{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:26PW23VF4LJIDVBPLDIRPZNWPM","short_pith_number":"pith:26PW23VF","canonical_record":{"source":{"id":"1702.00644","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-02-02T12:33:11Z","cross_cats_sorted":[],"title_canon_sha256":"578a1f8f58c6bf42e1133045777abef4617b6d17865e6609030e89f480a24fe6","abstract_canon_sha256":"33cf310f78b20b0a55bbc2df2d3b8391a90185aa6d223749bc498c538c7c7502"},"schema_version":"1.0"},"canonical_sha256":"d79f6d6ea5e2d281d42f58d117e5b67b30fa7867ab869d24e8be971d56d59f25","source":{"kind":"arxiv","id":"1702.00644","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1702.00644","created_at":"2026-05-18T00:38:57Z"},{"alias_kind":"arxiv_version","alias_value":"1702.00644v3","created_at":"2026-05-18T00:38:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.00644","created_at":"2026-05-18T00:38:57Z"},{"alias_kind":"pith_short_12","alias_value":"26PW23VF4LJI","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_16","alias_value":"26PW23VF4LJIDVBP","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_8","alias_value":"26PW23VF","created_at":"2026-05-18T12:30:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:26PW23VF4LJIDVBPLDIRPZNWPM","target":"record","payload":{"canonical_record":{"source":{"id":"1702.00644","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-02-02T12:33:11Z","cross_cats_sorted":[],"title_canon_sha256":"578a1f8f58c6bf42e1133045777abef4617b6d17865e6609030e89f480a24fe6","abstract_canon_sha256":"33cf310f78b20b0a55bbc2df2d3b8391a90185aa6d223749bc498c538c7c7502"},"schema_version":"1.0"},"canonical_sha256":"d79f6d6ea5e2d281d42f58d117e5b67b30fa7867ab869d24e8be971d56d59f25","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:38:57.988223Z","signature_b64":"jYicPhgpXyDA4yNDPSzzR8yM/asP8sBSzp0Uxcb6BCCM1FVru75Gp5fuxb+CjIMa89Ze3hyTgQBTiU4iClI9Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d79f6d6ea5e2d281d42f58d117e5b67b30fa7867ab869d24e8be971d56d59f25","last_reissued_at":"2026-05-18T00:38:57.987731Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:38:57.987731Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1702.00644","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:38:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Obz7KdV62kNg9pzhSJKQaZMUVru2Ddn9ihOxW9O/2doi5TAGrhvh5JHqWvae5br9Ssp77YFI09LMNmGdhjIFDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T22:06:16.578475Z"},"content_sha256":"963aa2fa44303b38dd0773868ec4243c5e350d58c17f710dce4eba503441f175","schema_version":"1.0","event_id":"sha256:963aa2fa44303b38dd0773868ec4243c5e350d58c17f710dce4eba503441f175"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:26PW23VF4LJIDVBPLDIRPZNWPM","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Kinetic modeling of the electronic response of a dielectric plasma-facing solid","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Franz X. Bronold, Holger Fehske","submitted_at":"2017-02-02T12:33:11Z","abstract_excerpt":"We present a self-consistent kinetic theory for the electronic response of a plasma-facing dielectric solid. Based on the Poisson equation and two sets of spatially separated Boltzmann equations, one for electrons and ions in the plasma and one for conduction band electrons and valence band holes in the dielectric, the approach gives the quasi-stationary density and potential profiles of the electric double layer forming at the interface due to the permanent influx of electrons and ions from the plasma. The two sets of Boltzmann equations are connected by quantum-mechanical matching conditions"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.00644","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"2026-05-18T00:38:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+Qzu51sIU7cSjbzx/FA01m+8mXCH0lHsgxIW3pEKpZjda4Npy5IFDw9KscgFqmEAwHG6e3CJN+8A5O5aOa2FCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T22:06:16.579170Z"},"content_sha256":"fe38f69134fc279f22c131b11c67b098f57ff31c16c0a256fed8386c46ee7c46","schema_version":"1.0","event_id":"sha256:fe38f69134fc279f22c131b11c67b098f57ff31c16c0a256fed8386c46ee7c46"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/26PW23VF4LJIDVBPLDIRPZNWPM/bundle.json","state_url":"https://pith.science/pith/26PW23VF4LJIDVBPLDIRPZNWPM/