{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:AS2TNVCUYEOIMRY5WVXGT4K5MT","short_pith_number":"pith:AS2TNVCU","canonical_record":{"source":{"id":"2502.01811","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-02-03T20:41:10Z","cross_cats_sorted":["physics.space-ph"],"title_canon_sha256":"199dc7ae09186d6ede5d5fac528419af731cad0b839dd6787b7349957cc8d29b","abstract_canon_sha256":"5b3d1a57273de0a0a16a872d5274c31c2dd3faa3e65c975f2659dad1c871efe5"},"schema_version":"1.0"},"canonical_sha256":"04b536d454c11c86471db56e69f15d64d209cd206ccfc61109513ade488ac0bc","source":{"kind":"arxiv","id":"2502.01811","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2502.01811","created_at":"2026-07-05T10:09:19Z"},{"alias_kind":"arxiv_version","alias_value":"2502.01811v1","created_at":"2026-07-05T10:09:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.01811","created_at":"2026-07-05T10:09:19Z"},{"alias_kind":"pith_short_12","alias_value":"AS2TNVCUYEOI","created_at":"2026-07-05T10:09:19Z"},{"alias_kind":"pith_short_16","alias_value":"AS2TNVCUYEOIMRY5","created_at":"2026-07-05T10:09:19Z"},{"alias_kind":"pith_short_8","alias_value":"AS2TNVCU","created_at":"2026-07-05T10:09:19Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:AS2TNVCUYEOIMRY5WVXGT4K5MT","target":"record","payload":{"canonical_record":{"source":{"id":"2502.01811","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-02-03T20:41:10Z","cross_cats_sorted":["physics.space-ph"],"title_canon_sha256":"199dc7ae09186d6ede5d5fac528419af731cad0b839dd6787b7349957cc8d29b","abstract_canon_sha256":"5b3d1a57273de0a0a16a872d5274c31c2dd3faa3e65c975f2659dad1c871efe5"},"schema_version":"1.0"},"canonical_sha256":"04b536d454c11c86471db56e69f15d64d209cd206ccfc61109513ade488ac0bc","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:09:19.642659Z","signature_b64":"tG+XLhO6hFysP8dy8bCTaIYb2g0lfbPk+i3y2hxpcGEA6nIcI/e6ksQzGzWvTnpv76mbUj+xu7LZ6hp5RgsXCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"04b536d454c11c86471db56e69f15d64d209cd206ccfc61109513ade488ac0bc","last_reissued_at":"2026-07-05T10:09:19.642128Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:09:19.642128Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2502.01811","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":"2026-07-05T10:09:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"c31lnFifaSeyXmOvRh6kyUHAxzm1WRFjjT1P2wuVObgeCU9m5oOj4bPlHQr0KwIDGdfPnG19cGpELFhEyuAcBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T10:37:02.033656Z"},"content_sha256":"cb473504a3d80a80cd891c50045baf8e63f62279175824975dcfc0190092e497","schema_version":"1.0","event_id":"sha256:cb473504a3d80a80cd891c50045baf8e63f62279175824975dcfc0190092e497"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:AS2TNVCUYEOIMRY5WVXGT4K5MT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Computing the generalized plasma dispersion function for non-Maxwellian plasmas, with applications to Thomson scattering","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.space-ph"],"primary_cat":"physics.plasm-ph","authors_text":"Chirag R. Skolar, Lindsay V. Goodwin, William J. Longley","submitted_at":"2025-02-03T20:41:10Z","abstract_excerpt":"Kinetic plasma studies often require computing integrals of the velocity distribution over a complex-valued pole. The standard method is to solve the integral in the complex plane using the Plemelj theorem, resulting in the standard plasma dispersion function for Maxwellian plasmas. For non-Maxwellian plasmas, the Plemelj theorem does not generalize to an analytic form, and computational methods must be used. In this paper, a new computational method is developed to accurately integrate a non-Maxwellian velocity distribution over an arbitrary set of complex valued poles. This method works by k"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.01811","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/2502.01811/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":"2026-07-05T10:09:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hbkCztkmYevtc4aevzsuTi/GKySONdDIl4hdg+hh009ONjqROifSNjuwVXnJIY59hRH58zzlj5SH01MrDAcDAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T10:37:02.034130Z"},"content_sha256":"ddb637c1e7012a6395497ab6fadeaee4794121a36f548aa9e19d6f4dbb8a4ab3","schema_version":"1.0","event_id":"sha256:ddb637c1e7012a6395497ab6fadeaee4794121a36f548aa9e19d6f4dbb8a4ab3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/AS2TNVCUYEOIMRY5WVXGT4K5MT/bundle.json","state_url":"https://pith.science