{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:E24XXVINOWZ3O53BAKCCYKV4QQ","short_pith_number":"pith:E24XXVIN","canonical_record":{"source":{"id":"2605.15427","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2026-05-14T21:18:27Z","cross_cats_sorted":[],"title_canon_sha256":"8ba6de3290962e73d13fbdeac907fe18016b1d1d7b52249425aea11f610cd890","abstract_canon_sha256":"74f687c0c649493b2ede5bdbc7a01b79ddaaee1ebdfa724b209b38f2b0cc8bd9"},"schema_version":"1.0"},"canonical_sha256":"26b97bd50d75b3b7776102842c2abc840a68dd85693427452b09a532a3ca579f","source":{"kind":"arxiv","id":"2605.15427","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.15427","created_at":"2026-05-20T00:00:58Z"},{"alias_kind":"arxiv_version","alias_value":"2605.15427v1","created_at":"2026-05-20T00:00:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.15427","created_at":"2026-05-20T00:00:58Z"},{"alias_kind":"pith_short_12","alias_value":"E24XXVINOWZ3","created_at":"2026-05-20T00:00:58Z"},{"alias_kind":"pith_short_16","alias_value":"E24XXVINOWZ3O53B","created_at":"2026-05-20T00:00:58Z"},{"alias_kind":"pith_short_8","alias_value":"E24XXVIN","created_at":"2026-05-20T00:00:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:E24XXVINOWZ3O53BAKCCYKV4QQ","target":"record","payload":{"canonical_record":{"source":{"id":"2605.15427","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2026-05-14T21:18:27Z","cross_cats_sorted":[],"title_canon_sha256":"8ba6de3290962e73d13fbdeac907fe18016b1d1d7b52249425aea11f610cd890","abstract_canon_sha256":"74f687c0c649493b2ede5bdbc7a01b79ddaaee1ebdfa724b209b38f2b0cc8bd9"},"schema_version":"1.0"},"canonical_sha256":"26b97bd50d75b3b7776102842c2abc840a68dd85693427452b09a532a3ca579f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-20T00:00:58.103856Z","signature_b64":"4nGfcezH0lwcE8zt3cpYeHjs0bPctBUYo6DAagvNYsVZS3hf3m783ff4pGjBUsscfAHj7pU0mfWenJ9CczcnBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"26b97bd50d75b3b7776102842c2abc840a68dd85693427452b09a532a3ca579f","last_reissued_at":"2026-05-20T00:00:58.103077Z","signature_status":"signed_v1","first_computed_at":"2026-05-20T00:00:58.103077Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2605.15427","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":"2026-05-20T00:00:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Yyg4cdhLF9DeFtvjr7EYfGN6n263zR/rZTBm4kiwwQXFw4TNcNxEZGH5LbTM3T6mc/vv9IV+w7SA1/fIIbkdBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T09:30:47.900516Z"},"content_sha256":"d052162691c0c58796e9f069723a13cdeb684f849359930036ceeb86b64236e1","schema_version":"1.0","event_id":"sha256:d052162691c0c58796e9f069723a13cdeb684f849359930036ceeb86b64236e1"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:E24XXVINOWZ3O53BAKCCYKV4QQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Delayed current sheet formation due to an external field in pulsed-power-driven reconnection experiments","license":"http://creativecommons.org/licenses/by/4.0/","headline":"A strong external magnetic field delays current sheet formation by creating a void between colliding plasma flows instead of a dense reconnection layer.","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"A. P. Shah, B. J. Sporer, D. M. Johnson, G. V. Dowhan, J. D. Hare, J. Lee, M. Chen, N. M. Jordan, R. D. McBride, R. Shapovalov, T. W. O. Varnish","submitted_at":"2026-05-14T21:18:27Z","abstract_excerpt":"We present results from pulsed-power-driven magnetic reconnection experiments, in which we drove two exploding wire arrays in parallel to produce colliding plasma flows with anti-parallel magnetic fields of 1.2$\\pm$0.2 T. The experimental volume was surrounded by a Helmholtz coil pair capable of externally applying a field of up to 2 T, parallel to the reconnecting electric field. We diagnosed these experiments using laser interferometric imaging in the direction of the anti-parallel magnetic fields, gated extreme ultraviolet pinhole imaging, and in situ inductive probes. For zero and weak (0."},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"When a strong external field (2 T) is applied, we observe a void between the arrays rather than a dense layer, and we hypothesise that the external field is frozen out of the plasma and provides a back-pressure which decelerates the flows.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"The external magnetic field remains frozen into the plasma on the experimental timescale and therefore exerts a sustained back-pressure on the incoming flows (stated in the hypothesis paragraph of the abstract).","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"Strong external magnetic fields applied parallel to the reconnecting electric field delay current-sheet formation in pulsed-power-driven reconnection by creating back-pressure that slows plasma inflows.