{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2023:RP22GMZGYUX2UKGRUP4KQDYCOJ","short_pith_number":"pith:RP22GMZG","canonical_record":{"source":{"id":"2309.05080","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.acc-ph","submitted_at":"2023-09-10T16:59:41Z","cross_cats_sorted":["hep-ex","nucl-ex"],"title_canon_sha256":"b9cc2bc9c437956e26862b0354d59e6647751747f3a85a4edda9520286cfeb95","abstract_canon_sha256":"280d8cd4205626d2ed3f6fb6641f1da9db3991125555698f007589f99e6a6f94"},"schema_version":"1.0"},"canonical_sha256":"8bf5a33326c52faa28d1a3f8a80f027275e1d8aff0fda13e15dadaf799a65ee5","source":{"kind":"arxiv","id":"2309.05080","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2309.05080","created_at":"2026-07-05T06:51:29Z"},{"alias_kind":"arxiv_version","alias_value":"2309.05080v2","created_at":"2026-07-05T06:51:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2309.05080","created_at":"2026-07-05T06:51:29Z"},{"alias_kind":"pith_short_12","alias_value":"RP22GMZGYUX2","created_at":"2026-07-05T06:51:29Z"},{"alias_kind":"pith_short_16","alias_value":"RP22GMZGYUX2UKGR","created_at":"2026-07-05T06:51:29Z"},{"alias_kind":"pith_short_8","alias_value":"RP22GMZG","created_at":"2026-07-05T06:51:29Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2023:RP22GMZGYUX2UKGRUP4KQDYCOJ","target":"record","payload":{"canonical_record":{"source":{"id":"2309.05080","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.acc-ph","submitted_at":"2023-09-10T16:59:41Z","cross_cats_sorted":["hep-ex","nucl-ex"],"title_canon_sha256":"b9cc2bc9c437956e26862b0354d59e6647751747f3a85a4edda9520286cfeb95","abstract_canon_sha256":"280d8cd4205626d2ed3f6fb6641f1da9db3991125555698f007589f99e6a6f94"},"schema_version":"1.0"},"canonical_sha256":"8bf5a33326c52faa28d1a3f8a80f027275e1d8aff0fda13e15dadaf799a65ee5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:51:29.723812Z","signature_b64":"g0LWCb60bvCdpM6WdVwTtmMPzwpVLPhDIbbAHVN8sSkHh4CxIkpjV9Vk3z2pKrSGvbYZxqwleMzQlfTvvoAPDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8bf5a33326c52faa28d1a3f8a80f027275e1d8aff0fda13e15dadaf799a65ee5","last_reissued_at":"2026-07-05T06:51:29.723333Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:51:29.723333Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2309.05080","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":"2026-07-05T06:51:29Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sgqWYGEJiUMWE56ahjlbUb0FTAI5UC1F+65WjdYquAZWqXeRCPZgM+gpoinFQqHB9nCpmskjSYgnkdDjL0uIAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T08:21:21.413451Z"},"content_sha256":"05403e0c7ef7e8890e8ac1cb46d132f618510ca75f2f02466ce4b8cd31d99163","schema_version":"1.0","event_id":"sha256:05403e0c7ef7e8890e8ac1cb46d132f618510ca75f2f02466ce4b8cd31d99163"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2023:RP22GMZGYUX2UKGRUP4KQDYCOJ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Spin decoherence and off-resonance behavior of radiofrequency-driven spin rotations in storage rings","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex","nucl-ex"],"primary_cat":"physics.acc-ph","authors_text":"A. Aggarwal, A. Aksentev, A. Andres, A. Kacharava, A. Kononov, A. Lehrach, A. Magiera, A. Melnikov, A. Nass, A. Pesce, A. Saleev, A. Silenko, A. Wirzba, A. Wro\\'nska, B. Alberdi, B. Breitkreutz, B. Lorentz, C. B\\\"ohme, D. Grzonka, D. Mchedlishvili, D. Prasuhn, D. Shergelashvili, E.J. Stephenson, F. Abusaif, F. M\\\"uller, F. Rathmann, G. Ciullo, G. Macharashvili, G. Tagliente, H. Soltner, H. Str\\\"oher, I. Bekman, I. Keshelashvili, J. Hetzel, J. Pretz, J. Slim, K. Grigoryev, K. Laihem, L. Barion, M. Bey\\ss, M. Gaisser, M. Tabidze, M. Vitz, M. \\.Zurek, N. Canale, N. Lomidze, N.N. Nikolaev, N.