{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:2MBV6E23N3KTDQZDUEF6PEBGAU","short_pith_number":"pith:2MBV6E23","canonical_record":{"source":{"id":"2605.13614","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2026-05-13T14:45:01Z","cross_cats_sorted":[],"title_canon_sha256":"5d43c5270a589391394c5e9252a38575680824390943ac7ba19d80c76b5e9ee9","abstract_canon_sha256":"2d56ef936c0236021aff679099f6ed020c239ccba30f78e1be9e019979950eeb"},"schema_version":"1.0"},"canonical_sha256":"d3035f135b6ed531c323a10be7902605153c3310652ac76dc04b442b437708bb","source":{"kind":"arxiv","id":"2605.13614","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.13614","created_at":"2026-05-18T02:44:17Z"},{"alias_kind":"arxiv_version","alias_value":"2605.13614v1","created_at":"2026-05-18T02:44:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.13614","created_at":"2026-05-18T02:44:17Z"},{"alias_kind":"pith_short_12","alias_value":"2MBV6E23N3KT","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_16","alias_value":"2MBV6E23N3KTDQZD","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_8","alias_value":"2MBV6E23","created_at":"2026-05-18T12:33:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:2MBV6E23N3KTDQZDUEF6PEBGAU","target":"record","payload":{"canonical_record":{"source":{"id":"2605.13614","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2026-05-13T14:45:01Z","cross_cats_sorted":[],"title_canon_sha256":"5d43c5270a589391394c5e9252a38575680824390943ac7ba19d80c76b5e9ee9","abstract_canon_sha256":"2d56ef936c0236021aff679099f6ed020c239ccba30f78e1be9e019979950eeb"},"schema_version":"1.0"},"canonical_sha256":"d3035f135b6ed531c323a10be7902605153c3310652ac76dc04b442b437708bb","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:44:17.995753Z","signature_b64":"2y7cbO5KzT/N4kxBpESkuUS8fmpAJr7AP5CcF2iY+ZbhpekgR3hpJUSzwfOCNudVs4xmZizgwBC4huG2SEi5BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d3035f135b6ed531c323a10be7902605153c3310652ac76dc04b442b437708bb","last_reissued_at":"2026-05-18T02:44:17.995224Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:44:17.995224Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2605.13614","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":"2026-05-18T02:44:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"TiMxcgwaNawWrY6hrkJ0bAnuSK6nX0JDfdBMTELeRIpOmhHAnZ9veSitBAsGQyt2tMLFa2R5nt4mJoxEdujDDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T21:37:48.978135Z"},"content_sha256":"fd35ca0dd83ae9548b0e56f5b0333443337cf9d6d3873ccccbff3f76ef799a66","schema_version":"1.0","event_id":"sha256:fd35ca0dd83ae9548b0e56f5b0333443337cf9d6d3873ccccbff3f76ef799a66"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:2MBV6E23N3KTDQZDUEF6PEBGAU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Search for pair production of additional neutral scalars within the Inert Doublet Model in a final state with two electrons or two muons in proton-proton collisions at $\\sqrt{s}$ = 13 TeV and 13.6 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"No significant excess observed in first dedicated search for inert doublet scalars, excluding masses up to 108 GeV","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2026-05-13T14:45:01Z","abstract_excerpt":"A first dedicated search for pair production of new scalars predicted by the Inert Doublet Model is performed using proton-proton collisions. Data were collected with the CMS detector at the CERN LHC at $\\sqrt{s}$ = 13 TeV and 13.6 TeV, corresponding to integrated luminosities of 138 fb$^{-1}$ and 35 fb$^{-1}$, respectively. Within this model, four additional scalar bosons (H, A, H$^+$, and H$^-$) are predicted. Through an additional discrete symmetry, the lightest new scalar, H, is stable, rendering it a viable dark matter candidate. These candidates can originate from quark-antiquark annihil"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"No significant excess of events is observed. Exclusion limits at 95% confidence level are set on the production cross section of the two new neutral scalars, H and A, expressed in terms of their masses, m_H and m_A, in the m_H vs. m_A plane. The observed (expected) exclusion region reaches m_H = 108 (106) GeV for m_H-m_A = 78 (76) GeV.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"Standard Model backgrounds are accurately modeled and subtracted, and the signal acceptance and efficiency for the Inert Doublet Model are correctly simulated across the scanned mass points.