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"A strong external magnetic field delays current sheet formation by creating a void between colliding plasma flows instead of a dense reconnection layer.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"242871a4700b858afd36979e9ab9015cb84afd2906c9b141e58b88109a83b8f8"},"source":{"id":"2605.15427","kind":"arxiv","version":1},"verdict":{"id":"b9c77743-e930-473c-a0de-f19e732a2c08","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-19T14:47:46.578931Z","strongest_claim":"When a strong external field (2 T) is applied, we observe a void between the arrays rather than a dense layer, and we hypothesise that the external field is frozen out of the plasma and provides a back-pressure which decelerates the flows.","one_line_summary":"Strong external magnetic fields applied parallel to the reconnecting electric field delay current-sheet formation in pulsed-power-driven reconnection by creating back-pressure that slows plasma inflows.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"The external magnetic field remains frozen into the plasma on the experimental timescale and therefore exerts a sustained back-pressure on the incoming flows (stated in the hypothesis paragraph of the abstract).","pith_extraction_headline":"A strong external magnetic field delays current sheet formation by creating a void between colliding plasma flows instead of a dense reconnection layer."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2605.15427/integrity.json","findings":[],"available":true,"detectors_run":[{"name":"cited_work_retraction","ran_at":"2026-05-19T15:55:04.939915Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"citation_quote_validity","ran_at":"2026-05-19T15:50:38.382495Z","status":"completed","version":"0.1.0","findings_count":0},{"name":"doi_compliance","ran_at":"2026-05-19T15:01:44.008905Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"doi_title_agreement","ran_at":"2026-05-19T15:01:17.679143Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"claim_evidence","ran_at":"2026-05-19T14:21:54.134609Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"ai_meta_artifact","ran_at":"2026-05-19T13:33:22.697871Z","status":"skipped","version":"1.0.0","findings_count":0}],"snapshot_sha256":"8503685848f113c69ef44da505bfa1389e7805cedc613600b50fcc11a45d4868"},"references":{"count":36,"sample":[{"doi":"10.1098/rspa.2016.0479","year":2016,"title":"Perspectives on magnetic reconnection , volume =","work_id":"9fd556e8-7e32-4e22-a10b-22d1ecc8aa1a","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"10.1103/physrevlett.116.105003","year":2016,"title":"Physical Review Letters , author =","work_id":"19378392-bc02-47e6-b990-0403f2133681","ref_index":2,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":null,"title":"Fiksel, G. and Fox, W. and Bhattacharjee, A. and Barnak, D. H. and Chang, P.-Y. and Germaschewski, K. and Hu, S. X. and Nilson, P. M. , year =. Magnetic. Physical Review Letters , volume =","work_id":"6a482745-0096-4c95-a959-bc54058d01d4","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":null,"title":"Felber, F. S. and Wessel, F. J. and Wild, N. C. and Rahman, H. U. and Fisher, A. and Fowler, C. M. and Liberman, M. A. and Velikovich, A. L. , year =. Ultrahigh Magnetic Fields Produced in a Gas-puff.","work_id":"d031b854-0023-42af-9313-3cb9b5195a71","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2013,"title":"Nuclear Fusion , author =","work_id":"9a344efb-fa9e-4d2f-a455-d902614aac8a","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":36,"snapshot_sha256":"fced0aea342cce581f297d20d4b7810957f7c04e22e2f4d74037e7e9109bddff","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":"b9c77743-e930-473c-a0de-f19e732a2c08"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-20T00:00:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4qEuOhdr34kapmlJndNg6frPYOq1JEA6ysEZdcs74SNaM4eSzErvmTCkcWLpv4639HQwsgmLUeQHUOm2ElRYCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T09:30:47.901182Z"},"content_sha256":"ac60bf02047587dda23af4101111b0d7b6cb96285bad3dea29f39fd54cd199e8","schema_version":"1.0","event_id":"sha256:ac60bf02047587dda23af4101111b0d7b6cb96285bad3dea29f39fd54cd199e8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/E24XXVINOWZ3O53BAKCCYKV4QQ/bundle.json","state_url":"https://pith