{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:HFFQV6EJPVZNGHC7I4Z6GJXUS7","short_pith_number":"pith:HFFQV6EJ","canonical_record":{"source":{"id":"2605.13934","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2026-05-13T16:12:38Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"00dcea7e59ca2efbabe8a33cd0b3e771d7fe35fcaed084ce1d9f412706846b44","abstract_canon_sha256":"e9e57fd2fc712c6d870fa94b9d0ef12628e048c8a499d9f663968ed645e9ba03"},"schema_version":"1.0"},"canonical_sha256":"394b0af8897d72d31c5f4733e326f497c1c882dfae93258962ffcc22babf4088","source":{"kind":"arxiv","id":"2605.13934","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.13934","created_at":"2026-05-17T23:39:13Z"},{"alias_kind":"arxiv_version","alias_value":"2605.13934v1","created_at":"2026-05-17T23:39:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.13934","created_at":"2026-05-17T23:39:13Z"},{"alias_kind":"pith_short_12","alias_value":"HFFQV6EJPVZN","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_16","alias_value":"HFFQV6EJPVZNGHC7","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_8","alias_value":"HFFQV6EJ","created_at":"2026-05-18T12:33:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:HFFQV6EJPVZNGHC7I4Z6GJXUS7","target":"record","payload":{"canonical_record":{"source":{"id":"2605.13934","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2026-05-13T16:12:38Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"00dcea7e59ca2efbabe8a33cd0b3e771d7fe35fcaed084ce1d9f412706846b44","abstract_canon_sha256":"e9e57fd2fc712c6d870fa94b9d0ef12628e048c8a499d9f663968ed645e9ba03"},"schema_version":"1.0"},"canonical_sha256":"394b0af8897d72d31c5f4733e326f497c1c882dfae93258962ffcc22babf4088","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:39:13.946847Z","signature_b64":"djGmhhO7lMSEwQM6cd3ycKKz8bg2K6w48/GYvu8o0dHpCHcNb6HkPav07DMKxjFEumQiR/bJUcMaJHA+V40SCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"394b0af8897d72d31c5f4733e326f497c1c882dfae93258962ffcc22babf4088","last_reissued_at":"2026-05-17T23:39:13.946096Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:39:13.946096Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2605.13934","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":"2026-05-17T23:39:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"g06mboBML0elus1KCp5XeFjTrSlMTvq/qP6knV24F5o07h261o+WbHEDSLz5xM+XE4zW2qToOkSe5SASxfvdBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T04:47:48.653588Z"},"content_sha256":"2c715ae5a3db91f0945d7ba334d7170a138b897133146817238b626e8b896a9d","schema_version":"1.0","event_id":"sha256:2c715ae5a3db91f0945d7ba334d7170a138b897133146817238b626e8b896a9d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:HFFQV6EJPVZNGHC7I4Z6GJXUS7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Diquark Correlators and Phase Structure in the Quark-Meson-Diquark Model beyond Mean Field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"Mesonic fluctuations beyond mean field substantially modify the phase structure of the two-flavor quark-meson-diquark model and allow diquark condensation to dominate at strong couplings.","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Mire Ugo, Schaefer Bernd-Jochen","submitted_at":"2026-05-13T16:12:38Z","abstract_excerpt":"A comprehensive study of the phase structure of the two-flavor quark-meson-diquark model is presented within the nonperturbative functional renormalization group framework. The influence of mesonic fluctuations beyond the mean-field approximation is investigated, and two-point functions of the diquark fields are computed at finite real-time frequencies. Renormalization group consistency of the effective potential is ensured in order to avoid cutoff artifacts. Substantial modifications of the phase structure are found once mesonic fluctuations are included, and for sufficiently strong diquark c"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"Substantial modifications of the phase structure are found once mesonic fluctuations are included, and for sufficiently strong diquark couplings the dynamics become dominated by diquark condensation. These effects are elucidated through an analysis of the diquark pole mass and the Silver-Blaze property.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"The quark-meson-diquark model with the chosen FRG truncation accurately captures the relevant non-perturbative QCD dynamics at finite density, and that ensuring RG consistency of the effective potential fully eliminates cutoff artifacts.