{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:YPMXU3XO74DJAQWAFB4LB2F4DG","short_pith_number":"pith:YPMXU3XO","canonical_record":{"source":{"id":"2512.18472","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-12-20T19:11:30Z","cross_cats_sorted":[],"title_canon_sha256":"470e8d7daf7449464e813072cdee1cd8d3eb93f44e77ca550a45e0c07fb1b30c","abstract_canon_sha256":"a732b1f750256114582803f923857f2ba7b57058487e8119696d2eb689d6559b"},"schema_version":"1.0"},"canonical_sha256":"c3d97a6eeeff069042c02878b0e8bc19915959065c051bfde81caaa8df20e0e3","source":{"kind":"arxiv","id":"2512.18472","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2512.18472","created_at":"2026-06-02T03:04:36Z"},{"alias_kind":"arxiv_version","alias_value":"2512.18472v2","created_at":"2026-06-02T03:04:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2512.18472","created_at":"2026-06-02T03:04:36Z"},{"alias_kind":"pith_short_12","alias_value":"YPMXU3XO74DJ","created_at":"2026-06-02T03:04:36Z"},{"alias_kind":"pith_short_16","alias_value":"YPMXU3XO74DJAQWA","created_at":"2026-06-02T03:04:36Z"},{"alias_kind":"pith_short_8","alias_value":"YPMXU3XO","created_at":"2026-06-02T03:04:36Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:YPMXU3XO74DJAQWAFB4LB2F4DG","target":"record","payload":{"canonical_record":{"source":{"id":"2512.18472","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-12-20T19:11:30Z","cross_cats_sorted":[],"title_canon_sha256":"470e8d7daf7449464e813072cdee1cd8d3eb93f44e77ca550a45e0c07fb1b30c","abstract_canon_sha256":"a732b1f750256114582803f923857f2ba7b57058487e8119696d2eb689d6559b"},"schema_version":"1.0"},"canonical_sha256":"c3d97a6eeeff069042c02878b0e8bc19915959065c051bfde81caaa8df20e0e3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-02T03:04:36.582861Z","signature_b64":"Km+sTlUAZw0twtnVt9czDo4xDz8VFgDVkL3o9vHsjb4zzV6MBu6yabOhgahKn/CL4P02NpnX5fNpUcPZZ/3oBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c3d97a6eeeff069042c02878b0e8bc19915959065c051bfde81caaa8df20e0e3","last_reissued_at":"2026-06-02T03:04:36.582331Z","signature_status":"signed_v1","first_computed_at":"2026-06-02T03:04:36.582331Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2512.18472","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":"2026-06-02T03:04:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MVy0a4WT4a4IT/sWJ3I4+MX+K0B2myAd0s29qjpjUBGHlXCoUfat/8eVz+qz3FcdaziP8QTskTWRXdTla5dtCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T13:10:13.359720Z"},"content_sha256":"ecc0a037a70873ada3d7c750eed6d453d620c658db0fb8931a3c8ec306f9c264","schema_version":"1.0","event_id":"sha256:ecc0a037a70873ada3d7c750eed6d453d620c658db0fb8931a3c8ec306f9c264"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:YPMXU3XO74DJAQWAFB4LB2F4DG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Evolution of charge-density-wave soft phonon modes in $\\mathrm{Pd}_x\\mathrm{ErTe}_3$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"Intercalating palladium into ErTe3 fully suppresses the a-CDW order while residual diffuse scattering at the a-wavevector arises from c-CDW phonon softening.","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Ahmet Alatas, Anisha G. Singh, Avishek Maity, Ayman H. Said, Frank Weber, Ian R. Fisher, Joshua A. W. Straquadine, Matthew J. Krogstad, Raymond Osborn, Rolf Heid, Stephan Rosenkranz","submitted_at":"2025-12-20T19:11:30Z","abstract_excerpt":"We investigated the lattice dynamics of quasi-two-dimensional Pd-intercalated $\\mathrm{ErTe}_3$ in relation to its charge-density-wave (CDW) transitions by means of x-ray diffuse and meV-resolution inelastic x-ray scattering. In pristine $\\mathrm{ErTe}_3$, CDW order develops at orthogonal in-plane wave vectors $\\boldsymbol{\\mathrm{q}}_{1}^{c} = (0, 0, 0.29)$ (the $c\\text{-}\\mathrm{CDW}$) and $\\boldsymbol{\\mathrm{q}}_{2}^{a} = (0.31, 0, 0)$ (the $a\\text{-}\\mathrm{CDW}$), with transition temperatures $T_{1}^{c} = 270$ K and $T_{2}^{a} = 160$ K, respectively. Remarkably, we observe diffuse x-ray "},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"These findings suggest that the a-CDW is fully suppressed for x ≥ 0.02, and that the residual diffuse scattering at q1^a originates from the partial phonon softening associated with the c-CDW, reflected by the near equality of the absolute size of q1^c and q1^a.