{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:JKN7I4IS3D5M5ZEKL7KO6UH5VV","short_pith_number":"pith:JKN7I4IS","canonical_record":{"source":{"id":"2210.09590","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2022-10-18T05:05:51Z","cross_cats_sorted":[],"title_canon_sha256":"01f1fe3fe00f8922bc9c9c495f73c1aadbb3526f24411bec66bb7068fe50d1b7","abstract_canon_sha256":"8a5c9ab6f7fbf38b110756efff8e8fa17daf62fc03c01abfc3cb47182da1df75"},"schema_version":"1.0"},"canonical_sha256":"4a9bf47112d8facee48a5fd4ef50fdad7c13401ab28a803c718356a54ad00913","source":{"kind":"arxiv","id":"2210.09590","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2210.09590","created_at":"2026-07-05T05:48:02Z"},{"alias_kind":"arxiv_version","alias_value":"2210.09590v2","created_at":"2026-07-05T05:48:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2210.09590","created_at":"2026-07-05T05:48:02Z"},{"alias_kind":"pith_short_12","alias_value":"JKN7I4IS3D5M","created_at":"2026-07-05T05:48:02Z"},{"alias_kind":"pith_short_16","alias_value":"JKN7I4IS3D5M5ZEK","created_at":"2026-07-05T05:48:02Z"},{"alias_kind":"pith_short_8","alias_value":"JKN7I4IS","created_at":"2026-07-05T05:48:02Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:JKN7I4IS3D5M5ZEKL7KO6UH5VV","target":"record","payload":{"canonical_record":{"source":{"id":"2210.09590","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2022-10-18T05:05:51Z","cross_cats_sorted":[],"title_canon_sha256":"01f1fe3fe00f8922bc9c9c495f73c1aadbb3526f24411bec66bb7068fe50d1b7","abstract_canon_sha256":"8a5c9ab6f7fbf38b110756efff8e8fa17daf62fc03c01abfc3cb47182da1df75"},"schema_version":"1.0"},"canonical_sha256":"4a9bf47112d8facee48a5fd4ef50fdad7c13401ab28a803c718356a54ad00913","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:48:02.404163Z","signature_b64":"FX+3wOQ8zF9fMPpGA8nqMslZ+3F5YwNN7c4++cp6/W4oEl6/W61WKmMmqOiBU9fFMmD9BE4q40ikjuVHMiTsAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4a9bf47112d8facee48a5fd4ef50fdad7c13401ab28a803c718356a54ad00913","last_reissued_at":"2026-07-05T05:48:02.403724Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:48:02.403724Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2210.09590","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":"2026-07-05T05:48:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fhsAYhFTnD2jIIlFZg4zo16AqKF+B4WFUAnrfH5d/6FXwVi3ECwOO82LauC68UA4hAaurumgeHMMqPnld7QEAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-23T19:53:33.269990Z"},"content_sha256":"c38fb0aa79b2676fbef943e0bf999f77ea479447d3e2017ccfea55db19bedfe4","schema_version":"1.0","event_id":"sha256:c38fb0aa79b2676fbef943e0bf999f77ea479447d3e2017ccfea55db19bedfe4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:JKN7I4IS3D5M5ZEKL7KO6UH5VV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Neutrino magnetohydrodynamic instabilities in presence of two-flavor oscillations","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"A. P. Misra, D. Chatterjee, S. Ghosh","submitted_at":"2022-10-18T05:05:51Z","abstract_excerpt":"The influence of neutrino flavor oscillations on the propagation of magnetohydrodynamic (MHD) waves and instabilities is studied in neutrino-beam driven magnetoplasmas. Using the neutrino MHD model, a general dispersion relation is derived which manifests the resonant interactions of MHD waves, not only with the neutrino beam, but also with the neutrino flavor oscillations. It is found that the latter contribute to the wave dispersion and enhance the magnitude of the instability of oblique magnetosonic waves. However, the shear-Alfv{\\'e}n wave remains unaffected by the neutrino beam and neutri"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2210.09590","kind":"arxiv","version":2},"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/2210.09590/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":"2026-07-05T05:48:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ARAB0sG4hCCKB4DM6TJOnWWR9RNG5yTI0SmVAcFafRkIrNVYe84ob8cq+eQk8ih07V8vTZmpgUs5SJzTzkjWBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-23T19:53:33.270638Z"},"content_sha256":"62b1fb2c66b4ce7f6b46cc75d37f0190f3252a4f715673070f6809352ed960f1","schema_version":"1.0","event_id":"sha256:62b1fb2c66b4ce7f6b46cc75d37f0190f3252a4f715673070f6809352ed960f1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JKN7I4IS3D5M5ZEKL7KO6UH5VV/bundle.json","state_url":"https://pith.science