.science/pith/E24XXVINOWZ3O53BAKCCYKV4QQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/E24XXVINOWZ3O53BAKCCYKV4QQ/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":"2026-05-28T09:30:47Z","links":{"resolver":"https://pith.science/pith/E24XXVINOWZ3O53BAKCCYKV4QQ","bundle":"https://pith.science/pith/E24XXVINOWZ3O53BAKCCYKV4QQ/bundle.json","state":"https://pith.science/pith/E24XXVINOWZ3O53BAKCCYKV4QQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/E24XXVINOWZ3O53BAKCCYKV4QQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:E24XXVINOWZ3O53BAKCCYKV4QQ","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":"74f687c0c649493b2ede5bdbc7a01b79ddaaee1ebdfa724b209b38f2b0cc8bd9","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2026-05-14T21:18:27Z","title_canon_sha256":"8ba6de3290962e73d13fbdeac907fe18016b1d1d7b52249425aea11f610cd890"},"schema_version":"1.0","source":{"id":"2605.15427","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.15427","created_at":"2026-05-20T00:00:58Z"},{"alias_kind":"arxiv_version","alias_value":"2605.15427v1","created_at":"2026-05-20T00:00:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.15427","created_at":"2026-05-20T00:00:58Z"},{"alias_kind":"pith_short_12","alias_value":"E24XXVINOWZ3","created_at":"2026-05-20T00:00:58Z"},{"alias_kind":"pith_short_16","alias_value":"E24XXVINOWZ3O53B","created_at":"2026-05-20T00:00:58Z"},{"alias_kind":"pith_short_8","alias_value":"E24XXVIN","created_at":"2026-05-20T00:00:58Z"}],"graph_snapshots":[{"event_id":"sha256:ac60bf02047587dda23af4101111b0d7b6cb96285bad3dea29f39fd54cd199e8","target":"graph","created_at":"2026-05-20T00:00:58Z","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":"When a strong external field (2 T) is applied, we observe a void between the arrays rather than a dense layer, and we hypothesise that the external field is frozen out of the plasma and provides a back-pressure which decelerates the flows."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"The external magnetic field remains frozen into the plasma on the experimental timescale and therefore exerts a sustained back-pressure on the incoming flows (stated in the hypothesis paragraph of the abstract)."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"Strong external magnetic fields applied parallel to the reconnecting electric field delay current-sheet formation in pulsed-power-driven reconnection by creating back-pressure that slows plasma inflows."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"A strong external magnetic field delays current sheet formation by creating a void between colliding plasma flows instead of a dense reconnection layer."}],"snapshot_sha256":"242871a4700b858afd36979e9ab9015cb84afd2906c9b141e58b88109a83b8f8"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[{"findings_count":0,"name":"cited_work_retraction","ran_at":"2026-05-19T15:55:04.939915Z","status":"completed","version":"1.0.0"},{"findings_count":0,"name":"citation_quote_validity","ran_at":"2026-05-19T15:50:38.382495Z","status":"completed","version":"0.1.0"},{"findings_count":0,"name":"doi_compliance","ran_at":"2026-05-19T15:01:44.008905Z","status":"completed","version":"1.0.0"},{"findings_count":0,"name":"doi_title_agreement","ran_at":"2026-05-19T15:01:17.679143Z","status":"completed","version":"1.0.0"},{"findings_count":0,"name":"claim_evidence","ran_at":"2026-05-19T14:21:54.134609Z","status":"completed","version":"1.0.0"},{"findings_count":0,"name":"ai_meta_artifact","ran_at":"2026-05-19T13:33:22.697871Z","status":"skipped","version":"1.0.0"}],"endpoint":"/pith/2605.15427/integrity.json","findings":[],"snapshot_sha256":"8503685848f113c69ef44da505bfa1389e7805cedc613600b50fcc11a45d4868","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present results from pulsed-power-driven magnetic reconnection experiments, in which we drove two exploding wire arrays in parallel to produce colliding plasma flows with anti-parallel magnetic fields of 1.2$\\pm$0.2 T. The experimental volume was surrounded by a Helmholtz coil pair capable of externally applying a field of up to 2 T, parallel to the reconnecting electric field. We diagnosed these experiments using laser interferometric imaging in the direction of the anti-parallel magnetic fields, gated extreme ultraviolet pinhole imaging, and in situ inductive probes. For zero and weak (0.","authors_text":"A. P. Shah, B. J. Sporer, D. M. Johnson, G. V. Dowhan, J. D. Hare, J. Lee, M. Chen, N. M. Jordan, R. D. McBride, R. Shapovalov, T. W. O. Varnish","cross_cats":[],"headline":"A strong external