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"Including mesonic fluctuations beyond mean field substantially modifies the phase structure of the quark-meson-diquark model, with diquark condensation dominating for strong couplings as analyzed via diquark pole mass and the Silver-Blaze property.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"Mesonic fluctuations beyond mean field substantially modify the phase structure of the two-flavor quark-meson-diquark model and allow diquark condensation to dominate at strong couplings.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"82f24b5f11e6073e95448914f0b0125bf751f57aa1b3233fef87dd82825f2237"},"source":{"id":"2605.13934","kind":"arxiv","version":1},"verdict":{"id":"1fc38a3c-2be3-4d5c-aaea-b74a19654b3d","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-15T02:50:28.985098Z","strongest_claim":"Substantial modifications of the phase structure are found once mesonic fluctuations are included, and for sufficiently strong diquark couplings the dynamics become dominated by diquark condensation. These effects are elucidated through an analysis of the diquark pole mass and the Silver-Blaze property.","one_line_summary":"Including mesonic fluctuations beyond mean field substantially modifies the phase structure of the quark-meson-diquark model, with diquark condensation dominating for strong couplings as analyzed via diquark pole mass and the Silver-Blaze property.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"The quark-meson-diquark model with the chosen FRG truncation accurately captures the relevant non-perturbative QCD dynamics at finite density, and that ensuring RG consistency of the effective potential fully eliminates cutoff artifacts.","pith_extraction_headline":"Mesonic fluctuations beyond mean field substantially modify the phase structure of the two-flavor quark-meson-diquark model and allow diquark condensation to dominate at strong couplings."},"references":{"count":113,"sample":[{"doi":"","year":null,"title":"(38) simplifies to ∂tUk(σ,∆) = k5 12π2 3 ϵπ + 1 ϵσ − 4Nf ϵq θ(ϵ− q ) + ϵ+ q E+q + ϵ− q E−q","work_id":"f7216f1f-55df-428b-b9cd-c05706be98ba","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":null,"title":"Quark-meson flows For ∆ = 0 and finite temperature, the quasi-particle energies reduce to E+ q →ϵ + q andE − q → |ϵ − q |.(44) Consequently, the flow converges to that of a quark- meson flow withN c =","work_id":"bfd2cd6c-37f3-4a70-91c9-d73092a71b82","ref_index":2,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":null,"title":"In principle, the corresponding RGC initial condition follows directly from the definition of the scale-dependent mean-field potential in Eq","work_id":"9879e45b-dfb2-4bab-a5b5-b770612da9a5","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":null,"title":"Mathematically, RG flows form a semi-group rather than a group: the coarse-graining from the UV to the IR is irreversible and no inverse trans- formation exists","work_id":"abbeb01c-2d20-4d24-938a-b40b8b435400","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":null,"title":"Back-bending of the chiral transition line in mLPA The characteristic back-bending of the chiral transi- tion line at decreasingT(Fig. 3, right panels) has also been observed in other low-energy effec","work_id":"35151ce2-d779-43ec-a760-772e8ed6abe1","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":113,"snapshot_sha256":"4354bc6203548f096d94ed420aab64294bd98f368fda2d6241a9f0dc87ac3949","internal_anchors":45},"formal_canon":{"evidence_count":1,"snapshot_sha256":"fcc4a97b6b5b7c6b1ce68500ae093a710d4a3e8f508760e66d9870e3f853425c"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":"1fc38a3c-2be3-4d5c-aaea-b74a19654b3d"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:39:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PmymVfVSRd9YqE0e3YP0lQO8qig/hJpDCKFrOeVWGHFjNdZOCljvN6xBFt7LmNjgkKZOMbUNd1F5sn9vJH8eCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T04:47:48.654181Z"},"content_sha256":"27ff7fb6a50f25a4e7adda779cebb201803d59833b23946fb038c3e4b66b5dba","schema_version":"1.0","event_id":"sha256:27ff7fb6a50f25a4e7adda779cebb201803d59833b23946fb038c3e4b66b5dba"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HFFQV6EJPVZNGHC7I4Z6GJXUS7/bundle.json","state_url":