{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:PFTJSDIRPDVB4RCKMNHSXK7TNY","short_pith_number":"pith:PFTJSDIR","canonical_record":{"source":{"id":"2511.04356","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-11-06T13:39:28Z","cross_cats_sorted":[],"title_canon_sha256":"e7d23673b0f20a55982f282e7d555c7d568a0f8c404cc76a9cc7c7018c7b1027","abstract_canon_sha256":"255460c0214dee508d03ea169a19c7be103c786110c302b405a243dbb2d9d0dd"},"schema_version":"1.0"},"canonical_sha256":"7966990d1178ea1e444a634f2babf36e16c995a259948bb86a2ba0967607158c","source":{"kind":"arxiv","id":"2511.04356","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2511.04356","created_at":"2026-05-25T02:02:10Z"},{"alias_kind":"arxiv_version","alias_value":"2511.04356v2","created_at":"2026-05-25T02:02:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2511.04356","created_at":"2026-05-25T02:02:10Z"},{"alias_kind":"pith_short_12","alias_value":"PFTJSDIRPDVB","created_at":"2026-05-25T02:02:10Z"},{"alias_kind":"pith_short_16","alias_value":"PFTJSDIRPDVB4RCK","created_at":"2026-05-25T02:02:10Z"},{"alias_kind":"pith_short_8","alias_value":"PFTJSDIR","created_at":"2026-05-25T02:02:10Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:PFTJSDIRPDVB4RCKMNHSXK7TNY","target":"record","payload":{"canonical_record":{"source":{"id":"2511.04356","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-11-06T13:39:28Z","cross_cats_sorted":[],"title_canon_sha256":"e7d23673b0f20a55982f282e7d555c7d568a0f8c404cc76a9cc7c7018c7b1027","abstract_canon_sha256":"255460c0214dee508d03ea169a19c7be103c786110c302b405a243dbb2d9d0dd"},"schema_version":"1.0"},"canonical_sha256":"7966990d1178ea1e444a634f2babf36e16c995a259948bb86a2ba0967607158c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-25T02:02:10.050863Z","signature_b64":"tUjeQjfjzJXJYwwzC68F7e3SGm+VRbKv3PjD2LoYzXQAKXKrt8KYMBlnMdhuBUDsfshXfV9f4T2kXrVNU8xEDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7966990d1178ea1e444a634f2babf36e16c995a259948bb86a2ba0967607158c","last_reissued_at":"2026-05-25T02:02:10.049870Z","signature_status":"signed_v1","first_computed_at":"2026-05-25T02:02:10.049870Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2511.04356","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":"2026-05-25T02:02:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"TOdiMqIzJn1kZhswxGp/a9KUe9SH2FEpkQj5mom2PgvXCuGpEYYpokKBMgMk+EfWcgRlHPlKd5o2gTkCkz1jCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T23:38:52.278167Z"},"content_sha256":"41f0163589ca3c27d69f067ed298180f19b710ae9e64981cd48bdbcf3c2d8312","schema_version":"1.0","event_id":"sha256:41f0163589ca3c27d69f067ed298180f19b710ae9e64981cd48bdbcf3c2d8312"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:PFTJSDIRPDVB4RCKMNHSXK7TNY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Stochastic simulation of partial discharge inception","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Jannis Teunissen, Yuting Gao","submitted_at":"2025-11-06T13:39:28Z","abstract_excerpt":"We present a Monte Carlo method for simulating the inception of electric discharges in gases. The input consists of an unstructured grid containing the electrostatic field. The output of the model is the estimated probability of discharge inception per initial electron position, as well as the estimated time lag between the appearance of the initial electron and discharge inception. To obtain these quantities electron avalanches are simulated for initial electron positions throughout the whole domain, also including regions below the critical electric field. Avalanches are assumed to propagate"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2511.04356","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/2511.04356/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":"2026-05-25T02:02:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IN/GAnXGa7fOdxoRxEFwZM2RATpGsYx/LomwMBpjukUIqu2dGJHvRkpuWX5DLqX53ahba1T+AJXY1EgLWN7hDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T23:38:52.278566Z"},"content_sha256":"b7f6844826809a72486dda37d866fcaab0eb7afe7ea81c00b0b7038aaef89940","schema_version":"1.0","event_id":"sha256:b7f6844826809a72486dda37d866fcaab0eb7afe7ea81c00b0b7038aaef89940"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PFTJSDIRPDVB4RCKMNHSXK7TNY/bundle.json","state_url":"https://pith.science