{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2023:L55DMTGFXVHTGA7WM6YH4NT5EC","short_pith_number":"pith:L55DMTGF","canonical_record":{"source":{"id":"2304.04417","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"math.PR","submitted_at":"2023-04-10T06:56:23Z","cross_cats_sorted":["math.CV"],"title_canon_sha256":"1955e78164cfee1b225892fcf038bd701e5e644c914585fb7749f601880f44a0","abstract_canon_sha256":"25cf164edf02508bbeba99040dd714b4118e0f09183785eedd5e2e46910c20b9"},"schema_version":"1.0"},"canonical_sha256":"5f7a364cc5bd4f3303f667b07e367d20890074aeee382bc5f0bf19cc6891325b","source":{"kind":"arxiv","id":"2304.04417","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2304.04417","created_at":"2026-05-27T01:05:31Z"},{"alias_kind":"arxiv_version","alias_value":"2304.04417v3","created_at":"2026-05-27T01:05:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2304.04417","created_at":"2026-05-27T01:05:31Z"},{"alias_kind":"pith_short_12","alias_value":"L55DMTGFXVHT","created_at":"2026-05-27T01:05:31Z"},{"alias_kind":"pith_short_16","alias_value":"L55DMTGFXVHTGA7W","created_at":"2026-05-27T01:05:31Z"},{"alias_kind":"pith_short_8","alias_value":"L55DMTGF","created_at":"2026-05-27T01:05:31Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2023:L55DMTGFXVHTGA7WM6YH4NT5EC","target":"record","payload":{"canonical_record":{"source":{"id":"2304.04417","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"math.PR","submitted_at":"2023-04-10T06:56:23Z","cross_cats_sorted":["math.CV"],"title_canon_sha256":"1955e78164cfee1b225892fcf038bd701e5e644c914585fb7749f601880f44a0","abstract_canon_sha256":"25cf164edf02508bbeba99040dd714b4118e0f09183785eedd5e2e46910c20b9"},"schema_version":"1.0"},"canonical_sha256":"5f7a364cc5bd4f3303f667b07e367d20890074aeee382bc5f0bf19cc6891325b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-27T01:05:31.674765Z","signature_b64":"pO8wN/Lfi/5oLSnVuY0gTcPkJOlsw5Y/3s4l37wYLBCEKYA2G9mlpoJl2wT7L8cuI+3qyMjYLgZObmR4+bUCAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5f7a364cc5bd4f3303f667b07e367d20890074aeee382bc5f0bf19cc6891325b","last_reissued_at":"2026-05-27T01:05:31.674164Z","signature_status":"signed_v1","first_computed_at":"2026-05-27T01:05:31.674164Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2304.04417","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-27T01:05:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VYhIcqB5mfxJMIEczDW0Kl85RBpTC1sJel7K5lnqEv57tNPGxMg1OpkkG99AADeWMpzvD10EYQ9f6wNoJlHwCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-19T22:49:14.280659Z"},"content_sha256":"8132deb6e735b81f75f3dccca8497eb675c4c5d3fdea20eecc5adb9018990ed4","schema_version":"1.0","event_id":"sha256:8132deb6e735b81f75f3dccca8497eb675c4c5d3fdea20eecc5adb9018990ed4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2023:L55DMTGFXVHTGA7WM6YH4NT5EC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Tip growth in a strongly concentrated aggregation model follows local geodesics","license":"http://creativecommons.org/licenses/by-sa/4.0/","headline":"Starting from k needles, the small-particle limit of aggregate Loewner evolution is the Laplacian path model in which tips grow along geodesics to infinity.","cross_cats":["math.CV"],"primary_cat":"math.PR","authors_text":"Frankie Higgs","submitted_at":"2023-04-10T06:56:23Z","abstract_excerpt":"We analyse the aggregate Loewner evolution (ALE), introduced in 2018 by Sola, Turner and Viklund to generalise versions of diffusion limited aggregation (DLA) in the plane using complex analysis. They showed convergence of the ALE for certain parameters to a single growing slit. Started from a non-trivial initial configuration of $k$ needles and the same parameters, we show that the small-particle scaling limit of ALE is the Laplacian path model, introduced by Carleson and Makarov in 2002, in which the tips grow along geodesics towards $\\infty$.\n  Our proof involves analysis of Loewner's equat"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"Started from a non-trivial initial configuration of k needles and the same parameters, we show that the small-particle scaling limit of ALE is the Laplacian path model, introduced by Carleson and Makarov in 2002, in which the tips grow along geodesics towards ∞.