-O. Fr\\\"ohlich, N. Shurkhno, O. Javakhishvili, P. Lenisa, P. W\\\"ustner, R. Gebel, S. Dymov, S. Karanth, S. Siddique, S. Stassen, T. Wagner, V. Hejny, V. Kamerdzhiev, V. Poncza, V. Shmakova, Y. Valdau","submitted_at":"2023-09-10T16:59:41Z","abstract_excerpt":"Radiofrequency-driven resonant spin rotators are routinely used as standard instruments in polarization experiments in particle and nuclear physics. Maintaining the continuous exact parametric spin-resonance condition of the equality of the spin rotator and the spin precession frequency during operation constitutes one of the challenges. We present a detailed analytic description of the impact of detuning the exact spin resonance on the vertical and the in-plane precessing components of the polarization. An important part of the formalism presented here is the consideration of experimentally r"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2309.05080","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2309.05080/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":"2026-07-05T06:51:29Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0QjqllyQUfsWUqvVW/1QgNPPlaW1g8sASzjiVqOcgsIg4WUy5VL/oHz28sPqYSfT4em/vY+OfElx6DTU5kCpBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T08:21:21.414448Z"},"content_sha256":"dc6a1078e2bfa10f27b34a1079435da837b8d935925a107d8bfaa10964a81f80","schema_version":"1.0","event_id":"sha256:dc6a1078e2bfa10f27b34a1079435da837b8d935925a107d8bfaa10964a81f80"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RP22GMZGYUX2UKGRUP4KQDYCOJ/bundle.json","state_url":"https://pith.science/pith/RP22GMZGYUX2UKGRUP4KQDYCOJ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RP22GMZGYUX2UKGRUP4KQDYCOJ/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":"2026-08-06T08:21:21Z","links":{"resolver":"https://pith.science/pith/RP22GMZGYUX2UKGRUP4KQDYCOJ","bundle":"https://pith.science/pith/RP22GMZGYUX2UKGRUP4KQDYCOJ/bundle.json","state":"https://pith.science/pith/RP22GMZGYUX2UKGRUP4KQDYCOJ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RP22GMZGYUX2UKGRUP4KQDYCOJ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:RP22GMZGYUX2UKGRUP4KQDYCOJ","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":"280d8cd4205626d2ed3f6fb6641f1da9db3991125555698f007589f99e6a6f94","cross_cats_sorted":["hep-ex","nucl-ex"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.acc-ph","submitted_at":"2023-09-10T16:59:41Z","title_canon_sha256":"b9cc2bc9c437956e26862b0354d59e6647751747f3a85a4edda9520286cfeb95"},"schema_version":"1.0","source":{"id":"2309.05080","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2309.05080","created_at":"2026-07-05T06:51:29Z"},{"alias_kind":"arxiv_version","alias_value":"2309.05080v2","created_at":"2026-07-05T06:51:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2309.05080","created_at":"2026-07-05T06:51:29Z"},{"alias_kind":"pith_short_12","alias_value":"RP22GMZGYUX2","created_at":"2026-07-05T06:51:29Z"},{"alias_kind":"pith_short_16","alias_value":"RP22GMZGYUX2UKGR","created_at":"2026-07-05T06:51:29Z"},{"alias_kind":"pith_short_8","alias_value":"RP22GMZG","created_at":"2026-07-05T06:51:29Z"}],"graph_snapshots":[{"event_id":"sha256:dc6a1078e2bfa10f27b34a1079435da837b8d935925a107d8bfaa10964a81f80","target":"graph","created_at":"2026-07-05T06:51:29Z","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/2309.05080/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Radiofrequency-driven