{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:5LITN6UTDFIEQNTAY3SNLOIK7O","short_pith_number":"pith:5LITN6UT","canonical_record":{"source":{"id":"2605.15840","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2026-05-15T10:54:44Z","cross_cats_sorted":["physics.atm-clus","physics.chem-ph"],"title_canon_sha256":"99567f34673dd689044053794f27ac1f411acfd819e5e6015ded74d396ab7b99","abstract_canon_sha256":"e0222b0061418bdd390e1b378823413e133388f0ab5c5c42e01246f6e18365e9"},"schema_version":"1.0"},"canonical_sha256":"ead136fa931950483660c6e4d5b90afb8f94fb5b5266c8dfe5d65968552bd77b","source":{"kind":"arxiv","id":"2605.15840","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.15840","created_at":"2026-05-20T00:01:21Z"},{"alias_kind":"arxiv_version","alias_value":"2605.15840v1","created_at":"2026-05-20T00:01:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.15840","created_at":"2026-05-20T00:01:21Z"},{"alias_kind":"pith_short_12","alias_value":"5LITN6UTDFIE","created_at":"2026-05-20T00:01:21Z"},{"alias_kind":"pith_short_16","alias_value":"5LITN6UTDFIEQNTA","created_at":"2026-05-20T00:01:21Z"},{"alias_kind":"pith_short_8","alias_value":"5LITN6UT","created_at":"2026-05-20T00:01:21Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:5LITN6UTDFIEQNTAY3SNLOIK7O","target":"record","payload":{"canonical_record":{"source":{"id":"2605.15840","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2026-05-15T10:54:44Z","cross_cats_sorted":["physics.atm-clus","physics.chem-ph"],"title_canon_sha256":"99567f34673dd689044053794f27ac1f411acfd819e5e6015ded74d396ab7b99","abstract_canon_sha256":"e0222b0061418bdd390e1b378823413e133388f0ab5c5c42e01246f6e18365e9"},"schema_version":"1.0"},"canonical_sha256":"ead136fa931950483660c6e4d5b90afb8f94fb5b5266c8dfe5d65968552bd77b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-20T00:01:21.171585Z","signature_b64":"Y2/bH0WlYebWt8aOziFRqd69RxMMgQVnU6k0XJtikuJg2OL2xvBX8NYDRtElq75sqXgnm6E2FBCG/ModIJwBDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ead136fa931950483660c6e4d5b90afb8f94fb5b5266c8dfe5d65968552bd77b","last_reissued_at":"2026-05-20T00:01:21.170820Z","signature_status":"signed_v1","first_computed_at":"2026-05-20T00:01:21.170820Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2605.15840","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":"2026-05-20T00:01:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"k0qUFxJy3kIxlGeQe2zPEXzgjm8c/Q3Nxe/LE+u4OjrKLafTlODEeqYGmvSNJ+T1kqCLBk3jMxF7ro9YO6LWCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T16:53:05.291176Z"},"content_sha256":"ee44691db1be83f63e29d49b5fe95da66d35e53e0ac902ecf42fb51414bb63fa","schema_version":"1.0","event_id":"sha256:ee44691db1be83f63e29d49b5fe95da66d35e53e0ac902ecf42fb51414bb63fa"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:5LITN6UTDFIEQNTAY3SNLOIK7O","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Fluorescence and Relaxation Dynamics of Cesium in Argon Matrices: Multiple Trapping Sites and Host-Guest Interactions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"Cesium atoms in argon matrices occupy two main trapping sites that produce distinct fluorescence and relaxation dynamics for their excited states.","cross_cats":["physics.atm-clus","physics.chem-ph"],"primary_cat":"physics.atom-ph","authors_text":"B. Gervais, C. Crepin, D. Comparat, H. Dinesan, J. Douady, L. Dontot, S. Lahs, S. Mahapatra, W. Chin","submitted_at":"2026-05-15T10:54:44Z","abstract_excerpt":"We investigate the fluorescence and relaxation dynamics of Cs atoms embedded in a cryogenic argon matrix using spectroscopy measurements combined with diatomic-in-molecule (DIM) simulations. The data reveal complex emission spectra, large Stokes shifts, and slow relaxation effects, indicating strong host-guest interactions and substantial lattice reorganization. Although the spectra are superimposed on a broad background, possibly due to low-symmetry, defect-related, or grain-boundary trapping sites, the main spectral structure is consistent with two dominant trapping environments that give ri"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"The main spectral structure is consistent with two dominant trapping environments that give rise to two triplet absorption features with distinct fluorescence behavior of the doublet and singlet components.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"That the observed main spectral features arise specifically from two dominant trapping sites rather than a continuum of sites or other effects, and that the DIM simulations correctly capture the host-guest interactions and lattice reorganization without significant model error.