/pith/AS2TNVCUYEOIMRY5WVXGT4K5MT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/AS2TNVCUYEOIMRY5WVXGT4K5MT/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":"2026-08-11T10:37:02Z","links":{"resolver":"https://pith.science/pith/AS2TNVCUYEOIMRY5WVXGT4K5MT","bundle":"https://pith.science/pith/AS2TNVCUYEOIMRY5WVXGT4K5MT/bundle.json","state":"https://pith.science/pith/AS2TNVCUYEOIMRY5WVXGT4K5MT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/AS2TNVCUYEOIMRY5WVXGT4K5MT/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:AS2TNVCUYEOIMRY5WVXGT4K5MT","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":"5b3d1a57273de0a0a16a872d5274c31c2dd3faa3e65c975f2659dad1c871efe5","cross_cats_sorted":["physics.space-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-02-03T20:41:10Z","title_canon_sha256":"199dc7ae09186d6ede5d5fac528419af731cad0b839dd6787b7349957cc8d29b"},"schema_version":"1.0","source":{"id":"2502.01811","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2502.01811","created_at":"2026-07-05T10:09:19Z"},{"alias_kind":"arxiv_version","alias_value":"2502.01811v1","created_at":"2026-07-05T10:09:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.01811","created_at":"2026-07-05T10:09:19Z"},{"alias_kind":"pith_short_12","alias_value":"AS2TNVCUYEOI","created_at":"2026-07-05T10:09:19Z"},{"alias_kind":"pith_short_16","alias_value":"AS2TNVCUYEOIMRY5","created_at":"2026-07-05T10:09:19Z"},{"alias_kind":"pith_short_8","alias_value":"AS2TNVCU","created_at":"2026-07-05T10:09:19Z"}],"graph_snapshots":[{"event_id":"sha256:ddb637c1e7012a6395497ab6fadeaee4794121a36f548aa9e19d6f4dbb8a4ab3","target":"graph","created_at":"2026-07-05T10:09:19Z","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/2502.01811/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Kinetic plasma studies often require computing integrals of the velocity distribution over a complex-valued pole. The standard method is to solve the integral in the complex plane using the Plemelj theorem, resulting in the standard plasma dispersion function for Maxwellian plasmas. For non-Maxwellian plasmas, the Plemelj theorem does not generalize to an analytic form, and computational methods must be used. In this paper, a new computational method is developed to accurately integrate a non-Maxwellian velocity distribution over an arbitrary set of complex valued poles. This method works by k","authors_text":"Chirag R. Skolar, Lindsay V. Goodwin, William J. Longley","cross_cats":["physics.space-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-02-03T20:41:10Z","title":"Computing the generalized plasma dispersion function for non-Maxwellian plasmas, with applications to Thomson scattering"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.01811","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:cb473504a3d80a80cd891c50045baf8e63f62279175824975dcfc0190092e497","target":"record","created_at":"2026-07-05T10:09:19Z","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":"5b3d1a57273de0a0a16a872d5274c31c2dd3faa3e65c975f2659dad1c871efe5","cross_cats_sorted":["physics.space-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-02-03T20:41:10Z","title_canon_sha256":"199dc7ae09186d6ede5d5fac528419af731cad0b839dd6787b7349957cc8d29b"},"schema_version":"1.0","source":{"id":"2502.01811","kind":"arxiv","version":1}},"canonical_sha256":"04b536d454c11c86471db56e69f15d64d209cd206ccfc61109513ade488ac0bc","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"04b536d454c11c86471db56e69f15d64d209cd206ccfc61109513ade488ac0bc","first_computed_at":"2026-07-05T10:09:19.642128Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:09:19.642128Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"tG+XLhO6hFysP8dy8bCTaIYb2g0lfbPk+i3y2hxpcGEA6nIcI/e6ksQzGzWvTnpv76mbUj+xu7LZ6hp5RgsXCg==","signature_status":"signed_v1","signed_at":"2026-07-05T10:09:19.642659Z","signed_message":"canonical_sha256_bytes"},"source_id":"2502.01811","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cb473504a3d80a80cd891c50045baf8e63f62279175824975dcfc0190092e497","sha256:ddb637c1e7012a6395497ab6fadeaee4794121a36f548aa9e19d6f4dbb8a4ab3"],"state_sha256":"eed398bd9cc2fa41fe326647e34f52697c847ba6c625e1e32e4ff3bfd3dfcd1f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"63Ec0rHmNvOzJsLsK/9AJ4724NGHH6KBKNvESqhU2GazAyofEfsPjzK55gZwAaZraBdysy8k7z5ITZKQVs3WDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-11T10:37:02.038458Z","bundle_sha256":"5c99dfd553bb284d04b47acd1fac97fdf5f800abcad1fa41903d37d87bdb9754"}}