resonant spin rotators are routinely used as standard instruments in polarization experiments in particle and nuclear physics. Maintaining the continuous exact parametric spin-resonance condition of the equality of the spin rotator and the spin precession frequency during operation constitutes one of the challenges. We present a detailed analytic description of the impact of detuning the exact spin resonance on the vertical and the in-plane precessing components of the polarization. An important part of the formalism presented here is the consideration of experimentally r","authors_text":"A. Aggarwal, A. Aksentev, A. Andres, A. Kacharava, A. Kononov, A. Lehrach, A. Magiera, A. Melnikov, A. Nass, A. Pesce, A. Saleev, A. Silenko, A. Wirzba, A. Wro\\'nska, B. Alberdi, B. Breitkreutz, B. Lorentz, C. B\\\"ohme, D. Grzonka, D. Mchedlishvili, D. Prasuhn, D. Shergelashvili, E.J. Stephenson, F. Abusaif, F. M\\\"uller, F. Rathmann, G. Ciullo, G. Macharashvili, G. Tagliente, H. Soltner, H. Str\\\"oher, I. Bekman, I. Keshelashvili, J. Hetzel, J. Pretz, J. Slim, K. Grigoryev, K. Laihem, L. Barion, M. Bey\\ss, M. Gaisser, M. Tabidze, M. Vitz, M. \\.Zurek, N. Canale, N. Lomidze, N.N. Nikolaev, N.-O. Fr\\\"ohlich, N. Shurkhno, O. Javakhishvili, P. Lenisa, P. W\\\"ustner, R. Gebel, S. Dymov, S. Karanth, S. Siddique, S. Stassen, T. Wagner, V. Hejny, V. Kamerdzhiev, V. Poncza, V. Shmakova, Y. Valdau","cross_cats":["hep-ex","nucl-ex"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.acc-ph","submitted_at":"2023-09-10T16:59:41Z","title":"Spin decoherence and off-resonance behavior of radiofrequency-driven spin rotations in storage rings"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2309.05080","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":"sha256:05403e0c7ef7e8890e8ac1cb46d132f618510ca75f2f02466ce4b8cd31d99163","target":"record","created_at":"2026-07-05T06:51:29Z","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":"280d8cd4205626d2ed3f6fb6641f1da9db3991125555698f007589f99e6a6f94","cross_cats_sorted":["hep-ex","nucl-ex"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.acc-ph","submitted_at":"2023-09-10T16:59:41Z","title_canon_sha256":"b9cc2bc9c437956e26862b0354d59e6647751747f3a85a4edda9520286cfeb95"},"schema_version":"1.0","source":{"id":"2309.05080","kind":"arxiv","version":2}},"canonical_sha256":"8bf5a33326c52faa28d1a3f8a80f027275e1d8aff0fda13e15dadaf799a65ee5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8bf5a33326c52faa28d1a3f8a80f027275e1d8aff0fda13e15dadaf799a65ee5","first_computed_at":"2026-07-05T06:51:29.723333Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:51:29.723333Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"g0LWCb60bvCdpM6WdVwTtmMPzwpVLPhDIbbAHVN8sSkHh4CxIkpjV9Vk3z2pKrSGvbYZxqwleMzQlfTvvoAPDg==","signature_status":"signed_v1","signed_at":"2026-07-05T06:51:29.723812Z","signed_message":"canonical_sha256_bytes"},"source_id":"2309.05080","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:05403e0c7ef7e8890e8ac1cb46d132f618510ca75f2f02466ce4b8cd31d99163","sha256:dc6a1078e2bfa10f27b34a1079435da837b8d935925a107d8bfaa10964a81f80"],"state_sha256":"f30cb01045a90df2a8f168d37a6a81f57b8284d697983650e5cd4996af7f8523"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ykV7o5Ux0o5i+nbyhTCOeY0+iC+wwgUFl8JjUsuS+9R7bxeFfMUg0IWM1TfC3Be/oCXnIoXFQzVAnCJmLY6cCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-06T08:21:21.430029Z","bundle_sha256":"020511bf787f9b20335338ca0a865465d8ee9703d700c0bda8c4df257a0c7d6a"}}