"https://pith.science/pith/HFFQV6EJPVZNGHC7I4Z6GJXUS7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HFFQV6EJPVZNGHC7I4Z6GJXUS7/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":"2026-06-27T04:47:48Z","links":{"resolver":"https://pith.science/pith/HFFQV6EJPVZNGHC7I4Z6GJXUS7","bundle":"https://pith.science/pith/HFFQV6EJPVZNGHC7I4Z6GJXUS7/bundle.json","state":"https://pith.science/pith/HFFQV6EJPVZNGHC7I4Z6GJXUS7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HFFQV6EJPVZNGHC7I4Z6GJXUS7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:HFFQV6EJPVZNGHC7I4Z6GJXUS7","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":"e9e57fd2fc712c6d870fa94b9d0ef12628e048c8a499d9f663968ed645e9ba03","cross_cats_sorted":["hep-th","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2026-05-13T16:12:38Z","title_canon_sha256":"00dcea7e59ca2efbabe8a33cd0b3e771d7fe35fcaed084ce1d9f412706846b44"},"schema_version":"1.0","source":{"id":"2605.13934","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.13934","created_at":"2026-05-17T23:39:13Z"},{"alias_kind":"arxiv_version","alias_value":"2605.13934v1","created_at":"2026-05-17T23:39:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.13934","created_at":"2026-05-17T23:39:13Z"},{"alias_kind":"pith_short_12","alias_value":"HFFQV6EJPVZN","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_16","alias_value":"HFFQV6EJPVZNGHC7","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_8","alias_value":"HFFQV6EJ","created_at":"2026-05-18T12:33:37Z"}],"graph_snapshots":[{"event_id":"sha256:27ff7fb6a50f25a4e7adda779cebb201803d59833b23946fb038c3e4b66b5dba","target":"graph","created_at":"2026-05-17T23:39:13Z","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":"Substantial modifications of the phase structure are found once mesonic fluctuations are included, and for sufficiently strong diquark couplings the dynamics become dominated by diquark condensation. These effects are elucidated through an analysis of the diquark pole mass and the Silver-Blaze property."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"The quark-meson-diquark model with the chosen FRG truncation accurately captures the relevant non-perturbative QCD dynamics at finite density, and that ensuring RG consistency of the effective potential fully eliminates cutoff artifacts."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"Including mesonic fluctuations beyond mean field substantially modifies the phase structure of the quark-meson-diquark model, with diquark condensation dominating for strong couplings as analyzed via diquark pole mass and the Silver-Blaze property."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"Mesonic fluctuations beyond mean field substantially modify the phase structure of the two-flavor quark-meson-diquark model and allow diquark condensation to dominate at strong couplings."}],"snapshot_sha256":"82f24b5f11e6073e95448914f0b0125bf751f57aa1b3233fef87dd82825f2237"},"formal_canon":{"evidence_count":1,"snapshot_sha256":"fcc4a97b6b5b7c6b1ce68500ae093a710d4a3e8f508760e66d9870e3f853425c"},"paper":{"abstract_excerpt":"A comprehensive study of the phase structure of the two-flavor quark-meson-diquark model is presented within the nonperturbative functional renormalization group framework. The influence of mesonic fluctuations beyond the mean-field approximation is investigated, and two-point functions of the diquark fields are computed at finite real-time frequencies. Renormalization group consistency of the effective potential is ensured in order to avoid cutoff artifacts. Substantial modifications of the phase structure are found once mesonic fluctuations are included, and for sufficiently strong diquark c","authors_text":"Mire Ugo, Schaefer Bernd-Jochen","cross_cats":["hep-th","nucl-th"],"headline":"Mesonic fluctuations beyond mean field substantially modify the phase structure of the two-flavor quark-meson-diquark model and allow diquark condensation to dominate at strong couplings.","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2026-05-13T16:12:38Z","title":"Diquark Correlators and Phase Structure in the Quark-Meson-Diquark Model beyond Mean Field"},"references":{"count":113,"internal_anchors":45,"resolved_work":113,"sample":[{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":1,"title":"(38) simplifies to ∂tUk(σ,∆) = k5 12π2 3 ϵπ + 1 ϵσ − 4Nf ϵq θ(ϵ− q ) + ϵ+ q E+q + ϵ− q E−q","work_id":"f7216f1f-55df-428b-b9cd-c05706be98ba","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":2,"title":"Quark-meson flows For ∆ = 0 and finite temperature, the quasi-particle energies reduce to E+ q →ϵ + q andE − q → |ϵ − q |.