{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:FG5VQIUZA2MBFXSWJS4VPKIIC6","short_pith_number":"pith:FG5VQIUZ","canonical_record":{"source":{"id":"2512.24855","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-12-31T13:25:55Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"f29718910824a09b2237075107a2d0cf99544430658619b2f7c375b695623379","abstract_canon_sha256":"b0991b8d4f47aed2419f754ea88545f69d4418a3532ca227ae29ae74b7d8f5fc"},"schema_version":"1.0"},"canonical_sha256":"29bb582299069812de564cb957a9081792bcdc2b5b7d7913b49043fff0b1cfa6","source":{"kind":"arxiv","id":"2512.24855","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2512.24855","created_at":"2026-05-28T02:04:44Z"},{"alias_kind":"arxiv_version","alias_value":"2512.24855v2","created_at":"2026-05-28T02:04:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2512.24855","created_at":"2026-05-28T02:04:44Z"},{"alias_kind":"pith_short_12","alias_value":"FG5VQIUZA2MB","created_at":"2026-05-28T02:04:44Z"},{"alias_kind":"pith_short_16","alias_value":"FG5VQIUZA2MBFXSW","created_at":"2026-05-28T02:04:44Z"},{"alias_kind":"pith_short_8","alias_value":"FG5VQIUZ","created_at":"2026-05-28T02:04:44Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:FG5VQIUZA2MBFXSWJS4VPKIIC6","target":"record","payload":{"canonical_record":{"source":{"id":"2512.24855","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-12-31T13:25:55Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"f29718910824a09b2237075107a2d0cf99544430658619b2f7c375b695623379","abstract_canon_sha256":"b0991b8d4f47aed2419f754ea88545f69d4418a3532ca227ae29ae74b7d8f5fc"},"schema_version":"1.0"},"canonical_sha256":"29bb582299069812de564cb957a9081792bcdc2b5b7d7913b49043fff0b1cfa6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-28T02:04:44.982865Z","signature_b64":"p6M9tavgdKQGjwLQDTvjQf8J2rN75XAJWfBsIlkDU0mAGBbhc0kxUNvI3CGBt3t5a3FEywBlWfE24651bQtlCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"29bb582299069812de564cb957a9081792bcdc2b5b7d7913b49043fff0b1cfa6","last_reissued_at":"2026-05-28T02:04:44.982255Z","signature_status":"signed_v1","first_computed_at":"2026-05-28T02:04:44.982255Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2512.24855","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":"2026-05-28T02:04:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"D2olwuM8TA/SMlusQQ15oTkifd6n87n5zFo22zwWTupNXleuLUt5MLExxtaR32hCAXEfJj/dfh2leb5A1gjSAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T09:09:25.086321Z"},"content_sha256":"9dc84cb81968cab765d11c105a7224097e3c56b17408413e6feb7833ea270db3","schema_version":"1.0","event_id":"sha256:9dc84cb81968cab765d11c105a7224097e3c56b17408413e6feb7833ea270db3"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:FG5VQIUZA2MBFXSWJS4VPKIIC6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"QCD Wehrl and entanglement entropies in a gluon spectator model at small-$x$","license":"http://creativecommons.org/licenses/by/4.0/","headline":"In a small-x gluon spectator model, the Wehrl entropy from the Husimi distribution decomposes into an entanglement entropy term plus a transverse residual term, with numerical values matching CMS proton data.","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Gabriel Rabelo-Soares, Gabriel S. Ramos, Giorgio Torrieri, Reinaldo Francener","submitted_at":"2025-12-31T13:25:55Z","abstract_excerpt":"Recent studies have shown that hadronic multiplicity in deep inelastic scattering can be associated with entanglement entropy. However, such definitions are intrinsically longitudinal and do not capture the full phase-space structure of the proton. In this work, we investigate the proton Wehrl entropy constructed from the gluon Husimi distribution, which provides a positive phase-space description within the present definitions and model calculations. Within this framework, we employ a gluon light-front spectator model based on soft-wall AdS/QCD-inspired wave functions, with free parameters co"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"From a normalized Husimi distribution one can decompose the Wehrl entropy into an entanglement entropy term and a residual term associated with transverse degrees of freedom. Numerical results for the proton entanglement entropy are shown and compared with CMS data.