{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:AOZRM5TN4NGPM3BKOSGMU3JY2B","short_pith_number":"pith:AOZRM5TN","canonical_record":{"source":{"id":"2606.26362","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2026-06-24T20:18:14Z","cross_cats_sorted":[],"title_canon_sha256":"fe318e5cbc449e9823d0913e7d3be111decf319c5167641ad685b0b4da4866ed","abstract_canon_sha256":"9dee8bee5258e8aa53f9a68c30d5c45a043683018e08f882f1ba71e144d0bd00"},"schema_version":"1.0"},"canonical_sha256":"03b316766de34cf66c2a748cca6d38d0555ba2e3e5eef48b779fb49363b5703a","source":{"kind":"arxiv","id":"2606.26362","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2606.26362","created_at":"2026-06-26T00:15:38Z"},{"alias_kind":"arxiv_version","alias_value":"2606.26362v1","created_at":"2026-06-26T00:15:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.26362","created_at":"2026-06-26T00:15:38Z"},{"alias_kind":"pith_short_12","alias_value":"AOZRM5TN4NGP","created_at":"2026-06-26T00:15:38Z"},{"alias_kind":"pith_short_16","alias_value":"AOZRM5TN4NGPM3BK","created_at":"2026-06-26T00:15:38Z"},{"alias_kind":"pith_short_8","alias_value":"AOZRM5TN","created_at":"2026-06-26T00:15:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:AOZRM5TN4NGPM3BKOSGMU3JY2B","target":"record","payload":{"canonical_record":{"source":{"id":"2606.26362","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2026-06-24T20:18:14Z","cross_cats_sorted":[],"title_canon_sha256":"fe318e5cbc449e9823d0913e7d3be111decf319c5167641ad685b0b4da4866ed","abstract_canon_sha256":"9dee8bee5258e8aa53f9a68c30d5c45a043683018e08f882f1ba71e144d0bd00"},"schema_version":"1.0"},"canonical_sha256":"03b316766de34cf66c2a748cca6d38d0555ba2e3e5eef48b779fb49363b5703a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-26T00:15:38.004564Z","signature_b64":"ep4K/0MkoV09AQOSbZHd6egCb9y1EHezi83cfNMQUZKJENYR/62AdP1k6mMU1PzpToaheWCHWBYUlZKfnG1/Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"03b316766de34cf66c2a748cca6d38d0555ba2e3e5eef48b779fb49363b5703a","last_reissued_at":"2026-06-26T00:15:38.004159Z","signature_status":"signed_v1","first_computed_at":"2026-06-26T00:15:38.004159Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2606.26362","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":"2026-06-26T00:15:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fASGmYL2RiU5fEsDZrV021xruWkQ5Ea0XU9zIUa+32B3uIFcDakKcw6P1zE2k+0Z4LolY0VT7fFlA2NercsLBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-26T18:47:12.316816Z"},"content_sha256":"d1227fd8ca4e2b0f7038c441fc1265df0ee56906354c930a1903342f7c2817c3","schema_version":"1.0","event_id":"sha256:d1227fd8ca4e2b0f7038c441fc1265df0ee56906354c930a1903342f7c2817c3"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:AOZRM5TN4NGPM3BKOSGMU3JY2B","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Integrating Gyrokinetic Flux Predictions with Ideal MHD Stability Boundaries","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"F. D. Halpern, J. Candy, J. McClenaghan, K. E. Thome, S. Saarelma, T. F. Neiser, the MAST-U team, T. H. Osborne","submitted_at":"2026-06-24T20:18:14Z","abstract_excerpt":"Accurate prediction of pedestal height and width in tokamaks remains a critical issue as it strongly influences the predicted plasma performance of all future reactors. We present an integrated pedestal-stability workflow that combines equilibrium scans with magnetohydrodynamic (MHD) stability analysis using ELITE and GATO and gyrokinetic transport predictions using CGYRO/QLGYRO. The workflow reproduces the characteristic KBM first- and second-stability structure previously identified in gyrokinetic pedestal studies. Applied to spherical tokamaks (STs), the workflow shows good agreement with p"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.26362","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2606.26362/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","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":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-06-26T00:15:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kmw56uPys6bmgvYDSSyhfnLLxMsLLvZolIf7kxSzqyH1UR72CZ9345S4zRiyLeEsiT1qV3H1zB+ISIXHsowWDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-26T18:47:12.317445Z"},"content_sha256":"43fd02bd6a32243c7c3c633ba920da62c870378d48f9b595e0f4a992c08016ac","schema_version":"1.0","event_id":"sha256:43fd02bd6a32243c7c3c633ba920da62c870378d48f9b595e0f4a992c08016ac"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/AOZRM5TN4NGPM3BKOSGMU3JY2B/bundle.json","state_url