{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:BVXOPG3FQDL7FRCMSVHQRZ5T5I","short_pith_number":"pith:BVXOPG3F","canonical_record":{"source":{"id":"2604.11160","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2026-04-13T08:24:40Z","cross_cats_sorted":[],"title_canon_sha256":"0bd3882f052418008b29249701d14bfd73a8df117eab24624682cb5c845df867","abstract_canon_sha256":"a0c6c7a1a9fe62aa54c6d5c046489dd461abab11a033a8380e8128081fa35973"},"schema_version":"1.0"},"canonical_sha256":"0d6ee79b6580d7f2c44c954f08e7b3ea294f092d8b78c466b6ba7909277fed86","source":{"kind":"arxiv","id":"2604.11160","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2604.11160","created_at":"2026-07-07T02:17:24Z"},{"alias_kind":"arxiv_version","alias_value":"2604.11160v1","created_at":"2026-07-07T02:17:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2604.11160","created_at":"2026-07-07T02:17:24Z"},{"alias_kind":"pith_short_12","alias_value":"BVXOPG3FQDL7","created_at":"2026-07-07T02:17:24Z"},{"alias_kind":"pith_short_16","alias_value":"BVXOPG3FQDL7FRCM","created_at":"2026-07-07T02:17:24Z"},{"alias_kind":"pith_short_8","alias_value":"BVXOPG3F","created_at":"2026-07-07T02:17:24Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:BVXOPG3FQDL7FRCMSVHQRZ5T5I","target":"record","payload":{"canonical_record":{"source":{"id":"2604.11160","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2026-04-13T08:24:40Z","cross_cats_sorted":[],"title_canon_sha256":"0bd3882f052418008b29249701d14bfd73a8df117eab24624682cb5c845df867","abstract_canon_sha256":"a0c6c7a1a9fe62aa54c6d5c046489dd461abab11a033a8380e8128081fa35973"},"schema_version":"1.0"},"canonical_sha256":"0d6ee79b6580d7f2c44c954f08e7b3ea294f092d8b78c466b6ba7909277fed86","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-07T02:17:24.283935Z","signature_b64":"aQ6CvWfPHkAtut+HcRvBdj6rwGFTtOEZY06VpnT4ca70KRWG3Otap16bOX1C4wbnqYUDbGUVnhpvtQ8eZSh6AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0d6ee79b6580d7f2c44c954f08e7b3ea294f092d8b78c466b6ba7909277fed86","last_reissued_at":"2026-07-07T02:17:24.283038Z","signature_status":"signed_v1","first_computed_at":"2026-07-07T02:17:24.283038Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2604.11160","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":"2026-07-07T02:17:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"T5Ns45ONwi6qGfKwigiu7VC7KbbjMfyqnvTwHzVbVDlEMbVqvlgfxvyTwkGL0ddf5vHDXfOKJFhC5/sx1kJnCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-07T09:46:01.495791Z"},"content_sha256":"beb71343dc9ea2e9ef9ecf7b7555a3aa4efb690f23449360a6df16a202225a29","schema_version":"1.0","event_id":"sha256:beb71343dc9ea2e9ef9ecf7b7555a3aa4efb690f23449360a6df16a202225a29"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:BVXOPG3FQDL7FRCMSVHQRZ5T5I","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Correcting the Energy-Dependent Asymmetry in Low-Energy $\\mu$SR","license":"http://creativecommons.org/licenses/by/4.0/","headline":"Updated reference measurements and beam simulations correct the energy-dependent asymmetry in low-energy μSR.","cross_cats":[],"primary_cat":"physics.ins-det","authors_text":"A. Suter, G. Janka, T. Prokscha, Z. Salman","submitted_at":"2026-04-13T08:24:40Z","abstract_excerpt":"Low-energy $\\mu$SR (LE-$\\mu$SR) enables depth-resolved studies of magnetic and electronic properties from the surface into the near-surface region, but the measured transverse-field asymmetry is not an intrinsic constant and depends on implantation energy and beamline conditions. Following an upgrade of the single-muon tagging system at the LEM beamline at PSI in 2023, updated asymmetry calibrations became necessary. Here, we present updated reference measurements that establish the energy-dependent maximum asymmetry using a silver reference and quantify spurious contributions from reflected m"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"Together, these updated calibrations and the simulation-based overlap correction provide a practical and up-to-date framework for LE-μSR data correction under current beam conditions and enable quantitative depth-resolved analysis of volume fractions.