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"No significant excess found; new exclusion limits reach m_H = 108 GeV for m_H - m_A = 78 GeV in the Inert Doublet Model.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"No significant excess observed in first dedicated search for inert doublet scalars, excluding masses up to 108 GeV","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"130476928e30344fc848c1873e023ff40a5629e8d141036da5696056256fb5d3"},"source":{"id":"2605.13614","kind":"arxiv","version":1},"verdict":{"id":"132571c4-e060-4a6f-a5b2-2b680d40a6d0","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-14T17:59:41.745704Z","strongest_claim":"No significant excess of events is observed. Exclusion limits at 95% confidence level are set on the production cross section of the two new neutral scalars, H and A, expressed in terms of their masses, m_H and m_A, in the m_H vs. m_A plane. The observed (expected) exclusion region reaches m_H = 108 (106) GeV for m_H-m_A = 78 (76) GeV.","one_line_summary":"No significant excess found; new exclusion limits reach m_H = 108 GeV for m_H - m_A = 78 GeV in the Inert Doublet Model.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"Standard Model backgrounds are accurately modeled and subtracted, and the signal acceptance and efficiency for the Inert Doublet Model are correctly simulated across the scanned mass points.","pith_extraction_headline":"No significant excess observed in first dedicated search for inert doublet scalars, excluding masses up to 108 GeV"},"references":{"count":107,"sample":[{"doi":"10.1103/physrevd.110.030001","year":2024,"title":"Review of particle physics","work_id":"6e4dcae4-4b24-43e5-bee3-2fc9806bc8b5","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"10.1088/1361-6633/aab913","year":2018,"title":"WIMP dark matter candidates and searches - current status and future prospects","work_id":"d69fbcc8-6817-4340-ba5a-947be2f63ef2","ref_index":2,"cited_arxiv_id":"1707.06277","is_internal_anchor":true},{"doi":"10.1016/j.physrep.2024.10.001","year":2025,"title":"Exploration at the high-energy frontier: ATLAS Run 2 searches investigating the exotic jungle beyond the Standard Model","work_id":"5f067619-ac20-4bc8-be54-db7166ea0166","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"10.1016/j.physrep.2024.09.013","year":2025,"title":"arXiv:2405.13778 [hep-ex]","work_id":"7a1e9313-de25-4d2b-ad0e-ba0f0f6b5a19","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"10.1103/physrevd.18.2574","year":1978,"title":"Pattern of symmetry breaking with two Higgs doublets","work_id":"4bbb135e-09d5-4313-bd57-08d799beca73","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":107,"snapshot_sha256":"f00eee93192879a898e414fa741750e6ce02a9cc386c72e6e634fbb6eff4b106","internal_anchors":58},"formal_canon":{"evidence_count":2,"snapshot_sha256":"6211b7382efefbf7860e9e974d5a79941c72185403a2baf3006ed5a1e25f7bd4"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":"132571c4-e060-4a6f-a5b2-2b680d40a6d0"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:44:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BJVfLls4iKELc02c6p2OTfrkqr3q2oCTVx1NxSJy/mM1QJL+YCb6r3Xre9wCY8M33glkxTOaHlmX7+Be0qgJBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T21:37:48.981105Z"},"content_sha256":"e7943e9bbc94d8ade9da37b92eaa56f812e1744d38813075339227defc2f6f40","schema_version":"1.0","event_id":"sha256:e7943e9bbc94d8ade9da37b92eaa56f812e1744d38813075339227defc2f6f40"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:2MBV6E23N3KTDQZDUEF6PEBGAU","target":"integrity","payload":{"note":"Identifier '10.17182/hepdata.172869' is syntactically valid but the DOI registry (doi.org) returned 404, and Crossref / OpenAlex / internal corpus also have no record. The cited work could not be located through any authoritative source.","snippet":"HEPData record for this analysis, 2026.doi:10.17182/hepdata.172869","arxiv_id":"2605.13614","detector":"doi_compliance","evidence":{"doi":"10.17182/hepdata.172869","arxiv_id":null,"ref_index":29,"raw_excerpt":"HEPData record for this analysis, 