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/26PW23VF4LJIDVBPLDIRPZNWPM/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":"2026-05-30T22:06:16Z","links":{"resolver":"https://pith.science/pith/26PW23VF4LJIDVBPLDIRPZNWPM","bundle":"https://pith.science/pith/26PW23VF4LJIDVBPLDIRPZNWPM/bundle.json","state":"https://pith.science/pith/26PW23VF4LJIDVBPLDIRPZNWPM/state.json","well_known_bundle":"https://pith.science/.well-known/pith/26PW23VF4LJIDVBPLDIRPZNWPM/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:26PW23VF4LJIDVBPLDIRPZNWPM","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":"33cf310f78b20b0a55bbc2df2d3b8391a90185aa6d223749bc498c538c7c7502","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-02-02T12:33:11Z","title_canon_sha256":"578a1f8f58c6bf42e1133045777abef4617b6d17865e6609030e89f480a24fe6"},"schema_version":"1.0","source":{"id":"1702.00644","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1702.00644","created_at":"2026-05-18T00:38:57Z"},{"alias_kind":"arxiv_version","alias_value":"1702.00644v3","created_at":"2026-05-18T00:38:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1702.00644","created_at":"2026-05-18T00:38:57Z"},{"alias_kind":"pith_short_12","alias_value":"26PW23VF4LJI","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_16","alias_value":"26PW23VF4LJIDVBP","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_8","alias_value":"26PW23VF","created_at":"2026-05-18T12:30:55Z"}],"graph_snapshots":[{"event_id":"sha256:fe38f69134fc279f22c131b11c67b098f57ff31c16c0a256fed8386c46ee7c46","target":"graph","created_at":"2026-05-18T00:38:57Z","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"},"paper":{"abstract_excerpt":"We present a self-consistent kinetic theory for the electronic response of a plasma-facing dielectric solid. Based on the Poisson equation and two sets of spatially separated Boltzmann equations, one for electrons and ions in the plasma and one for conduction band electrons and valence band holes in the dielectric, the approach gives the quasi-stationary density and potential profiles of the electric double layer forming at the interface due to the permanent influx of electrons and ions from the plasma. The two sets of Boltzmann equations are connected by quantum-mechanical matching conditions","authors_text":"Franz X. Bronold, Holger Fehske","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-02-02T12:33:11Z","title":"Kinetic modeling of the electronic response of a dielectric plasma-facing solid"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1702.00644","kind":"arxiv","version":3},"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":"sha256:963aa2fa44303b38dd0773868ec4243c5e350d58c17f710dce4eba503441f175","target":"record","created_at":"2026-05-18T00:38:57Z","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":"33cf310f78b20b0a55bbc2df2d3b8391a90185aa6d223749bc498c538c7c7502","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-02-02T12:33:11Z","title_canon_sha256":"578a1f8f58c6bf42e1133045777abef4617b6d17865e6609030e89f480a24fe6"},"schema_version":"1.0","source":{"id":"1702.00644","kind":"arxiv","version":3}},"canonical_sha256":"d79f6d6ea5e2d281d42f58d117e5b67b30fa7867ab869d24e8be971d56d59f25","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d79f6d6ea5e2d281d42f58d117e5b67b30fa7867ab869d24e8be971d56d59f25","first_computed_at":"2026-05-18T00:38:57.987731Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:38:57.987731Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"jYicPhgpXyDA4yNDPSzzR8yM/asP8sBSzp0Uxcb6BCCM1FVru75Gp5fuxb+CjIMa89Ze3hyTgQBTiU4iClI9Dg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:38:57.988223Z","signed_message":"canonical_sha256_bytes"},"source_id":"1702.00644","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:963aa2fa44303b38dd0773868ec4243c5e350d58c17f710dce4eba503441f175","sha256:fe38f69134fc279f22c131b11c67b098f57ff31c16c0a256fed8386c46ee7c46"],"state_sha256":"e9d411247ce882144ba8ed6cf7f75814fc77b2fa30156aa284b4b5875df58f9e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lYoAW1I9K16yACyNOxx4xXQIw2UTqNVVgjwovEATXh0uaPR4p1kFaEPbAtRUCUpI8mBTcIHDQ9j9oWzesuZPBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T22:06:16.582877Z","bundle_sha256":"a46fa36f8d1e167ae59d0b7c88bba309f358cacd61d18157bb5edd7ada819965"}}