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"The musrSim/Geant4 simulations with the updated electrostatic field map accurately model real beam-sample overlap, and the SrTiO3 benchmark validates the correction factor for general samples and conditions.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"Updated reference measurements and a Geant4-derived sample-size correction factor provide a practical framework for correcting energy-dependent asymmetry in current LE-μSR conditions.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"Updated reference measurements and beam simulations correct the energy-dependent asymmetry in low-energy μSR.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"d40c9f7d0f59f87c564e229cec0d72e0203d4405d36c0e7c2f745a5e0d18f1f2"},"source":{"id":"2604.11160","kind":"arxiv","version":1},"verdict":{"id":"b5d3474b-4507-4cbf-9e9a-a74e2ba038d7","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-10T16:26:50.593822Z","strongest_claim":"Together, these updated calibrations and the simulation-based overlap correction provide a practical and up-to-date framework for LE-μSR data correction under current beam conditions and enable quantitative depth-resolved analysis of volume fractions.","one_line_summary":"Updated reference measurements and a Geant4-derived sample-size correction factor provide a practical framework for correcting energy-dependent asymmetry in current LE-μSR conditions.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"The musrSim/Geant4 simulations with the updated electrostatic field map accurately model real beam-sample overlap, and the SrTiO3 benchmark validates the correction factor for general samples and conditions.","pith_extraction_headline":"Updated reference measurements and beam simulations correct the energy-dependent asymmetry in low-energy μSR."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2604.11160/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":29,"sample":[{"doi":"","year":null,"title":"Silver is non-magnetic and exhibits only negligible muon-spin depolarization; therefore, devia- tions ofA Ag from a constant value directly reflect instrumental effects","work_id":"b59391a1-211e-4d38-bfa8-e3f9cf1a4967","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":null,"title":"Nickel is fer- romagnetic even at room temperature, and muons stopping in the Ni layer depolarize on timescales too fast to be resolved by the LEM spectrometer (within∼0.07µs) [20]","work_id":"2ece2866-89c9-4794-af1e-4a67808d9b19","ref_index":2,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"10.16907/901d6fda-db9a-4925-","year":null,"title":"5 summarizes the combined impact of the instrumental effects discussed in Sec","work_id":"f6d1268f-914e-44eb-b365-1e2b0749e0ea","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2008,"title":"T. Prokscha, E. Morenzoni, K. Deiters, F. Foroughi, D. George, R. Kobler, A. Suter, and V . Vrankovic, Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detec","work_id":"e6415dc6-fc5c-4991-af30-d42b6d9c847b","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2001,"title":"T. Prokscha, E. Morenzoni, C. David, A. Hofer, H. Glückler, and L. Scandella, Applied Surface Science172, 235 (2001)","work_id":"75d939b3-c178-4069-aae7-5de6ea47021c","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":29,"snapshot_sha256":"00b224d1243fe69dae5760d2986c1fb0eacbbbfd8ce33bdb08cf73d233301ee8","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":"b5d3474b-4507-4cbf-9e9a-a74e2ba038d7"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-07T02:17:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9HeE8uvAQ9rxbOYFcqsIkrZhjz2c0GbT93wFBW7mzeSFQ25X5DLoKYQWpXWrq3I3QNUeSYrFUm6cvkfKp9akAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-07T09:46:01.497008Z"},"content_sha256":"5f98dec71c276becbf5f88dd3be339ffe7444b1fc30eca6ff6556cb9bed7ea16","schema_version":"1.0","event_id":"sha256:5f98dec71c276becbf5f88dd3be339ffe7444b1fc30eca6ff6556cb9bed7ea16"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BVXOPG3FQDL7FRCMSVHQRZ5T5I/bundle.json","state