{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:FW5UCLMCILZNQQRHRPLJKKUUFP","short_pith_number":"pith:FW5UCLMC","canonical_record":{"source":{"id":"2605.16693","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/publicdomain/zero/1.0/","primary_cat":"q-bio.PE","submitted_at":"2026-05-15T23:10:35Z","cross_cats_sorted":["cond-mat.stat-mech","math.PR","physics.bio-ph"],"title_canon_sha256":"36ebeefc4498081ef050ad27cb840693f818383619e8886e9a1e7be504ffd7c6","abstract_canon_sha256":"450fc7e282851f1f56bdb3ba66c8ffd1f9af2c9dae73b0c9422aa65aeef9a7ff"},"schema_version":"1.0"},"canonical_sha256":"2dbb412d8242f2d842278bd6952a942bcd2cfb14d9fff5f116bed3cf0218c680","source":{"kind":"arxiv","id":"2605.16693","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.16693","created_at":"2026-05-20T00:02:36Z"},{"alias_kind":"arxiv_version","alias_value":"2605.16693v1","created_at":"2026-05-20T00:02:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.16693","created_at":"2026-05-20T00:02:36Z"},{"alias_kind":"pith_short_12","alias_value":"FW5UCLMCILZN","created_at":"2026-05-20T00:02:36Z"},{"alias_kind":"pith_short_16","alias_value":"FW5UCLMCILZNQQRH","created_at":"2026-05-20T00:02:36Z"},{"alias_kind":"pith_short_8","alias_value":"FW5UCLMC","created_at":"2026-05-20T00:02:36Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:FW5UCLMCILZNQQRHRPLJKKUUFP","target":"record","payload":{"canonical_record":{"source":{"id":"2605.16693","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/publicdomain/zero/1.0/","primary_cat":"q-bio.PE","submitted_at":"2026-05-15T23:10:35Z","cross_cats_sorted":["cond-mat.stat-mech","math.PR","physics.bio-ph"],"title_canon_sha256":"36ebeefc4498081ef050ad27cb840693f818383619e8886e9a1e7be504ffd7c6","abstract_canon_sha256":"450fc7e282851f1f56bdb3ba66c8ffd1f9af2c9dae73b0c9422aa65aeef9a7ff"},"schema_version":"1.0"},"canonical_sha256":"2dbb412d8242f2d842278bd6952a942bcd2cfb14d9fff5f116bed3cf0218c680","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-20T00:02:36.940869Z","signature_b64":"VsyypkN3ZdYJ3b+R48CyJCZhwswYLgSBc8u+kzLijsuL0dtCCWTAlo+4kTt4lxe8sM+YOY0De+qx3TJnS8VXDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2dbb412d8242f2d842278bd6952a942bcd2cfb14d9fff5f116bed3cf0218c680","last_reissued_at":"2026-05-20T00:02:36.940046Z","signature_status":"signed_v1","first_computed_at":"2026-05-20T00:02:36.940046Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2605.16693","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":"2026-05-20T00:02:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bD7PMgPRV4UfGMRQGXQl7N2xXt/jjuPEzY3J9ENN0V/lQEBto+cOzbhddIKRByeDRnQu72exkKfy5Ulhbsk1BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T09:41:49.411510Z"},"content_sha256":"d89feddbee147c35cc99808b9bb3b11d692340e421d5f98e1b894ab4c93cf4c1","schema_version":"1.0","event_id":"sha256:d89feddbee147c35cc99808b9bb3b11d692340e421d5f98e1b894ab4c93cf4c1"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:FW5UCLMCILZNQQRHRPLJKKUUFP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Branching under First-Passage Resetting","license":"http://creativecommons.org/publicdomain/zero/1.0/","headline":"Stochastic timing fluctuations in first-passage triggered replication enhance population growth for fixed offspring number and mean time.","cross_cats":["cond-mat.stat-mech","math.PR","physics.bio-ph"],"primary_cat":"q-bio.PE","authors_text":"Aanjaneya Kumar, James Holehouse","submitted_at":"2026-05-15T23:10:35Z","abstract_excerpt":"Many biological processes, from cell division to viral lysis, are triggered when an internal stochastic variable reaches a threshold. Here we introduce Branching under First-Passage Resetting, a general framework in which replication events arise endogenously from first-passage dynamics rather than from externally imposed lifetime clocks. We show that the resulting population dynamics obey an exact renewal equation linking single-trajectory first-passage statistics to the population growth rate. This mapping shows that, for fixed offspring number and fixed mean replication time, stochastic tim"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"for fixed offspring number and fixed mean replication time, stochastic timing fluctuations necessarily enhance growth relative to a deterministic clock. When offspring yield depends on the first-passage time, fluctuations have non-trivial effects and expose a fundamental yield-delay trade-off.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"The population dynamics obey an exact renewal equation linking single-trajectory first-passage statistics to the population growth rate (abstract, paragraph 2), which presupposes that first-passage processes across independent lineages are statistically identical and that the branching occurs precisely at the first-passage event.