2026.doi:10.17182/hepdata.172869","verdict_class":"cross_source","checked_sources":["crossref_by_doi","openalex_by_doi","doi_org_head"]},"severity":"critical","ref_index":29,"audited_at":"2026-05-19T06:21:55.296340Z","event_type":"pith.integrity.v1","detected_doi":"10.17182/hepdata.172869","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"unresolvable_identifier","evidence_hash":"63bee96451828074c73e563772527e882b073db609a434eb4c4832ab4409ae4c","paper_version":1,"verdict_class":"cross_source","resolved_title":null,"detector_version":"1.0.0","detected_arxiv_id":null,"integrity_event_id":127,"payload_sha256":"4937dc014b96704f61885b0ee03ba25d4e33fe37c8d5fe11995d9b18e29ad262","signature_b64":"NMT0soMY7ZyXmS5vj3uCQrAoPaDDex726bofnGDdBJwWSq7VHBUkWKvILp2JBO+7shvokUUgCqSAVeDNkCUiAg==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-19T06:26:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qR6HPNZL79X/5SBuJUjAL2B2UCW5V2FYXtT+/w9mb+5CBB1eZ0UK2vkkHWXPArx86iACI3kGGOq/QHI/x3mfBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T21:37:48.982252Z"},"content_sha256":"ca5a86254d06edd6a3cbb756fc9bd2e4668ba09a1d4a30182137164b7e7ec404","schema_version":"1.0","event_id":"sha256:ca5a86254d06edd6a3cbb756fc9bd2e4668ba09a1d4a30182137164b7e7ec404"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2MBV6E23N3KTDQZDUEF6PEBGAU/bundle.json","state_url":"https://pith.science/pith/2MBV6E23N3KTDQZDUEF6PEBGAU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2MBV6E23N3KTDQZDUEF6PEBGAU/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":"2026-05-21T21:37:48Z","links":{"resolver":"https://pith.science/pith/2MBV6E23N3KTDQZDUEF6PEBGAU","bundle":"https://pith.science/pith/2MBV6E23N3KTDQZDUEF6PEBGAU/bundle.json","state":"https://pith.science/pith/2MBV6E23N3KTDQZDUEF6PEBGAU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2MBV6E23N3KTDQZDUEF6PEBGAU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:2MBV6E23N3KTDQZDUEF6PEBGAU","merge_version":"pith-open-graph-merge-v1","event_count":3,"valid_event_count":3,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"2d56ef936c0236021aff679099f6ed020c239ccba30f78e1be9e019979950eeb","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2026-05-13T14:45:01Z","title_canon_sha256":"5d43c5270a589391394c5e9252a38575680824390943ac7ba19d80c76b5e9ee9"},"schema_version":"1.0","source":{"id":"2605.13614","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.13614","created_at":"2026-05-18T02:44:17Z"},{"alias_kind":"arxiv_version","alias_value":"2605.13614v1","created_at":"2026-05-18T02:44:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.13614","created_at":"2026-05-18T02:44:17Z"},{"alias_kind":"pith_short_12","alias_value":"2MBV6E23N3KT","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_16","alias_value":"2MBV6E23N3KTDQZD","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_8","alias_value":"2MBV6E23","created_at":"2026-05-18T12:33:37Z"}],"graph_snapshots":[{"event_id":"sha256:e7943e9bbc94d8ade9da37b92eaa56f812e1744d38813075339227defc2f6f40","target":"graph","created_at":"2026-05-18T02:44:17Z","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":"No significant excess of events is observed. Exclusion limits at 95% confidence level are set on the production cross section of the two new neutral scalars, H and A, expressed in terms of their masses, m_H and m_A, in the m_H vs. m_A plane. The observed (expected) exclusion region reaches m_H = 108 (106) GeV for m_H-m_A = 78 (76) GeV."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"Standard Model backgrounds are accurately modeled and subtracted, and the signal acceptance and efficiency for the Inert Doublet Model are correctly simulated across the scanned mass points."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"No significant excess found; new exclusion limits reach m_H = 108 GeV for m_H - m_A = 78 GeV in the Inert Doublet Model."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"No significant excess observed in first dedicated search for inert doublet scalars, excluding masses up to 108 GeV"}],"snapshot_sha256":"130476928e30344fc848c1873e023ff40a5629e8d141036da5696056256fb5d3"},"formal_canon":{"evidence_count":2,"snapshot_sha256":"6211b7382efefbf7860e9e974d5a79941c72185403a2baf3006ed5a1e25f7bd4"},"paper":{"abstract_excerpt":"A first dedicated search for pair production of new scalars predicted by the Inert Doublet Model is performed using proton-proton collisions. Data were collected with the CMS detector at the CERN LHC at $\\sqrt{s}$ = 13 TeV and 13.6 TeV, corresponding to integrated luminosities of 138 fb$^{-1}$ and 35 fb$^{-1}$, respectively. Within this model, four additional scalar bosons (H, A, H$^+$, and H$^-$) are predicted. Through an additional discrete symmetry, the lightest new scalar, H, is stable, rendering it a viable dark matter candidate. These candidates can originate from quark-antiquark annihil","authors_text":"CMS Collaboration","cross_cats":[],"headline":"No significant excess observed in first dedicated search for inert doublet scalars, excluding