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"Spectroscopy and DIM simulations of Cs in Ar matrices indicate two dominant trapping sites with large Stokes shifts, slow relaxation, and distinct doublet/singlet fluorescence behaviors.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"Cesium atoms in argon matrices occupy two main trapping sites that produce distinct fluorescence and relaxation dynamics for their excited states.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"a9eadccb7e91bec1b37b0d626b1789ad60dca26dd313ecb7ddec66a766c8827c"},"source":{"id":"2605.15840","kind":"arxiv","version":1},"verdict":{"id":"987020ad-ac0a-42d9-8cf8-e885a104f105","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-19T18:30:15.862634Z","strongest_claim":"The main spectral structure is consistent with two dominant trapping environments that give rise to two triplet absorption features with distinct fluorescence behavior of the doublet and singlet components.","one_line_summary":"Spectroscopy and DIM simulations of Cs in Ar matrices indicate two dominant trapping sites with large Stokes shifts, slow relaxation, and distinct doublet/singlet fluorescence behaviors.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"That the observed main spectral features arise specifically from two dominant trapping sites rather than a continuum of sites or other effects, and that the DIM simulations correctly capture the host-guest interactions and lattice reorganization without significant model error.","pith_extraction_headline":"Cesium atoms in argon matrices occupy two main trapping sites that produce distinct fluorescence and relaxation dynamics for their excited states."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2605.15840/integrity.json","findings":[],"available":true,"detectors_run":[{"name":"doi_title_agreement","ran_at":"2026-05-19T19:01:19.003412Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"doi_compliance","ran_at":"2026-05-19T18:41:13.892693Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"ai_meta_artifact","ran_at":"2026-05-19T17:33:48.714270Z","status":"skipped","version":"1.0.0","findings_count":0},{"name":"claim_evidence","ran_at":"2026-05-19T17:21:55.844810Z","status":"completed","version":"1.0.0","findings_count":0}],"snapshot_sha256":"91077b41610021326a1242d4f6697cda0357da7505132675914d872b247c6fd2"},"references":{"count":35,"sample":[{"doi":"","year":null,"title":"Furthermore, as mentioned before, we exper- imentally observe a large background in the absorption spectrum that could indicate a crystal with numerous defects","work_id":"bd791d7e-0f72-47e9-b34e-c99de1bde6e9","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":null,"title":"As for the crystalline sites, the spectrum results from the complex superposition of all the spectra associated to each individual site, but we can no longer associate a series of 2 or 3 peaks to a sp","work_id":"56f94d35-d923-410a-bb82-f608cf565d58","ref_index":2,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":1981,"title":"A. Barnes, W. Orville-Thomas, A. M¨ uller, and R. Gaufr` es,Matrix isolation spectroscopy(Springer Dor- drecht, 1981)","work_id":"3e87f2d8-3542-4bf9-a59c-d64d4ceeaadf","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":1989,"title":"M. Almond and A. Downs,Spectroscopy of Matrix Iso- lated Species(Wiley, Chichester, 1989)","work_id":"57f0876f-cf43-40f1-9acb-f3e7d8530f6a","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":1996,"title":"V. E. Bondybey, A. M. Smith, and J. Agreiter, Chemical reviews96, 2113 (1996)","work_id":"62139a46-0613-4149-98b7-a624a5c56484","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":35,"snapshot_sha256":"90da9bbc25ba61366e82ed9864e27466d04f8900844a11a6c583c9a7c141c2b8","internal_anchors":0},"formal_canon":{"evidence_count":2,"snapshot_sha256":"98743d3430d715f891611426b2828a5ad671d746441879d9687516773db0934a"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":"987020ad-ac0a-42d9-8cf8-e885a104f105"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-20T00:01:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yDmUGGfgCDXYCoXPylL6UzD02B9juD+tWBWMQISdghfjNJaumfQMPRk4ryPRz4eQAI4YC4WpjvEn3liHmz2wBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T16:53:05.292513Z"},"content_sha256":"f4b4ce68648b0d7a038d560cbeedf2a6d2cf891c8e64d24fd2287328566c5d9f","schema_version":"1.0","event_id":"sha256:f4b4ce68648b0d7a038d560cbeedf2a6d2cf891c8e64d24fd2287328566c5d9f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5LITN6UTDFIEQNTAY3SNLOIK7O/bundle.json","state_url":"https://pith.science/pith/5LITN6