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"New framework links first-passage timing statistics to branching population growth via renewal equations, showing fluctuations enhance growth for fixed offspring and mean time while exposing optimization trade-offs, with bacteriophage lysis application matching empirical data.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"Stochastic timing fluctuations in first-passage triggered replication enhance population growth for fixed offspring number and mean time.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"76cdecfd611a12d616edc602d7f76fcfd858dca15e95d2425539eb94b74cdfb2"},"source":{"id":"2605.16693","kind":"arxiv","version":1},"verdict":{"id":"8028c962-b748-48d0-a34d-3b75de93bbf0","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-19T20:49:24.835833Z","strongest_claim":"for fixed offspring number and fixed mean replication time, stochastic timing fluctuations necessarily enhance growth relative to a deterministic clock. When offspring yield depends on the first-passage time, fluctuations have non-trivial effects and expose a fundamental yield-delay trade-off.","one_line_summary":"New framework links first-passage timing statistics to branching population growth via renewal equations, showing fluctuations enhance growth for fixed offspring and mean time while exposing optimization trade-offs, with bacteriophage lysis application matching empirical data.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"The population dynamics obey an exact renewal equation linking single-trajectory first-passage statistics to the population growth rate (abstract, paragraph 2), which presupposes that first-passage processes across independent lineages are statistically identical and that the branching occurs precisely at the first-passage event.","pith_extraction_headline":"Stochastic timing fluctuations in first-passage triggered replication enhance population growth for fixed offspring number and mean time."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2605.16693/integrity.json","findings":[],"available":true,"detectors_run":[{"name":"doi_compliance","ran_at":"2026-05-19T21:01:43.189266Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"doi_title_agreement","ran_at":"2026-05-19T21:01:19.283784Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"claim_evidence","ran_at":"2026-05-19T19:01:56.372716Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"ai_meta_artifact","ran_at":"2026-05-19T18:33:26.493721Z","status":"skipped","version":"1.0.0","findings_count":0}],"snapshot_sha256":"5bc642cabc7bb6ad365e882776dc38e5dbfcfb84711ba292101b29f5c2f9ec17"},"references":{"count":59,"sample":[{"doi":"","year":null,"title":"H. W. Watson and G. Galton, On the probability of the extinction of families, The Journal of the Anthropological Institute of Great Britain and Ireland4, 138 (1875)","work_id":"d9015e76-d967-475d-8524-b24e99d77721","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":1948,"title":"R. Bellman and T. E. Harris, On the theory of age- dependent stochastic branching processes, Proceedings of the National Academy of Sciences34, 601 (1948)","work_id":"3474f0c2-e01a-4cfb-a2ad-1a1fb81037b1","ref_index":2,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":1948,"title":"T. E. Harris, Branching processes, The Annals of Math- ematical Statistics , 474 (1948)","work_id":"07efd609-a897-49a9-805a-088360083df5","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":1963,"title":"T. E. Harriset al.,The theory of branching processes, Vol. 6 (Springer Berlin, 1963)","work_id":"9ec7a2b3-b5f4-4a60-a246-ca83c6a523ac","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":1983,"title":"S.AsmussenandH.Hering,Branchingprocesses, (1983)","work_id":"3e573ce2-bf58-424e-8e8a-10ea5d88896a","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":59,"snapshot_sha256":"a023c5d0fdcf2111207a83bf7106bfa5d0b9c6c8c26c42ab7caec4ca909f013c","internal_anchors":0},"formal_canon":{"evidence_count":2,"snapshot_sha256":"3dae29a2e4de0c89aedcf8de5523cec003a2e1cbaaaa910471f30d8592247d2d"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":"8028c962-b748-48d0-a34d-3b75de93bbf0"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-20T00:02:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DC78ojEGoy1oMHzua+bEAmPzRswu9IE11v+QnRG62/sLv1H2lU4knJxEbtX64MjvLiWgxS14+HaUMxs1IwgPAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T09:41:49.412122Z"},"content_sha256":"9b365845d3cad60931d3e171a5e8bcedb14f8974c0cffdc063a28cab277f9261","schema_version":"1.0","event_id":"sha256:9b365845d3cad60931d3e171a5e8bcedb14f8974c0cffdc063a28cab277f9261"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FW5UCLMCILZNQQRHRPLJKKUUFP/bundle.json","state_url":"https://pith.science/