{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:XZKSSUSDUNZ24WWO6N7SH4F6WE","short_pith_number":"pith:XZKSSUSD","canonical_record":{"source":{"id":"2605.03087","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-05-04T19:04:29Z","cross_cats_sorted":[],"title_canon_sha256":"e7f927aaa5986191c2d639ffccda5b6359a465ca9aa4fe7e1e1c1d9c7bd23aca","abstract_canon_sha256":"73e1413b54d48dbe519114bc61a50e16c65f891258386ac47411e083f33fed4b"},"schema_version":"1.0"},"canonical_sha256":"be55295243a373ae5acef37f23f0beb113268079d9acce0f896fc220aeb080f0","source":{"kind":"arxiv","id":"2605.03087","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.03087","created_at":"2026-05-20T00:00:40Z"},{"alias_kind":"arxiv_version","alias_value":"2605.03087v2","created_at":"2026-05-20T00:00:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.03087","created_at":"2026-05-20T00:00:40Z"},{"alias_kind":"pith_short_12","alias_value":"XZKSSUSDUNZ2","created_at":"2026-05-20T00:00:40Z"},{"alias_kind":"pith_short_16","alias_value":"XZKSSUSDUNZ24WWO","created_at":"2026-05-20T00:00:40Z"},{"alias_kind":"pith_short_8","alias_value":"XZKSSUSD","created_at":"2026-05-20T00:00:40Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:XZKSSUSDUNZ24WWO6N7SH4F6WE","target":"record","payload":{"canonical_record":{"source":{"id":"2605.03087","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-05-04T19:04:29Z","cross_cats_sorted":[],"title_canon_sha256":"e7f927aaa5986191c2d639ffccda5b6359a465ca9aa4fe7e1e1c1d9c7bd23aca","abstract_canon_sha256":"73e1413b54d48dbe519114bc61a50e16c65f891258386ac47411e083f33fed4b"},"schema_version":"1.0"},"canonical_sha256":"be55295243a373ae5acef37f23f0beb113268079d9acce0f896fc220aeb080f0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-20T00:00:40.504685Z","signature_b64":"Y6stcD1r8ZgkxhWtbYmeV8e5Ayw4J52CBoTeIf3SS11CWbAF/E+kLXA+Raa/SioeVK0VdZfSOLs5AnXgwYRnAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"be55295243a373ae5acef37f23f0beb113268079d9acce0f896fc220aeb080f0","last_reissued_at":"2026-05-20T00:00:40.504008Z","signature_status":"signed_v1","first_computed_at":"2026-05-20T00:00:40.504008Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2605.03087","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":"2026-05-20T00:00:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8Lc7vEQ45VPwDQUwz7f+gWSIX4Y31fWbr7lm0FfEArQRQMNsLd58krdGPENmGYb1pIpkUWgNUF+gwcKxnmh8BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T10:47:07.071945Z"},"content_sha256":"ad26ed07f0fa704fe86e780d6c07577ffff019374cf59197fcb39d6df254aad1","schema_version":"1.0","event_id":"sha256:ad26ed07f0fa704fe86e780d6c07577ffff019374cf59197fcb39d6df254aad1"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:XZKSSUSDUNZ24WWO6N7SH4F6WE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Bogoliubov mode dynamics and non-adiabatic transitions in time-varying condensed media","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"A dimensionless parameter quantifies phase-mode redistribution at sub-wavelength inhomogeneities via non-adiabatic excitations in condensed media.","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"A.M. Tishin","submitted_at":"2026-05-04T19:04:29Z","abstract_excerpt":"This study investigates non-adiabatic wave dynamics in condensed media and the transition from adiabatic stability to spectral chaos. We introduce a dimensionless parameter, as a universal metric to quantify phase-mode redistribution at sub-wavelength inhomogeneities. Our framework treats defects as localized sites of adiabaticity violation triggering non-adiabatic parametric excitation of the ground state. Numerical validation in an expanded 50-level bosonic basis demonstrates that the framework accurately distinguishes between adiabatic regimes in ENZ-metamaterials and non-adiabatic transiti"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"We establish a universal scaling law governed by the non-adiabaticity-to-regulation ratio, proving that the proposed metric remains a robust metrological tool for identifying sub-wavelength inhomogeneities across diverse material classes.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"That numerical validation in an expanded 50-level bosonic basis is sufficient to establish the universality of the metric and scaling law across all non-linear condensed media satisfying the stability criterion without significant basis truncation artifacts.