/pith/PFTJSDIRPDVB4RCKMNHSXK7TNY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PFTJSDIRPDVB4RCKMNHSXK7TNY/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":"2026-05-29T23:38:52Z","links":{"resolver":"https://pith.science/pith/PFTJSDIRPDVB4RCKMNHSXK7TNY","bundle":"https://pith.science/pith/PFTJSDIRPDVB4RCKMNHSXK7TNY/bundle.json","state":"https://pith.science/pith/PFTJSDIRPDVB4RCKMNHSXK7TNY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PFTJSDIRPDVB4RCKMNHSXK7TNY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:PFTJSDIRPDVB4RCKMNHSXK7TNY","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":"255460c0214dee508d03ea169a19c7be103c786110c302b405a243dbb2d9d0dd","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-11-06T13:39:28Z","title_canon_sha256":"e7d23673b0f20a55982f282e7d555c7d568a0f8c404cc76a9cc7c7018c7b1027"},"schema_version":"1.0","source":{"id":"2511.04356","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2511.04356","created_at":"2026-05-25T02:02:10Z"},{"alias_kind":"arxiv_version","alias_value":"2511.04356v2","created_at":"2026-05-25T02:02:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2511.04356","created_at":"2026-05-25T02:02:10Z"},{"alias_kind":"pith_short_12","alias_value":"PFTJSDIRPDVB","created_at":"2026-05-25T02:02:10Z"},{"alias_kind":"pith_short_16","alias_value":"PFTJSDIRPDVB4RCK","created_at":"2026-05-25T02:02:10Z"},{"alias_kind":"pith_short_8","alias_value":"PFTJSDIR","created_at":"2026-05-25T02:02:10Z"}],"graph_snapshots":[{"event_id":"sha256:b7f6844826809a72486dda37d866fcaab0eb7afe7ea81c00b0b7038aaef89940","target":"graph","created_at":"2026-05-25T02:02:10Z","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/2511.04356/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present a Monte Carlo method for simulating the inception of electric discharges in gases. The input consists of an unstructured grid containing the electrostatic field. The output of the model is the estimated probability of discharge inception per initial electron position, as well as the estimated time lag between the appearance of the initial electron and discharge inception. To obtain these quantities electron avalanches are simulated for initial electron positions throughout the whole domain, also including regions below the critical electric field. Avalanches are assumed to propagate","authors_text":"Jannis Teunissen, Yuting Gao","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-11-06T13:39:28Z","title":"Stochastic simulation of partial discharge inception"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2511.04356","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":"sha256:41f0163589ca3c27d69f067ed298180f19b710ae9e64981cd48bdbcf3c2d8312","target":"record","created_at":"2026-05-25T02:02:10Z","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":"255460c0214dee508d03ea169a19c7be103c786110c302b405a243dbb2d9d0dd","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-11-06T13:39:28Z","title_canon_sha256":"e7d23673b0f20a55982f282e7d555c7d568a0f8c404cc76a9cc7c7018c7b1027"},"schema_version":"1.0","source":{"id":"2511.04356","kind":"arxiv","version":2}},"canonical_sha256":"7966990d1178ea1e444a634f2babf36e16c995a259948bb86a2ba0967607158c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7966990d1178ea1e444a634f2babf36e16c995a259948bb86a2ba0967607158c","first_computed_at":"2026-05-25T02:02:10.049870Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-25T02:02:10.049870Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"tUjeQjfjzJXJYwwzC68F7e3SGm+VRbKv3PjD2LoYzXQAKXKrt8KYMBlnMdhuBUDsfshXfV9f4T2kXrVNU8xEDw==","signature_status":"signed_v1","signed_at":"2026-05-25T02:02:10.050863Z","signed_message":"canonical_sha256_bytes"},"source_id":"2511.04356","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:41f0163589ca3c27d69f067ed298180f19b710ae9e64981cd48bdbcf3c2d8312","sha256:b7f6844826809a72486dda37d866fcaab0eb7afe7ea81c00b0b7038aaef89940"],"state_sha256":"e5b035c38d9acc9867d2ab8d64f5d4e606fac30e4713db5886a926ade117e8a7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GpcqFgCV/as1Zt1tmV/YEPv3CBpoSJZ+8riiWDEHdt14DvQaNqL3QdliolyNmkKwpPL6uyOFj/gsw2HN/ukCCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-29T23:38:52.281369Z","bundle_sha256":"8cc011535bcdd04e77dafd7b62e28d76c7425aac94df405c82655e9a5e21f5b8"}}