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"That the near equality of the absolute magnitudes of q1^c and q1^a is sufficient to attribute all residual diffuse scattering at q1^a to c-CDW phonon softening rather than incomplete suppression or other scattering contributions.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"Pd intercalation above x=0.02 suppresses the a-CDW in ErTe3, with residual diffuse scattering at q=(0.29,0,0) arising from partial phonon softening of the c-CDW due to nearly equal wave-vector magnitudes.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"Intercalating palladium into ErTe3 fully suppresses the a-CDW order while residual diffuse scattering at the a-wavevector arises from c-CDW phonon softening.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"774226d804004af9f15e3756be83ea38c5297488b66f2f8ed6085712f6abdda6"},"source":{"id":"2512.18472","kind":"arxiv","version":2},"verdict":{"id":"532b54df-445b-4c22-9e27-f909ae285706","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-16T20:18:32.487627Z","strongest_claim":"These findings suggest that the a-CDW is fully suppressed for x ≥ 0.02, and that the residual diffuse scattering at q1^a originates from the partial phonon softening associated with the c-CDW, reflected by the near equality of the absolute size of q1^c and q1^a.","one_line_summary":"Pd intercalation above x=0.02 suppresses the a-CDW in ErTe3, with residual diffuse scattering at q=(0.29,0,0) arising from partial phonon softening of the c-CDW due to nearly equal wave-vector magnitudes.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"That the near equality of the absolute magnitudes of q1^c and q1^a is sufficient to attribute all residual diffuse scattering at q1^a to c-CDW phonon softening rather than incomplete suppression or other scattering contributions.","pith_extraction_headline":"Intercalating palladium into ErTe3 fully suppresses the a-CDW order while residual diffuse scattering at the a-wavevector arises from c-CDW phonon softening."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2512.18472/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":60,"sample":[{"doi":"","year":2025,"title":"Evolution of charge-density-wave soft phonon modes in $\\mathrm{Pd}_x\\mathrm{ErTe}_3$","work_id":"200f46e1-22f6-4f9b-88c4-4132776b3de4","ref_index":1,"cited_arxiv_id":"2512.18472","is_internal_anchor":true},{"doi":"","year":null,"title":"Furthermore, our results from phonon spectroscopy show that the XDS alonga ∗ in PdxErTe3 is related to a competing soft phonon mode and unrelated to thea-CDW present at low intercalation levels. II. E","work_id":"562ff2d5-c5c6-4e21-a160-f82239d673c9","ref_index":2,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":null,"title":"1(d)] andq a 2 = (0.31,0,0) [marked by the white boxes in Fig","work_id":"a105eb18-c7d6-4906-9e84-896b97a77727","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":null,"title":"Background scattering [Qarea indicated by red boxes in Fig","work_id":"c16591f9-dcc0-4360-a837-8ee6860a70a9","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":null,"title":"3(a) and 3(b)] and 0.023 [Figs","work_id":"2972a8ac-2375-4b23-9bef-db6e67e1c9fd","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":60,"snapshot_sha256":"739214dc337afc513f659c7b8963aabb6d29969c993888f96e1759024d0b533d","internal_anchors":1},"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":"532b54df-445b-4c22-9e27-f909ae285706"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-06-02T03:04:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6QrRtEZbm0Kbu1WrzOJa6S19jadgMRKSuQusxcsIC9YbQCB9nrj56ua8e0+9Ocyv5j9A+Brq7zLivZ8DWkjPDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T13:10:13.360331Z"},"content_sha256":"a8c0ed649fce9af91348765a92ef9216524c6051fce5c179fae0297bb423cb1d","schema_version":"1.0","event_id":"sha256:a8c0ed649fce9af91348765a92ef9216524c6051fce5c179fae0297bb423cb1d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