":"https://pith.science/pith/AOZRM5TN4NGPM3BKOSGMU3JY2B/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/AOZRM5TN4NGPM3BKOSGMU3JY2B/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":"2026-06-26T18:47:12Z","links":{"resolver":"https://pith.science/pith/AOZRM5TN4NGPM3BKOSGMU3JY2B","bundle":"https://pith.science/pith/AOZRM5TN4NGPM3BKOSGMU3JY2B/bundle.json","state":"https://pith.science/pith/AOZRM5TN4NGPM3BKOSGMU3JY2B/state.json","well_known_bundle":"https://pith.science/.well-known/pith/AOZRM5TN4NGPM3BKOSGMU3JY2B/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:AOZRM5TN4NGPM3BKOSGMU3JY2B","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":"9dee8bee5258e8aa53f9a68c30d5c45a043683018e08f882f1ba71e144d0bd00","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2026-06-24T20:18:14Z","title_canon_sha256":"fe318e5cbc449e9823d0913e7d3be111decf319c5167641ad685b0b4da4866ed"},"schema_version":"1.0","source":{"id":"2606.26362","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2606.26362","created_at":"2026-06-26T00:15:38Z"},{"alias_kind":"arxiv_version","alias_value":"2606.26362v1","created_at":"2026-06-26T00:15:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.26362","created_at":"2026-06-26T00:15:38Z"},{"alias_kind":"pith_short_12","alias_value":"AOZRM5TN4NGP","created_at":"2026-06-26T00:15:38Z"},{"alias_kind":"pith_short_16","alias_value":"AOZRM5TN4NGPM3BK","created_at":"2026-06-26T00:15:38Z"},{"alias_kind":"pith_short_8","alias_value":"AOZRM5TN","created_at":"2026-06-26T00:15:38Z"}],"graph_snapshots":[{"event_id":"sha256:43fd02bd6a32243c7c3c633ba920da62c870378d48f9b595e0f4a992c08016ac","target":"graph","created_at":"2026-06-26T00:15:38Z","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":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2606.26362/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Accurate prediction of pedestal height and width in tokamaks remains a critical issue as it strongly influences the predicted plasma performance of all future reactors. We present an integrated pedestal-stability workflow that combines equilibrium scans with magnetohydrodynamic (MHD) stability analysis using ELITE and GATO and gyrokinetic transport predictions using CGYRO/QLGYRO. The workflow reproduces the characteristic KBM first- and second-stability structure previously identified in gyrokinetic pedestal studies. Applied to spherical tokamaks (STs), the workflow shows good agreement with p","authors_text":"F. D. Halpern, J. Candy, J. McClenaghan, K. E. Thome, S. Saarelma, T. F. Neiser, the MAST-U team, T. H. Osborne","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2026-06-24T20:18:14Z","title":"Integrating Gyrokinetic Flux Predictions with Ideal MHD Stability Boundaries"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.26362","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:d1227fd8ca4e2b0f7038c441fc1265df0ee56906354c930a1903342f7c2817c3","target":"record","created_at":"2026-06-26T00:15:38Z","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":"9dee8bee5258e8aa53f9a68c30d5c45a043683018e08f882f1ba71e144d0bd00","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2026-06-24T20:18:14Z","title_canon_sha256":"fe318e5cbc449e9823d0913e7d3be111decf319c5167641ad685b0b4da4866ed"},"schema_version":"1.0","source":{"id":"2606.26362","kind":"arxiv","version":1}},"canonical_sha256":"03b316766de34cf66c2a748cca6d38d0555ba2e3e5eef48b779fb49363b5703a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"03b316766de34cf66c2a748cca6d38d0555ba2e3e5eef48b779fb49363b5703a","first_computed_at":"2026-06-26T00:15:38.004159Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-26T00:15:38.004159Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ep4K/0MkoV09AQOSbZHd6egCb9y1EHezi83cfNMQUZKJENYR/62AdP1k6mMU1PzpToaheWCHWBYUlZKfnG1/Bw==","signature_status":"signed_v1","signed_at":"2026-06-26T00:15:38.004564Z","signed_message":"canonical_sha256_bytes"},"source_id":"2606.26362","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d1227fd8ca4e2b0f7038c441fc1265df0ee56906354c930a1903342f7c2817c3","sha256:43fd02bd6a32243c7c3c633ba920da62c870378d48f9b595e0f4a992c08016ac"],"state_sha256":"47546e780123a150d7db5d671e2cf2e48043448ab64bfd1fa4d39a421379bee7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KjVPAd3fIM85UvpyZD9MtY6RQZ0e587qxbqGEJgBtDUrsO58HHA2HSpxulOzZ2woQef7/WerOF6fPTcqdzyrBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-26T18:47:12.320164Z","bundle_sha256":"f77802179ddf7817bb4ee9ec8c3f186edd1699620ad396ae978219a20e006928"}}