_url":"https://pith.science/pith/BVXOPG3FQDL7FRCMSVHQRZ5T5I/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BVXOPG3FQDL7FRCMSVHQRZ5T5I/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":"2026-08-07T09:46:01Z","links":{"resolver":"https://pith.science/pith/BVXOPG3FQDL7FRCMSVHQRZ5T5I","bundle":"https://pith.science/pith/BVXOPG3FQDL7FRCMSVHQRZ5T5I/bundle.json","state":"https://pith.science/pith/BVXOPG3FQDL7FRCMSVHQRZ5T5I/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BVXOPG3FQDL7FRCMSVHQRZ5T5I/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:BVXOPG3FQDL7FRCMSVHQRZ5T5I","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":"a0c6c7a1a9fe62aa54c6d5c046489dd461abab11a033a8380e8128081fa35973","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2026-04-13T08:24:40Z","title_canon_sha256":"0bd3882f052418008b29249701d14bfd73a8df117eab24624682cb5c845df867"},"schema_version":"1.0","source":{"id":"2604.11160","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2604.11160","created_at":"2026-07-07T02:17:24Z"},{"alias_kind":"arxiv_version","alias_value":"2604.11160v1","created_at":"2026-07-07T02:17:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2604.11160","created_at":"2026-07-07T02:17:24Z"},{"alias_kind":"pith_short_12","alias_value":"BVXOPG3FQDL7","created_at":"2026-07-07T02:17:24Z"},{"alias_kind":"pith_short_16","alias_value":"BVXOPG3FQDL7FRCM","created_at":"2026-07-07T02:17:24Z"},{"alias_kind":"pith_short_8","alias_value":"BVXOPG3F","created_at":"2026-07-07T02:17:24Z"}],"graph_snapshots":[{"event_id":"sha256:5f98dec71c276becbf5f88dd3be339ffe7444b1fc30eca6ff6556cb9bed7ea16","target":"graph","created_at":"2026-07-07T02:17:24Z","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":4,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","text":"Together, these updated calibrations and the simulation-based overlap correction provide a practical and up-to-date framework for LE-μSR data correction under current beam conditions and enable quantitative depth-resolved analysis of volume fractions."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"The musrSim/Geant4 simulations with the updated electrostatic field map accurately model real beam-sample overlap, and the SrTiO3 benchmark validates the correction factor for general samples and conditions."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"Updated reference measurements and a Geant4-derived sample-size correction factor provide a practical framework for correcting energy-dependent asymmetry in current LE-μSR conditions."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"Updated reference measurements and beam simulations correct the energy-dependent asymmetry in low-energy μSR."}],"snapshot_sha256":"d40c9f7d0f59f87c564e229cec0d72e0203d4405d36c0e7c2f745a5e0d18f1f2"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2604.11160/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Low-energy $\\mu$SR (LE-$\\mu$SR) enables depth-resolved studies of magnetic and electronic properties from the surface into the near-surface region, but the measured transverse-field asymmetry is not an intrinsic constant and depends on implantation energy and beamline conditions. Following an upgrade of the single-muon tagging system at the LEM beamline at PSI in 2023, updated asymmetry calibrations became necessary. Here, we present updated reference measurements that establish the energy-dependent maximum asymmetry using a silver reference and quantify spurious contributions from reflected m","authors_text":"A. Suter, G. Janka, T. Prokscha, Z. Salman","cross_cats":[],"headline":"Updated reference measurements and beam simulations correct the energy-dependent asymmetry in low-energy μSR.","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2026-04-13T08:24:40Z","title":"Correcting the Energy-Dependent Asymmetry in Low-Energy $\\mu$SR"},"references":{"count":29,"internal_anchors":0,"resolved_work":29,"sample":[{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":1,"title":"Silver is non-magnetic and exhibits only negligible muon-spin depolarization; therefore, devia- tions ofA