pith/FW5UCLMCILZNQQRHRPLJKKUUFP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FW5UCLMCILZNQQRHRPLJKKUUFP/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":"2026-05-28T09:41:49Z","links":{"resolver":"https://pith.science/pith/FW5UCLMCILZNQQRHRPLJKKUUFP","bundle":"https://pith.science/pith/FW5UCLMCILZNQQRHRPLJKKUUFP/bundle.json","state":"https://pith.science/pith/FW5UCLMCILZNQQRHRPLJKKUUFP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FW5UCLMCILZNQQRHRPLJKKUUFP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:FW5UCLMCILZNQQRHRPLJKKUUFP","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":"450fc7e282851f1f56bdb3ba66c8ffd1f9af2c9dae73b0c9422aa65aeef9a7ff","cross_cats_sorted":["cond-mat.stat-mech","math.PR","physics.bio-ph"],"license":"http://creativecommons.org/publicdomain/zero/1.0/","primary_cat":"q-bio.PE","submitted_at":"2026-05-15T23:10:35Z","title_canon_sha256":"36ebeefc4498081ef050ad27cb840693f818383619e8886e9a1e7be504ffd7c6"},"schema_version":"1.0","source":{"id":"2605.16693","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.16693","created_at":"2026-05-20T00:02:36Z"},{"alias_kind":"arxiv_version","alias_value":"2605.16693v1","created_at":"2026-05-20T00:02:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.16693","created_at":"2026-05-20T00:02:36Z"},{"alias_kind":"pith_short_12","alias_value":"FW5UCLMCILZN","created_at":"2026-05-20T00:02:36Z"},{"alias_kind":"pith_short_16","alias_value":"FW5UCLMCILZNQQRH","created_at":"2026-05-20T00:02:36Z"},{"alias_kind":"pith_short_8","alias_value":"FW5UCLMC","created_at":"2026-05-20T00:02:36Z"}],"graph_snapshots":[{"event_id":"sha256:9b365845d3cad60931d3e171a5e8bcedb14f8974c0cffdc063a28cab277f9261","target":"graph","created_at":"2026-05-20T00:02:36Z","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":"for fixed offspring number and fixed mean replication time, stochastic timing fluctuations necessarily enhance growth relative to a deterministic clock. When offspring yield depends on the first-passage time, fluctuations have non-trivial effects and expose a fundamental yield-delay trade-off."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"The population dynamics obey an exact renewal equation linking single-trajectory first-passage statistics to the population growth rate (abstract, paragraph 2), which presupposes that first-passage processes across independent lineages are statistically identical and that the branching occurs precisely at the first-passage event."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"New framework links first-passage timing statistics to branching population growth via renewal equations, showing fluctuations enhance growth for fixed offspring and mean time while exposing optimization trade-offs, with bacteriophage lysis application matching empirical data."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"Stochastic timing fluctuations in first-passage triggered replication enhance population growth for fixed offspring number and mean time."}],"snapshot_sha256":"76cdecfd611a12d616edc602d7f76fcfd858dca15e95d2425539eb94b74cdfb2"},"formal_canon":{"evidence_count":2,"snapshot_sha256":"3dae29a2e4de0c89aedcf8de5523cec003a2e1cbaaaa910471f30d8592247d2d"},"integrity":{"available":true,"clean":true,"detectors_run":[{"findings_count":0,"name":"doi_compliance","ran_at":"2026-05-19T21:01:43.189266Z","status":"completed","version":"1.0.0"},{"findings_count":0,"name":"doi_title_agreement","ran_at":"2026-05-19T21:01:19.283784Z","status":"completed","version":"1.0.0"},{"findings_count":0,"name":"claim_evidence","ran_at":"2026-05-19T19:01:56.372716Z","status":"completed","version":"1.0.0"},{"findings_count":0,"name":"ai_meta_artifact","ran_at":"2026-05-19T18:33:26.493721Z","status":"skipped","version":"1.0.0"}],"endpoint":"/pith/2605.16693/integrity.json","findings":[],"snapshot_sha256":"5bc642cabc7bb6ad365e882776dc38e5dbfcfb84711ba292101b29f5c2f9ec17","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Many biological processes, from cell division to viral lysis, are triggered when an internal stochastic variable reaches a threshold. Here we introduce Branching under First-Passage Resetting, a general framework in which replication events arise endogenously from first-passage dynamics rather than from externally imposed lifetime clocks. We show that the resulting population dynamics obey an exact renewal equation linking single-trajectory first-passage statistics to the population growth rate. This mapping shows that, for fixed offspring number and fixed mean replication time, stochastic tim","authors_text":"Aanjaneya Kumar, James Holehouse","cross_cats":["cond-mat.stat-mech","math.PR","physics.bio-ph"],"headline":"Stochastic timing fluctuations in first-passage triggered replication enhance population growth