"2026-05-18T03:29:49Z","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":"cb788b5bfa043b7422a1897b2a7016feed0607a46ccd589dbdc77c6657ee4252","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"physics.acc-ph","submitted_at":"2013-03-26T14:46:59Z","title_canon_sha256":"102d42a6c08ea088ece9fa66cf563b626b22d3276eb9d54050015e209c609fc8"},"schema_version":"1.0","source":{"id":"1303.6514","kind":"arxiv","version":1}},"canonical_sha256":"5c4149dfcd4c3a7661446e22306ee7cbcef2d58ff54152a033752e9cbf0e5b97","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5c4149dfcd4c3a7661446e22306ee7cbcef2d58ff54152a033752e9cbf0e5b97","first_computed_at":"2026-05-18T03:29:49.216381Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:29:49.216381Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"DkUnPnLpQzCEaDGn1nw6kFJlru+SZ25ntwBl2MEwjG7kEQbMtHZpoGwIZkBn9dA8pGTuV0VQ8jwR3Xko1RCCBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:29:49.217192Z","signed_message":"canonical_sha256_bytes"},"source_id":"1303.6514","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e8d9936cf7ef0af9ab109f438bc2dac10acf4167778802407e8ce5b5312f56d0","sha256:cdb278247c8a6cbb6f41ddc26e3fae2a735cd35e0bf5240063ce04e2711003f0"],"state_sha256":"8803eeac5636cc4499ca03055e567c1fa43d07c52bc0ad919646afec28446443"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RiyxRRCZWZEmXfxMrnUg7N4LH9mpQhZ9jbuekhZ2DAGN3mXP5bjLyv/+x6u3mamqQL412PXEwaE9SMurmq6bAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-10T08:22:39.813731Z","bundle_sha256":"7ea823d04a8c01cfd2b8c40fdf47e31a35cf16a72e317215cfd9c014c450e83a"}}