masses up to 108 GeV","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2026-05-13T14:45:01Z","title":"Search for pair production of additional neutral scalars within the Inert Doublet Model in a final state with two electrons or two muons in proton-proton collisions at $\\sqrt{s}$ = 13 TeV and 13.6 TeV"},"references":{"count":107,"internal_anchors":58,"resolved_work":107,"sample":[{"cited_arxiv_id":"","doi":"10.1103/physrevd.110.030001","is_internal_anchor":false,"ref_index":1,"title":"Review of particle physics","work_id":"6e4dcae4-4b24-43e5-bee3-2fc9806bc8b5","year":2024},{"cited_arxiv_id":"1707.06277","doi":"10.1088/1361-6633/aab913","is_internal_anchor":true,"ref_index":2,"title":"WIMP dark matter candidates and searches - current status and future prospects","work_id":"d69fbcc8-6817-4340-ba5a-947be2f63ef2","year":2018},{"cited_arxiv_id":"","doi":"10.1016/j.physrep.2024.10.001","is_internal_anchor":false,"ref_index":3,"title":"Exploration at the high-energy frontier: ATLAS Run 2 searches investigating the exotic jungle beyond the Standard Model","work_id":"5f067619-ac20-4bc8-be54-db7166ea0166","year":2025},{"cited_arxiv_id":"","doi":"10.1016/j.physrep.2024.09.013","is_internal_anchor":false,"ref_index":4,"title":"arXiv:2405.13778 [hep-ex]","work_id":"7a1e9313-de25-4d2b-ad0e-ba0f0f6b5a19","year":2025},{"cited_arxiv_id":"","doi":"10.1103/physrevd.18.2574","is_internal_anchor":false,"ref_index":5,"title":"Pattern of symmetry breaking with two Higgs doublets","work_id":"4bbb135e-09d5-4313-bd57-08d799beca73","year":1978}],"snapshot_sha256":"f00eee93192879a898e414fa741750e6ce02a9cc386c72e6e634fbb6eff4b106"},"source":{"id":"2605.13614","kind":"arxiv","version":1},"verdict":{"created_at":"2026-05-14T17:59:41.745704Z","id":"132571c4-e060-4a6f-a5b2-2b680d40a6d0","model_set":{"reader":"grok-4.3"},"one_line_summary":"No significant excess found; new exclusion limits reach m_H = 108 GeV for m_H - m_A = 78 GeV in the Inert Doublet Model.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"No significant excess observed in first dedicated search for inert doublet scalars, excluding masses up to 108 GeV","strongest_claim":"No significant excess of events is observed. Exclusion limits at 95% confidence level are set on the production cross section of the two new neutral scalars, H and A, expressed in terms of their masses, m_H and m_A, in the m_H vs. m_A plane. The observed (expected) exclusion region reaches m_H = 108 (106) GeV for m_H-m_A = 78 (76) GeV.","weakest_assumption":"Standard Model backgrounds are accurately modeled and subtracted, and the signal acceptance and efficiency for the Inert Doublet Model are correctly simulated across the scanned mass points."}},"verdict_id":"132571c4-e060-4a6f-a5b2-2b680d40a6d0"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:fd35ca0dd83ae9548b0e56f5b0333443337cf9d6d3873ccccbff3f76ef799a66","target":"record","created_at":"2026-05-18T02:44:17Z","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":"2d56ef936c0236021aff679099f6ed020c239ccba30f78e1be9e019979950eeb","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2026-05-13T14:45:01Z","title_canon_sha256":"5d43c5270a589391394c5e9252a38575680824390943ac7ba19d80c76b5e9ee9"},"schema_version":"1.0","source":{"id":"2605.13614","kind":"arxiv","version":1}},"canonical_sha256":"d3035f135b6ed531c323a10be7902605153c3310652ac76dc04b442b437708bb","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d3035f135b6ed531c323a10be7902605153c3310652ac76dc04b442b437708bb","first_computed_at":"2026-05-18T02:44:17.995224Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:44:17.995224Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2y7cbO5KzT/N4kxBpESkuUS8fmpAJr7AP5CcF2iY+ZbhpekgR3hpJUSzwfOCNudVs4xmZizgwBC4huG2SEi5BQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:44:17.995753Z","signed_message":"canonical_sha256_bytes"},"source_id":"2605.13614","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fd35ca0dd83ae9548b0e56f5b0333443337cf9d6d3873ccccbff3f76ef799a66","sha256:e7943e9bbc94d8ade9da37b92eaa56f812e1744d38813075339227defc2f6f40","sha256:ca5a86254d06edd6a3cbb756fc9bd2e4668ba09a1d4a30182137164b7e7ec404"],"state_sha256":"02551db64773255bdb6942d4270d025ea3e959e136be518b0b326fcf7472c55f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vDiKg9EWW9H6A8fjfblIqY6Ea8CBq/H/K6UV8KrjBn2pYua+Vpl+7dQuL9941LeMQyz6AZh9O9Y5nQEonjOAAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-21T21:37:48.984663Z","bundle_sha256":"312f01a14fd905cc2f4fe3666b21902b3fcd11fb9a36f72af061b5b020eadcf5"}}