YPMXU3XO74DJAQWAFB4LB2F4DG/bundle.json","state_url":"https://pith.science/pith/YPMXU3XO74DJAQWAFB4LB2F4DG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YPMXU3XO74DJAQWAFB4LB2F4DG/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":"2026-06-02T13:10:13Z","links":{"resolver":"https://pith.science/pith/YPMXU3XO74DJAQWAFB4LB2F4DG","bundle":"https://pith.science/pith/YPMXU3XO74DJAQWAFB4LB2F4DG/bundle.json","state":"https://pith.science/pith/YPMXU3XO74DJAQWAFB4LB2F4DG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YPMXU3XO74DJAQWAFB4LB2F4DG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:YPMXU3XO74DJAQWAFB4LB2F4DG","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":"a732b1f750256114582803f923857f2ba7b57058487e8119696d2eb689d6559b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-12-20T19:11:30Z","title_canon_sha256":"470e8d7daf7449464e813072cdee1cd8d3eb93f44e77ca550a45e0c07fb1b30c"},"schema_version":"1.0","source":{"id":"2512.18472","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2512.18472","created_at":"2026-06-02T03:04:36Z"},{"alias_kind":"arxiv_version","alias_value":"2512.18472v2","created_at":"2026-06-02T03:04:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2512.18472","created_at":"2026-06-02T03:04:36Z"},{"alias_kind":"pith_short_12","alias_value":"YPMXU3XO74DJ","created_at":"2026-06-02T03:04:36Z"},{"alias_kind":"pith_short_16","alias_value":"YPMXU3XO74DJAQWA","created_at":"2026-06-02T03:04:36Z"},{"alias_kind":"pith_short_8","alias_value":"YPMXU3XO","created_at":"2026-06-02T03:04:36Z"}],"graph_snapshots":[{"event_id":"sha256:a8c0ed649fce9af91348765a92ef9216524c6051fce5c179fae0297bb423cb1d","target":"graph","created_at":"2026-06-02T03:04:36Z","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":"These findings suggest that the a-CDW is fully suppressed for x ≥ 0.02, and that the residual diffuse scattering at q1^a originates from the partial phonon softening associated with the c-CDW, reflected by the near equality of the absolute size of q1^c and q1^a."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"That the near equality of the absolute magnitudes of q1^c and q1^a is sufficient to attribute all residual diffuse scattering at q1^a to c-CDW phonon softening rather than incomplete suppression or other scattering contributions."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"Pd intercalation above x=0.02 suppresses the a-CDW in ErTe3, with residual diffuse scattering at q=(0.29,0,0) arising from partial phonon softening of the c-CDW due to nearly equal wave-vector magnitudes."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"Intercalating palladium into ErTe3 fully suppresses the a-CDW order while residual diffuse scattering at the a-wavevector arises from c-CDW phonon softening."}],"snapshot_sha256":"774226d804004af9f15e3756be83ea38c5297488b66f2f8ed6085712f6abdda6"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2512.18472/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We investigated the lattice dynamics of quasi-two-dimensional Pd-intercalated $\\mathrm{ErTe}_3$ in relation to its charge-density-wave (CDW) transitions by means of x-ray diffuse and meV-resolution inelastic x-ray scattering. In pristine $\\mathrm{ErTe}_3$, CDW order develops at orthogonal in-plane wave vectors $\\boldsymbol{\\mathrm{q}}_{1}^{c} = (0, 0, 0.29)$ (the $c\\text{-}\\mathrm{CDW}$) and $\\boldsymbol{\\mathrm{q}}_{2}^{a} = (0.31, 0, 0)$ (the $a\\text{-}\\mathrm{CDW}$), with transition temperatures $T_{1}^{c} = 270$ K and $T_{2}^{a} = 160$ K, respectively. Remarkably, we observe diffuse x-ray ","authors_text":"Ahmet Alatas, Anisha G. Singh, Avishek Maity, Ayman H. Said, Frank Weber, Ian R. Fisher, Joshua A. W. Straquadine, Matthew J. Krogstad, Raymond Osborn, Rolf Heid, Stephan Rosenkranz","cross_cats":[],"headline":"Intercalating palladium into ErTe3 fully suppresses the a-CDW order while residual diffuse scattering at the a-wavevector arises from c-CDW phonon softening.","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-12-20T19:11:30Z","title":"Evolution of charge-density-wave soft phonon modes in $\\mathrm{Pd}_x\\mathrm{ErTe}_3$"},"references":{"count":60,"internal_anchors":1,"resolved_work":60,"sample":[{"cited_arxiv_id":"2512.18472","doi":"","is_internal_anchor":true,"ref_index":1,"title":"Evolution of charge-density-wave soft phonon modes in $\\mathrm{Pd}_x\\mathrm{ErTe}_3$","work_id":"200f46e1-22f6-4f9b-88c4-4132776b3de4","year":2025},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":2,"title":"Furthermore, our results from phonon spectroscopy show that the XDS alonga ∗ in PdxErTe3 is related to a competing soft phonon mode and unrelated to thea-CDW present at low intercalation levels. II. E","work_id":"562ff2d5-c5c6-4e21-a160-f82239d673c9","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":3,"title":"1(d)] andq a 2 = (0.31,0,0) [marked by the white boxes in Fig","work_id":"a105eb18-c7d6-4906-9e84-896b97a77727","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":4,"title":"Background scattering [Qarea indicated by red boxes in Fig","work_id":"c16591f9-dcc0-4360-a837-8ee6860a70a9","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":5,"title":"3(a) and 3(b)] and 0.023 [Figs","work_id":"2972a8ac-2375-4b23-9bef-db6e67e1c9fd","year":null}],"snapshot_sha256":"739214dc337afc513f659c7b8963aabb6d29969c993888f96e1759024d0b533d"},"source":{"id":"2512.18472","kind":"arxiv","version":2},"verdict":{"created_at":"2026-05-16T20:18:32.487627Z","id":"532b54df-445b-4c22-9e27-f909ae285706","model_set":{"reader":"grok-4.3"},"one_line_summary":"Pd intercalation above x=0.02 suppresses the a-CDW in ErTe3, with residual diffuse scattering at q=(0.29,0,0) arising from partial phonon softening of the c-CDW due to nearly equal wave-vector magnitudes.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"Intercalating palladium into ErTe3 fully suppresses the a-CDW order while residual diffuse scattering at the a-wavevector arises from c-CDW phonon softening.","strongest_claim":"These findings suggest that the a-CDW is fully suppressed for x ≥ 0.02, and that the residual diffuse scattering at q1^a originates from the partial phonon softening associated with the c-CDW, reflected by the near equality of the absolute size of q1^c and q1^a.","weakest_assumption":"That the near equality of the absolute magnitudes of q1^c and q1^a is sufficient to attribute all residual diffuse scattering at q1^a to c-CDW phonon softening rather than incomplete suppression or other scattering contributions."}},"verdict_id":"532b54df-445b-4c22-9e27-f909ae285706"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:ecc0a037a70873ada3d7c750eed6d453d620c658db0fb8931a3c8ec306f9c264","target":"record","created_at":"2026-06-02T03:04:36Z","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":"a732b1f750256114582803f923857f2ba7b57058487e8119696d2eb689d6559b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-12-20T19:11:30Z","title_canon_sha256":"470e8d7daf7449464e813072cdee1cd8d3eb93f44e77ca550a45e0c07fb1b30c"},"schema_version":"1.0","source":{"id":"2512.18472","kind":"arxiv","version":2}},"canonical_sha256":"c3d97a6eeeff069042c02878b0e8bc19915959065c051bfde81caaa8df20e0e3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c3d97a6eeeff069042c02878b0e8bc19915959065c051bfde81caaa8df20e0e3","first_computed_at":"2026-06-02T03:04:36.582331Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-02T03:04:36.582331Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Km+sTlUAZw0twtnVt9czDo4xDz8VFgDVkL3o9vHsjb4zzV6MBu6yabOhgahKn/CL4P02NpnX5fNpUcPZZ/3oBQ==","signature_status":"signed_v1","signed_at":"2026-06-02T03:04:36.582861Z","signed_message":"canonical_sha256_bytes"},"source_id":"2512.18472","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ecc0a037a70873ada3d7c750eed6d453d620c658db0fb8931a3c8ec306f9c264","sha256:a8c0ed649fce9af91348765a92ef9216524c6051fce5c179fae0297bb423cb1d"],"state_sha256":"7d2ecef328dd5778eea39f5884ac79373111306ee23d83aad3af64ca7bc7c0ac"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oUvUTfTIm8/rvW12M4f629vIqLgbOewGgtOpxgeLgRzHRGe1dk1YJk/benwcHJvLpTYWuMbMb5ZWqVTm5OpaBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T13:10:13.362750Z","bundle_sha256":"9f5f166c49391d44b32322ff2776834a2425bf87a35b4844ff1081e96100b10c"}}