magnetic field delays current sheet formation by creating a void between colliding plasma flows instead of a dense reconnection layer.","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2026-05-14T21:18:27Z","title":"Delayed current sheet formation due to an external field in pulsed-power-driven reconnection experiments"},"references":{"count":36,"internal_anchors":0,"resolved_work":36,"sample":[{"cited_arxiv_id":"","doi":"10.1098/rspa.2016.0479","is_internal_anchor":false,"ref_index":1,"title":"Perspectives on magnetic reconnection , volume =","work_id":"9fd556e8-7e32-4e22-a10b-22d1ecc8aa1a","year":2016},{"cited_arxiv_id":"","doi":"10.1103/physrevlett.116.105003","is_internal_anchor":false,"ref_index":2,"title":"Physical Review Letters , author =","work_id":"19378392-bc02-47e6-b990-0403f2133681","year":2016},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":3,"title":"Fiksel, G. and Fox, W. and Bhattacharjee, A. and Barnak, D. H. and Chang, P.-Y. and Germaschewski, K. and Hu, S. X. and Nilson, P. M. , year =. Magnetic. Physical Review Letters , volume =","work_id":"6a482745-0096-4c95-a959-bc54058d01d4","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":4,"title":"Felber, F. S. and Wessel, F. J. and Wild, N. C. and Rahman, H. U. and Fisher, A. and Fowler, C. M. and Liberman, M. A. and Velikovich, A. L. , year =. Ultrahigh Magnetic Fields Produced in a Gas-puff.","work_id":"d031b854-0023-42af-9313-3cb9b5195a71","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":5,"title":"Nuclear Fusion , author =","work_id":"9a344efb-fa9e-4d2f-a455-d902614aac8a","year":2013}],"snapshot_sha256":"fced0aea342cce581f297d20d4b7810957f7c04e22e2f4d74037e7e9109bddff"},"source":{"id":"2605.15427","kind":"arxiv","version":1},"verdict":{"created_at":"2026-05-19T14:47:46.578931Z","id":"b9c77743-e930-473c-a0de-f19e732a2c08","model_set":{"reader":"grok-4.3"},"one_line_summary":"Strong external magnetic fields applied parallel to the reconnecting electric field delay current-sheet formation in pulsed-power-driven reconnection by creating back-pressure that slows plasma inflows.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"A strong external magnetic field delays current sheet formation by creating a void between colliding plasma flows instead of a dense reconnection layer.","strongest_claim":"When a strong external field (2 T) is applied, we observe a void between the arrays rather than a dense layer, and we hypothesise that the external field is frozen out of the plasma and provides a back-pressure which decelerates the flows.","weakest_assumption":"The external magnetic field remains frozen into the plasma on the experimental timescale and therefore exerts a sustained back-pressure on the incoming flows (stated in the hypothesis paragraph of the abstract)."}},"verdict_id":"b9c77743-e930-473c-a0de-f19e732a2c08"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:d052162691c0c58796e9f069723a13cdeb684f849359930036ceeb86b64236e1","target":"record","created_at":"2026-05-20T00:00:58Z","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":"74f687c0c649493b2ede5bdbc7a01b79ddaaee1ebdfa724b209b38f2b0cc8bd9","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2026-05-14T21:18:27Z","title_canon_sha256":"8ba6de3290962e73d13fbdeac907fe18016b1d1d7b52249425aea11f610cd890"},"schema_version":"1.0","source":{"id":"2605.15427","kind":"arxiv","version":1}},"canonical_sha256":"26b97bd50d75b3b7776102842c2abc840a68dd85693427452b09a532a3ca579f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"26b97bd50d75b3b7776102842c2abc840a68dd85693427452b09a532a3ca579f","first_computed_at":"2026-05-20T00:00:58.103077Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-20T00:00:58.103077Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4nGfcezH0lwcE8zt3cpYeHjs0bPctBUYo6DAagvNYsVZS3hf3m783ff4pGjBUsscfAHj7pU0mfWenJ9CczcnBg==","signature_status":"signed_v1","signed_at":"2026-05-20T00:00:58.103856Z","signed_message":"canonical_sha256_bytes"},"source_id":"2605.15427","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d052162691c0c58796e9f069723a13cdeb684f849359930036ceeb86b64236e1","sha256:ac60bf02047587dda23af4101111b0d7b6cb96285bad3dea29f39fd54cd199e8"],"state_sha256":"051d3fb1f0997326e73940bd8f6789284785a6ecfad4062658fd31fcd24db52d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"D0pCMcRoeIuscgezPRzo1ibPLVyzoDClPEwpC2IC+MWiMrgU9HwMW1VA11a9Sz6JVg0G8zmw2aeHELI+6dOMBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T09:30:47.904089Z","bundle_sha256":"d419b74b602b3004a3465d7bff8e2a1de98b837ee55c401adb68e5716e910f05"}}