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"Introduces a universal dimensionless metric for non-adiabatic phase-mode redistribution at defects in condensed media, supported by numerical simulations in a 50-level bosonic basis and a scaling law.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"A dimensionless parameter quantifies phase-mode redistribution at sub-wavelength inhomogeneities via non-adiabatic excitations in condensed media.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"5777a18f1bf02fd573ffeccfe5b494ee512b9e43fb3e0e57a70afce074b1aa97"},"source":{"id":"2605.03087","kind":"arxiv","version":2},"verdict":{"id":"24ce2b2b-7653-4f12-934b-34ca80e49eb6","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-19T16:59:10.133949Z","strongest_claim":"We establish a universal scaling law governed by the non-adiabaticity-to-regulation ratio, proving that the proposed metric remains a robust metrological tool for identifying sub-wavelength inhomogeneities across diverse material classes.","one_line_summary":"Introduces a universal dimensionless metric for non-adiabatic phase-mode redistribution at defects in condensed media, supported by numerical simulations in a 50-level bosonic basis and a scaling law.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"That numerical validation in an expanded 50-level bosonic basis is sufficient to establish the universality of the metric and scaling law across all non-linear condensed media satisfying the stability criterion without significant basis truncation artifacts.","pith_extraction_headline":"A dimensionless parameter quantifies phase-mode redistribution at sub-wavelength inhomogeneities via non-adiabatic excitations in condensed media."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2605.03087/integrity.json","findings":[],"available":true,"detectors_run":[{"name":"doi_compliance","ran_at":"2026-05-19T15:44:00.238261Z","status":"completed","version":"1.0.0","findings_count":0}],"snapshot_sha256":"590fbfbac409f52966621ddbf4a0a186e86b35ec204bfb232a82bda2f7386eb4"},"references":{"count":21,"sample":[{"doi":"10.1126/science.257.5067.189","year":1992,"title":"E. Betzig and J. K. Trautman, Near-field optics: Microscopy, spectroscopy, and surface modification. Science, 257, 5067 (1992), 189-195. DOI: 10.1126/science.257.5067.189","work_id":"b8448fe1-cb24-4a99-b149-bce05b05dc35","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":1968,"title":"V. G. Veselago, The electrodynamics of substances with simultaneously negative values of ε and μ. Soviet Physics Uspekhi ;10, 4, 509-514 (1968)","work_id":"50ea4424-8d26-4c00-af6d-b80fac9e5f23","ref_index":2,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"10.1063/1.1784272","year":2004,"title":"J. B. Pendry, D.R. Smith, Reversing light with negative refraction , Phys. Today 57, (2004) 37–43 . Doi: 10.1063/1.1784272","work_id":"7a500156-ef40-4649-960b-9c5f6e717584","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"10.1103/physrevlett.108.253901","year":2012,"title":"E. Rubino, J. McLenaghan, S.C. Kehr, F. Belgiorno, D. Townsend, S. Rohr, C.E. Kuklewicz, U. Leonhardt, F. Konig, Negative-Frequency Resonant Radiation Phys. Rev. Lett. 108 (2012) 253901 https://doi.or","work_id":"dda12f43-d97f-44f2-8389-c02655e819a5","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2011,"title":"Measurement of stimulated Hawking emission in an analogue system","work_id":"7d7d3548-f3d8-46a8-9669-11eece9cebae","ref_index":5,"cited_arxiv_id":"1008.1911","is_internal_anchor":true}],"resolved_work":21,"snapshot_sha256":"31cf8f44cc860eba03bce6fe598e194527ae8f6ab0b9cc6f56d3c2346fd5540d","internal_anchors":6},"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":"24ce2b2b-7653-4f12-934b-34ca80e49eb6"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-20T00:00:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CnxOjcb+tqRm+U8rG7UHzwwVmA7Wu/6T2tNQGtOyJeFNh5GT2GCzD2Fpq3TCcruvOaycPzWqkdYaylxatmGbBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T10:47:07.072906Z"},"content_sha256":"f8b85a8da456d846725eae7e116888e1b339076f311ab75cc745340275bc8512","schema_version":"1.0","event_id":"sha256:f8b85a8da456d846725eae7e116888e1b339076f311ab75cc745340275bc8512"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XZKSSUSDUNZ24WWO6N7SH4F6WE/bundle.json","state_url":"https://pith.science/pith/XZKSSUSDUNZ24WWO6N7SH4F6WE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XZKSSUSDUNZ24WWO6N7SH4F6WE/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":"2026-05-23T10:47:07Z","links":{"resolver":"https://pith.science/pith/XZKSSUSDUNZ24WWO6N7SH4F6WE","bundle":"https://pith.science/pith/XZKSSUSDUNZ24WWO6N7SH4F6WE/bundle.json","state":"https://pith.science/pith/XZKSSUSDUNZ24WWO6N7SH4F6WE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XZKSSUSDUNZ24WWO6N7SH4F6WE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:XZKSSUSDUNZ24WWO6N7SH4F6WE","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":"73e1413b54d48dbe519114bc61a50e16c65f891258386ac47411e083f33fed4b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-05-04T19:04:29Z","title_canon_sha256":"e7f927aaa5986191c2d639ffccda5b6359a465ca9aa4fe7e1e1c1d9c7bd23aca"},"schema_version":"1.0","source":{"id":"2605.03087","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.03087","created_at":"2026-05-20T00:00:40Z"},{"alias_kind":"arxiv_version","alias_value":"2605.03087v2","created_at":"2026-05-20T00:00:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.03087","created_at":"2026-05-20T00:00:40Z"},{"alias_kind":"pith_short_12","alias_value":"XZKSSUSDUNZ2","created_at":"2026-05-20T00:00:40Z"},{"alias_kind":"pith_short_16","alias_value":"XZKSSUSDUNZ24WWO","created_at":"2026-05-20T00:00:40Z"},{"alias_kind":"pith_short_8","alias_value":"XZKSSUSD","created_at":"2026-05-20T00:00:40Z"}],"graph_snapshots":[{"event_id":"sha256:f8b85a8da456d846725eae7e116888e1b339076f311ab75cc745340275bc8512","target":"graph","created_at":"2026-05-20T00:00:40Z","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":"We establish a universal scaling law governed by the non-adiabaticity-to-regulation ratio, proving that the proposed metric remains a robust metrological tool for identifying sub-wavelength inhomogeneities across diverse material classes."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"That numerical validation in an expanded 50-level bosonic basis is sufficient to establish the universality of the metric and scaling law across all non-linear condensed media satisfying the stability criterion without significant basis truncation artifacts."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"Introduces a universal dimensionless metric for non-adiabatic phase-mode redistribution at defects in condensed media, supported by numerical simulations in a 50-level bosonic basis and a scaling law."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"A dimensionless parameter quantifies phase-mode redistribution at sub-wavelength inhomogeneities via non-adiabatic excitations in condensed media."}],"snapshot_sha256":"5777a18f1bf02fd573ffeccfe5b494ee512b9e43fb3e0e57a70afce074b1aa97"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[{"findings_count":0,"name":"doi_compliance","ran_at":"2026-05-19T15:44:00.238261Z","status":"completed","version":"1.0.0"}],"endpoint":"/pith/2605.03087/integrity.json","findings":[],"snapshot_sha256":"590fbfbac409f52966621ddbf4a0a186e86b35ec204bfb232a82bda2f7386eb4","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"This study investigates non-adiabatic wave dynamics in condensed media and the transition from adiabatic stability to spectral chaos. We introduce a dimensionless parameter, as a universal metric to quantify phase-mode redistribution at sub-wavelength inhomogeneities. Our framework treats defects as localized sites of adiabaticity violation triggering non-adiabatic parametric excitation of the ground state. Numerical validation in an expanded 50-level bosonic basis demonstrates that the framework accurately distinguishes between adiabatic regimes in ENZ-metamaterials and non-adiabatic transiti","authors_text":"A.M. Tishin","cross_cats":[],"headline":"A dimensionless parameter quantifies phase-mode redistribution at sub-wavelength inhomogeneities via non-adiabatic excitations in condensed media.","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-05-04T19:04:29Z","title":"Bogoliubov mode dynamics and non-adiabatic transitions in time-varying condensed media"},"references":{"count":21,"internal_anchors":6,"resolved_work":21,"sample":[{"cited_arxiv_id":"","doi":"10.1126/science.257.5067.189","is_internal_anchor":false,"ref_index":1,"title":"E. Betzig and