/pith/JKN7I4IS3D5M5ZEKL7KO6UH5VV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JKN7I4IS3D5M5ZEKL7KO6UH5VV/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":"2026-08-23T19:53:33Z","links":{"resolver":"https://pith.science/pith/JKN7I4IS3D5M5ZEKL7KO6UH5VV","bundle":"https://pith.science/pith/JKN7I4IS3D5M5ZEKL7KO6UH5VV/bundle.json","state":"https://pith.science/pith/JKN7I4IS3D5M5ZEKL7KO6UH5VV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JKN7I4IS3D5M5ZEKL7KO6UH5VV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:JKN7I4IS3D5M5ZEKL7KO6UH5VV","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":"8a5c9ab6f7fbf38b110756efff8e8fa17daf62fc03c01abfc3cb47182da1df75","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2022-10-18T05:05:51Z","title_canon_sha256":"01f1fe3fe00f8922bc9c9c495f73c1aadbb3526f24411bec66bb7068fe50d1b7"},"schema_version":"1.0","source":{"id":"2210.09590","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2210.09590","created_at":"2026-07-05T05:48:02Z"},{"alias_kind":"arxiv_version","alias_value":"2210.09590v2","created_at":"2026-07-05T05:48:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2210.09590","created_at":"2026-07-05T05:48:02Z"},{"alias_kind":"pith_short_12","alias_value":"JKN7I4IS3D5M","created_at":"2026-07-05T05:48:02Z"},{"alias_kind":"pith_short_16","alias_value":"JKN7I4IS3D5M5ZEK","created_at":"2026-07-05T05:48:02Z"},{"alias_kind":"pith_short_8","alias_value":"JKN7I4IS","created_at":"2026-07-05T05:48:02Z"}],"graph_snapshots":[{"event_id":"sha256:62b1fb2c66b4ce7f6b46cc75d37f0190f3252a4f715673070f6809352ed960f1","target":"graph","created_at":"2026-07-05T05:48:02Z","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/2210.09590/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The influence of neutrino flavor oscillations on the propagation of magnetohydrodynamic (MHD) waves and instabilities is studied in neutrino-beam driven magnetoplasmas. Using the neutrino MHD model, a general dispersion relation is derived which manifests the resonant interactions of MHD waves, not only with the neutrino beam, but also with the neutrino flavor oscillations. It is found that the latter contribute to the wave dispersion and enhance the magnitude of the instability of oblique magnetosonic waves. However, the shear-Alfv{\\'e}n wave remains unaffected by the neutrino beam and neutri","authors_text":"A. P. Misra, D. Chatterjee, S. Ghosh","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2022-10-18T05:05:51Z","title":"Neutrino magnetohydrodynamic instabilities in presence of two-flavor oscillations"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2210.09590","kind":"arxiv","version":2},"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:c38fb0aa79b2676fbef943e0bf999f77ea479447d3e2017ccfea55db19bedfe4","target":"record","created_at":"2026-07-05T05:48:02Z","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":"8a5c9ab6f7fbf38b110756efff8e8fa17daf62fc03c01abfc3cb47182da1df75","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2022-10-18T05:05:51Z","title_canon_sha256":"01f1fe3fe00f8922bc9c9c495f73c1aadbb3526f24411bec66bb7068fe50d1b7"},"schema_version":"1.0","source":{"id":"2210.09590","kind":"arxiv","version":2}},"canonical_sha256":"4a9bf47112d8facee48a5fd4ef50fdad7c13401ab28a803c718356a54ad00913","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4a9bf47112d8facee48a5fd4ef50fdad7c13401ab28a803c718356a54ad00913","first_computed_at":"2026-07-05T05:48:02.403724Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:48:02.403724Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"FX+3wOQ8zF9fMPpGA8nqMslZ+3F5YwNN7c4++cp6/W4oEl6/W61WKmMmqOiBU9fFMmD9BE4q40ikjuVHMiTsAA==","signature_status":"signed_v1","signed_at":"2026-07-05T05:48:02.404163Z","signed_message":"canonical_sha256_bytes"},"source_id":"2210.09590","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c38fb0aa79b2676fbef943e0bf999f77ea479447d3e2017ccfea55db19bedfe4","sha256:62b1fb2c66b4ce7f6b46cc75d37f0190f3252a4f715673070f6809352ed960f1"],"state_sha256":"e51705f631e2f00af83b02b7e3eb97ea88534536e4345fff8941c47cbd5b0dcf"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"EClWChDs495FccuvNll0zunVMbJTMfmzQzTFGm/1T8j2X9xbr7aKj3YjCWTv9bQG64AhAnORMm+SP373OsvsAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-23T19:53:33.276248Z","bundle_sha256":"d2dd9e258bc776ac03b6b4c056e25dcf664e00cdab5503203cbc6dc6326fa636"}}