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"The Husimi distribution is obtained via Gaussian smearing of the Wigner distribution with width given by the saturation scale in the GBW model, and the underlying wave functions are taken from the soft-wall AdS/QCD-inspired spectator model whose parameters are constrained by NNPDF fits.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"In a gluon spectator model at small x, the normalized Husimi distribution yields a Wehrl entropy that decomposes into an entanglement entropy term matching CMS data and a transverse residual term.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"In a small-x gluon spectator model, the Wehrl entropy from the Husimi distribution decomposes into an entanglement entropy term plus a transverse residual term, with numerical values matching CMS proton data.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"5b771e62e31c8bae532738e7e5bbebdcde310b5ee584038b0e76c644fe73ef5a"},"source":{"id":"2512.24855","kind":"arxiv","version":2},"verdict":{"id":"f410ffab-96bb-4877-ba79-b1dad7787b85","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-16T19:07:40.823984Z","strongest_claim":"From a normalized Husimi distribution one can decompose the Wehrl entropy into an entanglement entropy term and a residual term associated with transverse degrees of freedom. Numerical results for the proton entanglement entropy are shown and compared with CMS data.","one_line_summary":"In a gluon spectator model at small x, the normalized Husimi distribution yields a Wehrl entropy that decomposes into an entanglement entropy term matching CMS data and a transverse residual term.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"The Husimi distribution is obtained via Gaussian smearing of the Wigner distribution with width given by the saturation scale in the GBW model, and the underlying wave functions are taken from the soft-wall AdS/QCD-inspired spectator model whose parameters are constrained by NNPDF fits.","pith_extraction_headline":"In a small-x gluon spectator model, the Wehrl entropy from the Husimi distribution decomposes into an entanglement entropy term plus a transverse residual term, with numerical values matching CMS proton data."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2512.24855/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":57,"sample":[{"doi":"","year":2024,"title":"The solid blue line and the blue shadow represents the NNPDF 4.0 at NN LO data set for the unpolarized gluon PDF and its uncertainty band with 1 σ , respectively","work_id":"c5b46790-7757-4c3d-9a6d-a9453ab7f7db","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2017,"title":"D. E. Kharzeev and E. M. Levin, Physical Review D 95, 114008 (2017)","work_id":"5ad4110b-2e08-4eb9-ae2d-87a6f966318f","ref_index":2,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2020,"title":"Z. Tu, D. E. Kharzeev, and T. Ullrich, Physical review let ters 124, 062001 (2020)","work_id":"707ef830-bdca-4281-91b6-c058ce73b56f","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2021,"title":"D. E. Kharzeev and E. Levin, Physical Review D 104, L031503 (2021)","work_id":"eefca1dd-4835-42fc-8314-3debea488fa5","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2022,"title":"M. Hentschinski and K. Kutak, The European Physical Jour nal C 82, 111 (2022)","work_id":"b02f5e08-6b58-4fdb-9dc7-3bd7c6ea88a9","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":57,"snapshot_sha256":"4e3452873d35701fc2cc94861af14c69c6907dd630619ee488795a8df050e007","internal_anchors":18},"formal_canon":{"evidence_count":2,"snapshot_sha256":"569dfd6c0e72710d49f4a512ff4d840395f2f54faf479919a23cd00ace562dd8"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":"f410ffab-96bb-4877-ba79-b1dad7787b85"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-28T02:04:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"O1HqM29Wcongs3G+3A3qqHgJBw+P4Kd14r+Q6on5FTj4n1+cGGmWoEPwHuiCNFYASfJ8lJFFNh/Sd8eK/3SQAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T09:09:25.086903Z"},"content_sha256":"3bf0850d853e3ba40f8bc3eb2d2b339b7ef7ff3871adf2a0677088810b7a064b","schema_version":"1.0","event_id":"sha256:3bf0850d853e3ba40f8bc3eb2d2b339b7ef7ff3871adf2a0677088810b7a064b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FG5VQIUZA2MBFXSWJS4VPKIIC6/bundle.json","