J. K. Trautman, Near-field optics: Microscopy, spectroscopy, and surface modification. Science, 257, 5067 (1992), 189-195. DOI: 10.1126/science.257.5067.189","work_id":"b8448fe1-cb24-4a99-b149-bce05b05dc35","year":1992},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":2,"title":"V. G. Veselago, The electrodynamics of substances with simultaneously negative values of ε and μ. Soviet Physics Uspekhi ;10, 4, 509-514 (1968)","work_id":"50ea4424-8d26-4c00-af6d-b80fac9e5f23","year":1968},{"cited_arxiv_id":"","doi":"10.1063/1.1784272","is_internal_anchor":false,"ref_index":3,"title":"J. B. Pendry, D.R. Smith, Reversing light with negative refraction , Phys. Today 57, (2004) 37–43 . Doi: 10.1063/1.1784272","work_id":"7a500156-ef40-4649-960b-9c5f6e717584","year":2004},{"cited_arxiv_id":"","doi":"10.1103/physrevlett.108.253901","is_internal_anchor":false,"ref_index":4,"title":"E. Rubino, J. McLenaghan, S.C. Kehr, F. Belgiorno, D. Townsend, S. Rohr, C.E. Kuklewicz, U. Leonhardt, F. Konig, Negative-Frequency Resonant Radiation Phys. Rev. Lett. 108 (2012) 253901 https://doi.or","work_id":"dda12f43-d97f-44f2-8389-c02655e819a5","year":2012},{"cited_arxiv_id":"1008.1911","doi":"","is_internal_anchor":true,"ref_index":5,"title":"Measurement of stimulated Hawking emission in an analogue system","work_id":"7d7d3548-f3d8-46a8-9669-11eece9cebae","year":2011}],"snapshot_sha256":"31cf8f44cc860eba03bce6fe598e194527ae8f6ab0b9cc6f56d3c2346fd5540d"},"source":{"id":"2605.03087","kind":"arxiv","version":2},"verdict":{"created_at":"2026-05-19T16:59:10.133949Z","id":"24ce2b2b-7653-4f12-934b-34ca80e49eb6","model_set":{"reader":"grok-4.3"},"one_line_summary":"Introduces a universal dimensionless metric for non-adiabatic phase-mode redistribution at defects in condensed media, supported by numerical simulations in a 50-level bosonic basis and a scaling law.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"A dimensionless parameter quantifies phase-mode redistribution at sub-wavelength inhomogeneities via non-adiabatic excitations in condensed media.","strongest_claim":"We establish a universal scaling law governed by the non-adiabaticity-to-regulation ratio, proving that the proposed metric remains a robust metrological tool for identifying sub-wavelength inhomogeneities across diverse material classes.","weakest_assumption":"That numerical validation in an expanded 50-level bosonic basis is sufficient to establish the universality of the metric and scaling law across all non-linear condensed media satisfying the stability criterion without significant basis truncation artifacts."}},"verdict_id":"24ce2b2b-7653-4f12-934b-34ca80e49eb6"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:ad26ed07f0fa704fe86e780d6c07577ffff019374cf59197fcb39d6df254aad1","target":"record","created_at":"2026-05-20T00:00:40Z","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":"73e1413b54d48dbe519114bc61a50e16c65f891258386ac47411e083f33fed4b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-05-04T19:04:29Z","title_canon_sha256":"e7f927aaa5986191c2d639ffccda5b6359a465ca9aa4fe7e1e1c1d9c7bd23aca"},"schema_version":"1.0","source":{"id":"2605.03087","kind":"arxiv","version":2}},"canonical_sha256":"be55295243a373ae5acef37f23f0beb113268079d9acce0f896fc220aeb080f0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"be55295243a373ae5acef37f23f0beb113268079d9acce0f896fc220aeb080f0","first_computed_at":"2026-05-20T00:00:40.504008Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-20T00:00:40.504008Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Y6stcD1r8ZgkxhWtbYmeV8e5Ayw4J52CBoTeIf3SS11CWbAF/E+kLXA+Raa/SioeVK0VdZfSOLs5AnXgwYRnAA==","signature_status":"signed_v1","signed_at":"2026-05-20T00:00:40.504685Z","signed_message":"canonical_sha256_bytes"},"source_id":"2605.03087","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ad26ed07f0fa704fe86e780d6c07577ffff019374cf59197fcb39d6df254aad1","sha256:f8b85a8da456d846725eae7e116888e1b339076f311ab75cc745340275bc8512"],"state_sha256":"0a6a5d90fbac5648d6ec6820748fe2b7f383b484c2e416f13310fc0e01ead19c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZL094xTq37dEIRVlaLmOAudp8gy2Y7pQwBSDYCkfDkPrBnVdE/t1vtWQfQNC5PbpHjGY07xH8i/y78I36tqkCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-23T10:47:07.076577Z","bundle_sha256":"fbc439cb8710e119933e174487459f7d1a5b0d60c78749283cf7942472b1a31a"}}