for fixed offspring number and mean time.","license":"http://creativecommons.org/publicdomain/zero/1.0/","primary_cat":"q-bio.PE","submitted_at":"2026-05-15T23:10:35Z","title":"Branching under First-Passage Resetting"},"references":{"count":59,"internal_anchors":0,"resolved_work":59,"sample":[{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":1,"title":"H. W. Watson and G. Galton, On the probability of the extinction of families, The Journal of the Anthropological Institute of Great Britain and Ireland4, 138 (1875)","work_id":"d9015e76-d967-475d-8524-b24e99d77721","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":2,"title":"R. Bellman and T. E. Harris, On the theory of age- dependent stochastic branching processes, Proceedings of the National Academy of Sciences34, 601 (1948)","work_id":"3474f0c2-e01a-4cfb-a2ad-1a1fb81037b1","year":1948},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":3,"title":"T. E. Harris, Branching processes, The Annals of Math- ematical Statistics , 474 (1948)","work_id":"07efd609-a897-49a9-805a-088360083df5","year":1948},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":4,"title":"T. E. Harriset al.,The theory of branching processes, Vol. 6 (Springer Berlin, 1963)","work_id":"9ec7a2b3-b5f4-4a60-a246-ca83c6a523ac","year":1963},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":5,"title":"S.AsmussenandH.Hering,Branchingprocesses, (1983)","work_id":"3e573ce2-bf58-424e-8e8a-10ea5d88896a","year":1983}],"snapshot_sha256":"a023c5d0fdcf2111207a83bf7106bfa5d0b9c6c8c26c42ab7caec4ca909f013c"},"source":{"id":"2605.16693","kind":"arxiv","version":1},"verdict":{"created_at":"2026-05-19T20:49:24.835833Z","id":"8028c962-b748-48d0-a34d-3b75de93bbf0","model_set":{"reader":"grok-4.3"},"one_line_summary":"New framework links first-passage timing statistics to branching population growth via renewal equations, showing fluctuations enhance growth for fixed offspring and mean time while exposing optimization trade-offs, with bacteriophage lysis application matching empirical data.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"Stochastic timing fluctuations in first-passage triggered replication enhance population growth for fixed offspring number and mean time.","strongest_claim":"for fixed offspring number and fixed mean replication time, stochastic timing fluctuations necessarily enhance growth relative to a deterministic clock. When offspring yield depends on the first-passage time, fluctuations have non-trivial effects and expose a fundamental yield-delay trade-off.","weakest_assumption":"The population dynamics obey an exact renewal equation linking single-trajectory first-passage statistics to the population growth rate (abstract, paragraph 2), which presupposes that first-passage processes across independent lineages are statistically identical and that the branching occurs precisely at the first-passage event."}},"verdict_id":"8028c962-b748-48d0-a34d-3b75de93bbf0"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:d89feddbee147c35cc99808b9bb3b11d692340e421d5f98e1b894ab4c93cf4c1","target":"record","created_at":"2026-05-20T00:02:36Z","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":"450fc7e282851f1f56bdb3ba66c8ffd1f9af2c9dae73b0c9422aa65aeef9a7ff","cross_cats_sorted":["cond-mat.stat-mech","math.PR","physics.bio-ph"],"license":"http://creativecommons.org/publicdomain/zero/1.0/","primary_cat":"q-bio.PE","submitted_at":"2026-05-15T23:10:35Z","title_canon_sha256":"36ebeefc4498081ef050ad27cb840693f818383619e8886e9a1e7be504ffd7c6"},"schema_version":"1.0","source":{"id":"2605.16693","kind":"arxiv","version":1}},"canonical_sha256":"2dbb412d8242f2d842278bd6952a942bcd2cfb14d9fff5f116bed3cf0218c680","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2dbb412d8242f2d842278bd6952a942bcd2cfb14d9fff5f116bed3cf0218c680","first_computed_at":"2026-05-20T00:02:36.940046Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-20T00:02:36.940046Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"VsyypkN3ZdYJ3b+R48CyJCZhwswYLgSBc8u+kzLijsuL0dtCCWTAlo+4kTt4lxe8sM+YOY0De+qx3TJnS8VXDw==","signature_status":"signed_v1","signed_at":"2026-05-20T00:02:36.940869Z","signed_message":"canonical_sha256_bytes"},"source_id":"2605.16693","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d89feddbee147c35cc99808b9bb3b11d692340e421d5f98e1b894ab4c93cf4c1","sha256:9b365845d3cad60931d3e171a5e8bcedb14f8974c0cffdc063a28cab277f9261"],"state_sha256":"89d216cf6247357f126813be1de41b51892e6a375714b36ee6bb54a5f05bbfa1"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7d4IUDWdd99N7ToxthRLs85QtQwQUE+/wAFc0yx7o0A4Gf0jWmPIawMhYFsSZhdueaMh7QY86G9hy+kkiR8tCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T09:41:49.414902Z","bundle_sha256":"fe02c5f689cb4314f2f0985c921d55238de277bc0c7ab52726b1d11175c5fb28"}}