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"The result assumes the same parameters as the 2018 work (where ALE converges to a single slit) together with an initial configuration of exactly k needles; the scaling limit and geodesic behavior are shown only under these choices and may fail for other parameter regimes or initial data.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"The small-particle scaling limit of aggregate Loewner evolution from k needles is the Laplacian path model with geodesic tip growth.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"Starting from k needles, the small-particle limit of aggregate Loewner evolution is the Laplacian path model in which tips grow along geodesics to infinity.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"56c6db01ad440ede116d914cb75d006b8dc5b85e1530622ffa6b3ad9ba8de327"},"source":{"id":"2304.04417","kind":"arxiv","version":3},"verdict":{"id":"4a13e5b6-8134-43b4-b421-3d5faf78230e","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-24T09:01:29.475288Z","strongest_claim":"Started from a non-trivial initial configuration of k needles and the same parameters, we show that the small-particle scaling limit of ALE is the Laplacian path model, introduced by Carleson and Makarov in 2002, in which the tips grow along geodesics towards ∞.","one_line_summary":"The small-particle scaling limit of aggregate Loewner evolution from k needles is the Laplacian path model with geodesic tip growth.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"The result assumes the same parameters as the 2018 work (where ALE converges to a single slit) together with an initial configuration of exactly k needles; the scaling limit and geodesic behavior are shown only under these choices and may fail for other parameter regimes or initial data.","pith_extraction_headline":"Starting from k needles, the small-particle limit of aggregate Loewner evolution is the Laplacian path model in which tips grow along geodesics to infinity."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2304.04417/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":16,"sample":[{"doi":"","year":2002,"title":"Laplacian path mo dels","work_id":"89c3936f-3054-4f73-ac08-093382f7d689","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"10.1073/pnas.1215218109","year":2012,"title":"Petroff, Hansj¨ org F","work_id":"76e5452e-3d8b-4400-a7a1-ba81814733ee","ref_index":2,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"10.1103/physreve.95.033113","year":2017,"title":"Seybold, and Daniel H","work_id":"22e7eb06-48d4-40af-9db3-1ed1509a3418","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"10.1017/cbo9780511755347","year":2002,"title":"Richard M. Dudley. Real Analysis and Probability . Cambridge Studies in Advanced Mathematics. Cambridge University Press, seco nd edition, 2002. doi:10.1017/CBO9780511755347","work_id":"07d966c4-0816-4b67-9448-8451ff937982","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"10.1103/physreve.77.041602","year":2008,"title":"Fingered growth in cha nnel geome- try: A Loewner-equation approach","work_id":"b5a71413-c647-40da-8cdb-bdbb7e17f0ab","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":16,"snapshot_sha256":"19f86c292f3e2cd5a6716014aa3381b9c7bae7cfbfdaa8250c78df689154ed74","internal_anchors":0},"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":"4a13e5b6-8134-43b4-b421-3d5faf78230e"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-27T01:05:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ABc+4P6U1/EIiyozfBYwWys4bL8zD7DBa6XZIRDwnxPavIdICbS2I1OX/C7pcv2vQoUSc3MFvVmYxSv8nCOIBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-19T22:49:14.281404Z"},"content_sha256":"93af5366821dc1fa29a14c6428d856eb990c5a6f120d4babaa2ceb42f25e792b","schema_version":"1.0","event_id":"sha256:93af5366821dc1fa29a14c6428d856eb990c5a6f120d4babaa2ceb42f25e792b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/L55DMTGFXVHTGA7WM6YH4NT5EC/bundle.json","state_url":"https://pith.science/pith/L55DMTGFXVHTGA7WM6YH4NT5EC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/L55DMTGFXVHTGA7WM6YH4NT5EC/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":"2026-06-19T22:49:14Z","links":{"resolver":"https://pith.science/pith/L55DMTGFXVHTGA7WM6YH4NT5EC","bundle":"https://pith.science/pith/L55DMTGFXVHTGA7WM6YH4NT5EC/bundle.json","state":"https://pith.science/pith/L55DMTGFXVHTGA7WM6YH4NT5EC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/L55DMTGFXVHTGA7WM6YH4NT5EC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:L55DMTGFXVHTGA7WM6YH4NT5EC","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":"25cf164edf02508bbeba99040dd714b4118e0f09183785eedd5e2e46910c20b9","cross_cats_sorted":["math.CV"],"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"math.PR","submitted_at":"2023-04-10T06:56:23Z","title_canon_sha256":"1955e78164cfee1b225892fcf038bd701e5e644c914585fb7749f601880f44a0"},"schema_version":"1.0","source":{"id":"2304.04417","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2304.04417","created_at":"2026-05-27T01:05:31Z"},{"alias_kind":"arxiv_version","alias_value":"2304.04417v3","created_at":"2026-05-27T01:05:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2304.04417","created_at":"2026-05-27T01:05:31Z"},{"alias_kind":"pith_short_12","alias_value":"L55DMTGFXVHT","created_at":"2026-05-27T01:05:31Z"},{"alias_kind":"pith_short_16","alias_value":"L55DMTGFXVHTGA7W","created_at":"2026-05-27T01:05:31Z"},{"alias_kind":"pith_short_8","alias_value":"L55DMTGF","created_at":"2026-05-27T01:05:31Z"}],"graph_snapshots":[{"event_id":"sha256:93af5366821dc1fa29a14c6428d856eb990c5a6f120d4babaa2ceb42f25e792b","target":"graph","created_at":"2026-05-27T01:05:31Z","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":"Started from a non-trivial initial configuration of k needles and the same parameters, we show that the small-particle scaling limit of ALE is the Laplacian path model, introduced by Carleson and Makarov in 2002, in which the tips grow along geodesics towards ∞."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"The result assumes the same parameters as the 2018 work (where ALE converges to a single slit) together with an initial configuration of exactly k needles; the scaling limit and geodesic behavior are shown only under these choices and may fail for other parameter regimes or initial data."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"The small-particle scaling limit of aggregate Loewner evolution from k needles is the Laplacian path model with geodesic tip growth."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"Starting from k needles, the small-particle limit of aggregate Loewner evolution is the Laplacian path model in which tips grow along geodesics to infinity."}],"snapshot_sha256":"56c6db01ad440ede116d914cb75d006b8dc5b85e1530622ffa6b3ad9ba8de327"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2304.04417/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We analyse the aggregate Loewner evolution (ALE), introduced in 2018 by Sola, Turner and Viklund to generalise versions of diffusion limited aggregation (DLA) in the plane using complex analysis. They showed convergence of the ALE for certain parameters to a single growing slit. Started from a non-trivial initial configuration of $k$ needles and the same parameters, we show that the small-particle scaling limit of ALE is the Laplacian path model, introduced by Carleson and Makarov in 2002, in which the tips grow along geodesics towards $\\infty$.