UTDFIEQNTAY3SNLOIK7O/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5LITN6UTDFIEQNTAY3SNLOIK7O/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":"2026-05-27T16:53:05Z","links":{"resolver":"https://pith.science/pith/5LITN6UTDFIEQNTAY3SNLOIK7O","bundle":"https://pith.science/pith/5LITN6UTDFIEQNTAY3SNLOIK7O/bundle.json","state":"https://pith.science/pith/5LITN6UTDFIEQNTAY3SNLOIK7O/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5LITN6UTDFIEQNTAY3SNLOIK7O/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:5LITN6UTDFIEQNTAY3SNLOIK7O","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":"e0222b0061418bdd390e1b378823413e133388f0ab5c5c42e01246f6e18365e9","cross_cats_sorted":["physics.atm-clus","physics.chem-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2026-05-15T10:54:44Z","title_canon_sha256":"99567f34673dd689044053794f27ac1f411acfd819e5e6015ded74d396ab7b99"},"schema_version":"1.0","source":{"id":"2605.15840","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.15840","created_at":"2026-05-20T00:01:21Z"},{"alias_kind":"arxiv_version","alias_value":"2605.15840v1","created_at":"2026-05-20T00:01:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.15840","created_at":"2026-05-20T00:01:21Z"},{"alias_kind":"pith_short_12","alias_value":"5LITN6UTDFIE","created_at":"2026-05-20T00:01:21Z"},{"alias_kind":"pith_short_16","alias_value":"5LITN6UTDFIEQNTA","created_at":"2026-05-20T00:01:21Z"},{"alias_kind":"pith_short_8","alias_value":"5LITN6UT","created_at":"2026-05-20T00:01:21Z"}],"graph_snapshots":[{"event_id":"sha256:f4b4ce68648b0d7a038d560cbeedf2a6d2cf891c8e64d24fd2287328566c5d9f","target":"graph","created_at":"2026-05-20T00:01:21Z","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":4,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","text":"The main spectral structure is consistent with two dominant trapping environments that give rise to two triplet absorption features with distinct fluorescence behavior of the doublet and singlet components."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"That the observed main spectral features arise specifically from two dominant trapping sites rather than a continuum of sites or other effects, and that the DIM simulations correctly capture the host-guest interactions and lattice reorganization without significant model error."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"Spectroscopy and DIM simulations of Cs in Ar matrices indicate two dominant trapping sites with large Stokes shifts, slow relaxation, and distinct doublet/singlet fluorescence behaviors."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"Cesium atoms in argon matrices occupy two main trapping sites that produce distinct fluorescence and relaxation dynamics for their excited states."}],"snapshot_sha256":"a9eadccb7e91bec1b37b0d626b1789ad60dca26dd313ecb7ddec66a766c8827c"},"formal_canon":{"evidence_count":2,"snapshot_sha256":"98743d3430d715f891611426b2828a5ad671d746441879d9687516773db0934a"},"integrity":{"available":true,"clean":true,"detectors_run":[{"findings_count":0,"name":"doi_title_agreement","ran_at":"2026-05-19T19:01:19.003412Z","status":"completed","version":"1.0.0"},{"findings_count":0,"name":"doi_compliance","ran_at":"2026-05-19T18:41:13.892693Z","status":"completed","version":"1.0.0"},{"findings_count":0,"name":"ai_meta_artifact","ran_at":"2026-05-19T17:33:48.714270Z","status":"skipped","version":"1.0.0"},{"findings_count":0,"name":"claim_evidence","ran_at":"2026-05-19T17:21:55.844810Z","status":"completed","version":"1.0.0"}],"endpoint":"/pith/2605.15840/integrity.json","findings":[],"snapshot_sha256":"91077b41610021326a1242d4f6697cda0357da7505132675914d872b247c6fd2","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We investigate the fluorescence and relaxation dynamics of Cs atoms embedded in a cryogenic argon matrix using spectroscopy measurements combined with diatomic-in-molecule (DIM) simulations. The data reveal complex emission spectra, large Stokes shifts, and slow relaxation effects, indicating strong host-guest interactions and substantial lattice reorganization. Although the spectra are superimposed on a broad background, possibly due to low-symmetry, defect-related, or grain-boundary trapping sites, the main spectral structure is consistent with two dominant trapping environments that give ri","authors_text":"B. Gervais, C. Crepin, D. Comparat, H. Dinesan, J. Douady, L. Dontot, S. Lahs, S. Mahapatra, W. Chin","cross_cats":["physics.atm-clus","physics.chem-ph"],"headline":"Cesium atoms in argon matrices occupy two main trapping sites that produce distinct fluorescence and