state_url":"https://pith.science/pith/FG5VQIUZA2MBFXSWJS4VPKIIC6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FG5VQIUZA2MBFXSWJS4VPKIIC6/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":"2026-06-01T09:09:25Z","links":{"resolver":"https://pith.science/pith/FG5VQIUZA2MBFXSWJS4VPKIIC6","bundle":"https://pith.science/pith/FG5VQIUZA2MBFXSWJS4VPKIIC6/bundle.json","state":"https://pith.science/pith/FG5VQIUZA2MBFXSWJS4VPKIIC6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FG5VQIUZA2MBFXSWJS4VPKIIC6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:FG5VQIUZA2MBFXSWJS4VPKIIC6","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":"b0991b8d4f47aed2419f754ea88545f69d4418a3532ca227ae29ae74b7d8f5fc","cross_cats_sorted":["nucl-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-12-31T13:25:55Z","title_canon_sha256":"f29718910824a09b2237075107a2d0cf99544430658619b2f7c375b695623379"},"schema_version":"1.0","source":{"id":"2512.24855","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2512.24855","created_at":"2026-05-28T02:04:44Z"},{"alias_kind":"arxiv_version","alias_value":"2512.24855v2","created_at":"2026-05-28T02:04:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2512.24855","created_at":"2026-05-28T02:04:44Z"},{"alias_kind":"pith_short_12","alias_value":"FG5VQIUZA2MB","created_at":"2026-05-28T02:04:44Z"},{"alias_kind":"pith_short_16","alias_value":"FG5VQIUZA2MBFXSW","created_at":"2026-05-28T02:04:44Z"},{"alias_kind":"pith_short_8","alias_value":"FG5VQIUZ","created_at":"2026-05-28T02:04:44Z"}],"graph_snapshots":[{"event_id":"sha256:3bf0850d853e3ba40f8bc3eb2d2b339b7ef7ff3871adf2a0677088810b7a064b","target":"graph","created_at":"2026-05-28T02:04:44Z","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":"From a normalized Husimi distribution one can decompose the Wehrl entropy into an entanglement entropy term and a residual term associated with transverse degrees of freedom. Numerical results for the proton entanglement entropy are shown and compared with CMS data."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"The Husimi distribution is obtained via Gaussian smearing of the Wigner distribution with width given by the saturation scale in the GBW model, and the underlying wave functions are taken from the soft-wall AdS/QCD-inspired spectator model whose parameters are constrained by NNPDF fits."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"In a gluon spectator model at small x, the normalized Husimi distribution yields a Wehrl entropy that decomposes into an entanglement entropy term matching CMS data and a transverse residual term."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"In a small-x gluon spectator model, the Wehrl entropy from the Husimi distribution decomposes into an entanglement entropy term plus a transverse residual term, with numerical values matching CMS proton data."}],"snapshot_sha256":"5b771e62e31c8bae532738e7e5bbebdcde310b5ee584038b0e76c644fe73ef5a"},"formal_canon":{"evidence_count":2,"snapshot_sha256":"569dfd6c0e72710d49f4a512ff4d840395f2f54faf479919a23cd00ace562dd8"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2512.24855/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Recent studies have shown that hadronic multiplicity in deep inelastic scattering can be associated with entanglement entropy. However, such definitions are intrinsically longitudinal and do not capture the full phase-space structure of the proton. In this work, we investigate the proton Wehrl entropy constructed from the gluon Husimi distribution, which provides a positive phase-space description within the present definitions and model calculations. Within this framework, we employ a gluon light-front spectator model based on soft-wall AdS/QCD-inspired wave functions, with free parameters co","authors_text":"Gabriel Rabelo-Soares, Gabriel S. Ramos, Giorgio Torrieri, Reinaldo Francener","cross_cats":["nucl-th"],"headline":"In a small-x gluon spectator model, the Wehrl entropy from the Husimi distribution decomposes into an entanglement entropy term plus a transverse residual term, with numerical values matching CMS proton data.","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-12-31T13:25:55Z","title":"QCD Wehrl and entanglement entropies in a gluon spectator model at