\n  Our proof involves analysis of Loewner's equat","authors_text":"Frankie Higgs","cross_cats":["math.CV"],"headline":"Starting from k needles, the small-particle limit of aggregate Loewner evolution is the Laplacian path model in which tips grow along geodesics to infinity.","license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"math.PR","submitted_at":"2023-04-10T06:56:23Z","title":"Tip growth in a strongly concentrated aggregation model follows local geodesics"},"references":{"count":16,"internal_anchors":0,"resolved_work":16,"sample":[{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":1,"title":"Laplacian path mo dels","work_id":"89c3936f-3054-4f73-ac08-093382f7d689","year":2002},{"cited_arxiv_id":"","doi":"10.1073/pnas.1215218109","is_internal_anchor":false,"ref_index":2,"title":"Petroff, Hansj¨ org F","work_id":"76e5452e-3d8b-4400-a7a1-ba81814733ee","year":2012},{"cited_arxiv_id":"","doi":"10.1103/physreve.95.033113","is_internal_anchor":false,"ref_index":3,"title":"Seybold, and Daniel H","work_id":"22e7eb06-48d4-40af-9db3-1ed1509a3418","year":2017},{"cited_arxiv_id":"","doi":"10.1017/cbo9780511755347","is_internal_anchor":false,"ref_index":4,"title":"Richard M. Dudley. Real Analysis and Probability . Cambridge Studies in Advanced Mathematics. Cambridge University Press, seco nd edition, 2002. doi:10.1017/CBO9780511755347","work_id":"07d966c4-0816-4b67-9448-8451ff937982","year":2002},{"cited_arxiv_id":"","doi":"10.1103/physreve.77.041602","is_internal_anchor":false,"ref_index":5,"title":"Fingered growth in cha nnel geome- try: A Loewner-equation approach","work_id":"b5a71413-c647-40da-8cdb-bdbb7e17f0ab","year":2008}],"snapshot_sha256":"19f86c292f3e2cd5a6716014aa3381b9c7bae7cfbfdaa8250c78df689154ed74"},"source":{"id":"2304.04417","kind":"arxiv","version":3},"verdict":{"created_at":"2026-05-24T09:01:29.475288Z","id":"4a13e5b6-8134-43b4-b421-3d5faf78230e","model_set":{"reader":"grok-4.3"},"one_line_summary":"The small-particle scaling limit of aggregate Loewner evolution from k needles is the Laplacian path model with geodesic tip growth.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"Starting from k needles, the small-particle limit of aggregate Loewner evolution is the Laplacian path model in which tips grow along geodesics to infinity.","strongest_claim":"Started from a non-trivial initial configuration of k needles and the same parameters, we show that the small-particle scaling limit of ALE is the Laplacian path model, introduced by Carleson and Makarov in 2002, in which the tips grow along geodesics towards ∞.","weakest_assumption":"The result assumes the same parameters as the 2018 work (where ALE converges to a single slit) together with an initial configuration of exactly k needles; the scaling limit and geodesic behavior are shown only under these choices and may fail for other parameter regimes or initial data."}},"verdict_id":"4a13e5b6-8134-43b4-b421-3d5faf78230e"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:8132deb6e735b81f75f3dccca8497eb675c4c5d3fdea20eecc5adb9018990ed4","target":"record","created_at":"2026-05-27T01:05:31Z","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":"25cf164edf02508bbeba99040dd714b4118e0f09183785eedd5e2e46910c20b9","cross_cats_sorted":["math.CV"],"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"math.PR","submitted_at":"2023-04-10T06:56:23Z","title_canon_sha256":"1955e78164cfee1b225892fcf038bd701e5e644c914585fb7749f601880f44a0"},"schema_version":"1.0","source":{"id":"2304.04417","kind":"arxiv","version":3}},"canonical_sha256":"5f7a364cc5bd4f3303f667b07e367d20890074aeee382bc5f0bf19cc6891325b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5f7a364cc5bd4f3303f667b07e367d20890074aeee382bc5f0bf19cc6891325b","first_computed_at":"2026-05-27T01:05:31.674164Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-27T01:05:31.674164Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"pO8wN/Lfi/5oLSnVuY0gTcPkJOlsw5Y/3s4l37wYLBCEKYA2G9mlpoJl2wT7L8cuI+3qyMjYLgZObmR4+bUCAg==","signature_status":"signed_v1","signed_at":"2026-05-27T01:05:31.674765Z","signed_message":"canonical_sha256_bytes"},"source_id":"2304.04417","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8132deb6e735b81f75f3dccca8497eb675c4c5d3fdea20eecc5adb9018990ed4","sha256:93af5366821dc1fa29a14c6428d856eb990c5a6f120d4babaa2ceb42f25e792b"],"state_sha256":"36ba0451e7a5fc50dd560d9b34c41d4c874a06ddac5648613cbd11e13111aec6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Cx0aF9ezjae2DED1RqvHow/fDWeTdUq/1w/HJhTHwOXBA7PtAvUYiRIPsf8A1ahsmOP7ZInNW4BydqcfQmHZAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-19T22:49:14.284192Z","bundle_sha256":"8467419869009a7efc763d82d4dd3a64a2c588062ee9549b95c5f96e532b44aa"}}