Ag from a constant value directly reflect instrumental effects","work_id":"b59391a1-211e-4d38-bfa8-e3f9cf1a4967","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":2,"title":"Nickel is fer- romagnetic even at room temperature, and muons stopping in the Ni layer depolarize on timescales too fast to be resolved by the LEM spectrometer (within∼0.07µs) [20]","work_id":"2ece2866-89c9-4794-af1e-4a67808d9b19","year":null},{"cited_arxiv_id":"","doi":"10.16907/901d6fda-db9a-4925-","is_internal_anchor":false,"ref_index":3,"title":"5 summarizes the combined impact of the instrumental effects discussed in Sec","work_id":"f6d1268f-914e-44eb-b365-1e2b0749e0ea","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":4,"title":"T. Prokscha, E. Morenzoni, K. Deiters, F. Foroughi, D. George, R. Kobler, A. Suter, and V . Vrankovic, Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detec","work_id":"e6415dc6-fc5c-4991-af30-d42b6d9c847b","year":2008},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":5,"title":"T. Prokscha, E. Morenzoni, C. David, A. Hofer, H. Glückler, and L. Scandella, Applied Surface Science172, 235 (2001)","work_id":"75d939b3-c178-4069-aae7-5de6ea47021c","year":2001}],"snapshot_sha256":"00b224d1243fe69dae5760d2986c1fb0eacbbbfd8ce33bdb08cf73d233301ee8"},"source":{"id":"2604.11160","kind":"arxiv","version":1},"verdict":{"created_at":"2026-05-10T16:26:50.593822Z","id":"b5d3474b-4507-4cbf-9e9a-a74e2ba038d7","model_set":{"reader":"grok-4.3"},"one_line_summary":"Updated reference measurements and a Geant4-derived sample-size correction factor provide a practical framework for correcting energy-dependent asymmetry in current LE-μSR conditions.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"Updated reference measurements and beam simulations correct the energy-dependent asymmetry in low-energy μSR.","strongest_claim":"Together, these updated calibrations and the simulation-based overlap correction provide a practical and up-to-date framework for LE-μSR data correction under current beam conditions and enable quantitative depth-resolved analysis of volume fractions.","weakest_assumption":"The musrSim/Geant4 simulations with the updated electrostatic field map accurately model real beam-sample overlap, and the SrTiO3 benchmark validates the correction factor for general samples and conditions."}},"verdict_id":"b5d3474b-4507-4cbf-9e9a-a74e2ba038d7"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:beb71343dc9ea2e9ef9ecf7b7555a3aa4efb690f23449360a6df16a202225a29","target":"record","created_at":"2026-07-07T02:17:24Z","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":"a0c6c7a1a9fe62aa54c6d5c046489dd461abab11a033a8380e8128081fa35973","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2026-04-13T08:24:40Z","title_canon_sha256":"0bd3882f052418008b29249701d14bfd73a8df117eab24624682cb5c845df867"},"schema_version":"1.0","source":{"id":"2604.11160","kind":"arxiv","version":1}},"canonical_sha256":"0d6ee79b6580d7f2c44c954f08e7b3ea294f092d8b78c466b6ba7909277fed86","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0d6ee79b6580d7f2c44c954f08e7b3ea294f092d8b78c466b6ba7909277fed86","first_computed_at":"2026-07-07T02:17:24.283038Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-07T02:17:24.283038Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"aQ6CvWfPHkAtut+HcRvBdj6rwGFTtOEZY06VpnT4ca70KRWG3Otap16bOX1C4wbnqYUDbGUVnhpvtQ8eZSh6AA==","signature_status":"signed_v1","signed_at":"2026-07-07T02:17:24.283935Z","signed_message":"canonical_sha256_bytes"},"source_id":"2604.11160","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:beb71343dc9ea2e9ef9ecf7b7555a3aa4efb690f23449360a6df16a202225a29","sha256:5f98dec71c276becbf5f88dd3be339ffe7444b1fc30eca6ff6556cb9bed7ea16"],"state_sha256":"2d92501e587ba6282d8da9d2f9aad3fd91a0719b1a95832001418497a09b2cd7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cuciM9+kamVnLDllEhuj7OsBjQ6FeKRLy4fO+rv9nSBqILYeel5DzH8wYEAmOvwWv1Q1KVwqu+NXm1WwhQuIDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-07T09:46:01.506957Z","bundle_sha256":"6f0cc848ee8032a40a9960933c98d8a41debbbb8606bebc6794ab1dc6371b166"}}