small-$x$"},"references":{"count":57,"internal_anchors":18,"resolved_work":57,"sample":[{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":1,"title":"The solid blue line and the blue shadow represents the NNPDF 4.0 at NN LO data set for the unpolarized gluon PDF and its uncertainty band with 1 σ , respectively","work_id":"c5b46790-7757-4c3d-9a6d-a9453ab7f7db","year":2024},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":2,"title":"D. E. Kharzeev and E. M. Levin, Physical Review D 95, 114008 (2017)","work_id":"5ad4110b-2e08-4eb9-ae2d-87a6f966318f","year":2017},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":3,"title":"Z. Tu, D. E. Kharzeev, and T. Ullrich, Physical review let ters 124, 062001 (2020)","work_id":"707ef830-bdca-4281-91b6-c058ce73b56f","year":2020},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":4,"title":"D. E. Kharzeev and E. Levin, Physical Review D 104, L031503 (2021)","work_id":"eefca1dd-4835-42fc-8314-3debea488fa5","year":2021},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":5,"title":"M. Hentschinski and K. Kutak, The European Physical Jour nal C 82, 111 (2022)","work_id":"b02f5e08-6b58-4fdb-9dc7-3bd7c6ea88a9","year":2022}],"snapshot_sha256":"4e3452873d35701fc2cc94861af14c69c6907dd630619ee488795a8df050e007"},"source":{"id":"2512.24855","kind":"arxiv","version":2},"verdict":{"created_at":"2026-05-16T19:07:40.823984Z","id":"f410ffab-96bb-4877-ba79-b1dad7787b85","model_set":{"reader":"grok-4.3"},"one_line_summary":"In a gluon spectator model at small x, the normalized Husimi distribution yields a Wehrl entropy that decomposes into an entanglement entropy term matching CMS data and a transverse residual term.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"In a small-x gluon spectator model, the Wehrl entropy from the Husimi distribution decomposes into an entanglement entropy term plus a transverse residual term, with numerical values matching CMS proton data.","strongest_claim":"From a normalized Husimi distribution one can decompose the Wehrl entropy into an entanglement entropy term and a residual term associated with transverse degrees of freedom. Numerical results for the proton entanglement entropy are shown and compared with CMS data.","weakest_assumption":"The Husimi distribution is obtained via Gaussian smearing of the Wigner distribution with width given by the saturation scale in the GBW model, and the underlying wave functions are taken from the soft-wall AdS/QCD-inspired spectator model whose parameters are constrained by NNPDF fits."}},"verdict_id":"f410ffab-96bb-4877-ba79-b1dad7787b85"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:9dc84cb81968cab765d11c105a7224097e3c56b17408413e6feb7833ea270db3","target":"record","created_at":"2026-05-28T02:04:44Z","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":"b0991b8d4f47aed2419f754ea88545f69d4418a3532ca227ae29ae74b7d8f5fc","cross_cats_sorted":["nucl-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-12-31T13:25:55Z","title_canon_sha256":"f29718910824a09b2237075107a2d0cf99544430658619b2f7c375b695623379"},"schema_version":"1.0","source":{"id":"2512.24855","kind":"arxiv","version":2}},"canonical_sha256":"29bb582299069812de564cb957a9081792bcdc2b5b7d7913b49043fff0b1cfa6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"29bb582299069812de564cb957a9081792bcdc2b5b7d7913b49043fff0b1cfa6","first_computed_at":"2026-05-28T02:04:44.982255Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-28T02:04:44.982255Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"p6M9tavgdKQGjwLQDTvjQf8J2rN75XAJWfBsIlkDU0mAGBbhc0kxUNvI3CGBt3t5a3FEywBlWfE24651bQtlCg==","signature_status":"signed_v1","signed_at":"2026-05-28T02:04:44.982865Z","signed_message":"canonical_sha256_bytes"},"source_id":"2512.24855","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9dc84cb81968cab765d11c105a7224097e3c56b17408413e6feb7833ea270db3","sha256:3bf0850d853e3ba40f8bc3eb2d2b339b7ef7ff3871adf2a0677088810b7a064b"],"state_sha256":"6719858a6d66a8cab726972fea8efea904d0c4ba12a530633258efa0d64db1b9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vEVtipEmQSdLsbVsvSOiEGiaxfFtpz9xlcZhuL+Hvjr77uXkCGralxslMqfcG8V0zD0xdD1BHd/YXZp5WzttCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T09:09:25.089493Z","bundle_sha256":"b7b536aba6f86ce3b9fdef0ad06c2144b47b3c6e267fd194eef7f2db35e1ac4f"}}