relaxation dynamics for their excited states.","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2026-05-15T10:54:44Z","title":"Fluorescence and Relaxation Dynamics of Cesium in Argon Matrices: Multiple Trapping Sites and Host-Guest Interactions"},"references":{"count":35,"internal_anchors":0,"resolved_work":35,"sample":[{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":1,"title":"Furthermore, as mentioned before, we exper- imentally observe a large background in the absorption spectrum that could indicate a crystal with numerous defects","work_id":"bd791d7e-0f72-47e9-b34e-c99de1bde6e9","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":2,"title":"As for the crystalline sites, the spectrum results from the complex superposition of all the spectra associated to each individual site, but we can no longer associate a series of 2 or 3 peaks to a sp","work_id":"56f94d35-d923-410a-bb82-f608cf565d58","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":3,"title":"A. Barnes, W. Orville-Thomas, A. M¨ uller, and R. Gaufr` es,Matrix isolation spectroscopy(Springer Dor- drecht, 1981)","work_id":"3e87f2d8-3542-4bf9-a59c-d64d4ceeaadf","year":1981},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":4,"title":"M. Almond and A. Downs,Spectroscopy of Matrix Iso- lated Species(Wiley, Chichester, 1989)","work_id":"57f0876f-cf43-40f1-9acb-f3e7d8530f6a","year":1989},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":5,"title":"V. E. Bondybey, A. M. Smith, and J. Agreiter, Chemical reviews96, 2113 (1996)","work_id":"62139a46-0613-4149-98b7-a624a5c56484","year":1996}],"snapshot_sha256":"90da9bbc25ba61366e82ed9864e27466d04f8900844a11a6c583c9a7c141c2b8"},"source":{"id":"2605.15840","kind":"arxiv","version":1},"verdict":{"created_at":"2026-05-19T18:30:15.862634Z","id":"987020ad-ac0a-42d9-8cf8-e885a104f105","model_set":{"reader":"grok-4.3"},"one_line_summary":"Spectroscopy and DIM simulations of Cs in Ar matrices indicate two dominant trapping sites with large Stokes shifts, slow relaxation, and distinct doublet/singlet fluorescence behaviors.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"Cesium atoms in argon matrices occupy two main trapping sites that produce distinct fluorescence and relaxation dynamics for their excited states.","strongest_claim":"The main spectral structure is consistent with two dominant trapping environments that give rise to two triplet absorption features with distinct fluorescence behavior of the doublet and singlet components.","weakest_assumption":"That the observed main spectral features arise specifically from two dominant trapping sites rather than a continuum of sites or other effects, and that the DIM simulations correctly capture the host-guest interactions and lattice reorganization without significant model error."}},"verdict_id":"987020ad-ac0a-42d9-8cf8-e885a104f105"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:ee44691db1be83f63e29d49b5fe95da66d35e53e0ac902ecf42fb51414bb63fa","target":"record","created_at":"2026-05-20T00:01:21Z","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":"e0222b0061418bdd390e1b378823413e133388f0ab5c5c42e01246f6e18365e9","cross_cats_sorted":["physics.atm-clus","physics.chem-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2026-05-15T10:54:44Z","title_canon_sha256":"99567f34673dd689044053794f27ac1f411acfd819e5e6015ded74d396ab7b99"},"schema_version":"1.0","source":{"id":"2605.15840","kind":"arxiv","version":1}},"canonical_sha256":"ead136fa931950483660c6e4d5b90afb8f94fb5b5266c8dfe5d65968552bd77b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ead136fa931950483660c6e4d5b90afb8f94fb5b5266c8dfe5d65968552bd77b","first_computed_at":"2026-05-20T00:01:21.170820Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-20T00:01:21.170820Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Y2/bH0WlYebWt8aOziFRqd69RxMMgQVnU6k0XJtikuJg2OL2xvBX8NYDRtElq75sqXgnm6E2FBCG/ModIJwBDA==","signature_status":"signed_v1","signed_at":"2026-05-20T00:01:21.171585Z","signed_message":"canonical_sha256_bytes"},"source_id":"2605.15840","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ee44691db1be83f63e29d49b5fe95da66d35e53e0ac902ecf42fb51414bb63fa","sha256:f4b4ce68648b0d7a038d560cbeedf2a6d2cf891c8e64d24fd2287328566c5d9f"],"state_sha256":"1ac16ba6779d0222fe026b7b5c5fdaef703285928dd7bf7700a4957e24bd149c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ICaOADgH/WJO9iQkd3Wmv+a4nBYxD3daAyT+9OFn5Y51qQWhgkfq5dIkN0gxXxujvjPVjKcdCifpZGPNVJ0IAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T16:53:05.298418Z","bundle_sha256":"d403b8109e2510337b0ea8a45f3af1a2cd4dca1b6925c77679085d2b55baa2be"}}