(44) Consequently, the flow converges to that of a quark- meson flow withN c =","work_id":"bfd2cd6c-37f3-4a70-91c9-d73092a71b82","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":3,"title":"In principle, the corresponding RGC initial condition follows directly from the definition of the scale-dependent mean-field potential in Eq","work_id":"9879e45b-dfb2-4bab-a5b5-b770612da9a5","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":4,"title":"Mathematically, RG flows form a semi-group rather than a group: the coarse-graining from the UV to the IR is irreversible and no inverse trans- formation exists","work_id":"abbeb01c-2d20-4d24-938a-b40b8b435400","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":5,"title":"Back-bending of the chiral transition line in mLPA The characteristic back-bending of the chiral transi- tion line at decreasingT(Fig. 3, right panels) has also been observed in other low-energy effec","work_id":"35151ce2-d779-43ec-a760-772e8ed6abe1","year":null}],"snapshot_sha256":"4354bc6203548f096d94ed420aab64294bd98f368fda2d6241a9f0dc87ac3949"},"source":{"id":"2605.13934","kind":"arxiv","version":1},"verdict":{"created_at":"2026-05-15T02:50:28.985098Z","id":"1fc38a3c-2be3-4d5c-aaea-b74a19654b3d","model_set":{"reader":"grok-4.3"},"one_line_summary":"Including mesonic fluctuations beyond mean field substantially modifies the phase structure of the quark-meson-diquark model, with diquark condensation dominating for strong couplings as analyzed via diquark pole mass and the Silver-Blaze property.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"Mesonic fluctuations beyond mean field substantially modify the phase structure of the two-flavor quark-meson-diquark model and allow diquark condensation to dominate at strong couplings.","strongest_claim":"Substantial modifications of the phase structure are found once mesonic fluctuations are included, and for sufficiently strong diquark couplings the dynamics become dominated by diquark condensation. These effects are elucidated through an analysis of the diquark pole mass and the Silver-Blaze property.","weakest_assumption":"The quark-meson-diquark model with the chosen FRG truncation accurately captures the relevant non-perturbative QCD dynamics at finite density, and that ensuring RG consistency of the effective potential fully eliminates cutoff artifacts."}},"verdict_id":"1fc38a3c-2be3-4d5c-aaea-b74a19654b3d"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:2c715ae5a3db91f0945d7ba334d7170a138b897133146817238b626e8b896a9d","target":"record","created_at":"2026-05-17T23:39:13Z","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":"e9e57fd2fc712c6d870fa94b9d0ef12628e048c8a499d9f663968ed645e9ba03","cross_cats_sorted":["hep-th","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2026-05-13T16:12:38Z","title_canon_sha256":"00dcea7e59ca2efbabe8a33cd0b3e771d7fe35fcaed084ce1d9f412706846b44"},"schema_version":"1.0","source":{"id":"2605.13934","kind":"arxiv","version":1}},"canonical_sha256":"394b0af8897d72d31c5f4733e326f497c1c882dfae93258962ffcc22babf4088","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"394b0af8897d72d31c5f4733e326f497c1c882dfae93258962ffcc22babf4088","first_computed_at":"2026-05-17T23:39:13.946096Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:39:13.946096Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"djGmhhO7lMSEwQM6cd3ycKKz8bg2K6w48/GYvu8o0dHpCHcNb6HkPav07DMKxjFEumQiR/bJUcMaJHA+V40SCw==","signature_status":"signed_v1","signed_at":"2026-05-17T23:39:13.946847Z","signed_message":"canonical_sha256_bytes"},"source_id":"2605.13934","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2c715ae5a3db91f0945d7ba334d7170a138b897133146817238b626e8b896a9d","sha256:27ff7fb6a50f25a4e7adda779cebb201803d59833b23946fb038c3e4b66b5dba"],"state_sha256":"ce9cdac03a3b77d07ab5b88955d2c01ad1ba89a64003c9df580b31ea32fb6e6f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aT7QRz3mCuXxs8v54kLPKC049q6n4jN0XpG0SdOih9yTiMwezpyz0NPfECFnXSgAk7EJKfaAOW1PGfAiToH3Dg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-27T04:47:48.656989Z","bundle_sha256":"51927062295086dc48e3681dde234213a0aa3bb2c0ee92b05639a99d36af020d"}}