{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2019:56UMMM7YBR53ZZBUOXJ65ZWTSW","short_pith_number":"pith:56UMMM7Y","canonical_record":{"source":{"id":"1906.08883","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2019-06-20T22:35:06Z","cross_cats_sorted":[],"title_canon_sha256":"5917251e216687d1f51c2bde4e924b934a2d7f4753095812219c5818183cac76","abstract_canon_sha256":"321f12140c81675e8e841c3f9889ff567112c38e883481142bb54f3583e0dfd8"},"schema_version":"1.0"},"canonical_sha256":"efa8c633f80c7bbce43475d3eee6d395907a88be323171c7f8a3847c8452b3b3","source":{"kind":"arxiv","id":"1906.08883","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1906.08883","created_at":"2026-05-17T23:41:07Z"},{"alias_kind":"arxiv_version","alias_value":"1906.08883v2","created_at":"2026-05-17T23:41:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1906.08883","created_at":"2026-05-17T23:41:07Z"},{"alias_kind":"pith_short_12","alias_value":"56UMMM7YBR53","created_at":"2026-05-18T12:33:10Z"},{"alias_kind":"pith_short_16","alias_value":"56UMMM7YBR53ZZBU","created_at":"2026-05-18T12:33:10Z"},{"alias_kind":"pith_short_8","alias_value":"56UMMM7Y","created_at":"2026-05-18T12:33:10Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2019:56UMMM7YBR53ZZBUOXJ65ZWTSW","target":"record","payload":{"canonical_record":{"source":{"id":"1906.08883","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2019-06-20T22:35:06Z","cross_cats_sorted":[],"title_canon_sha256":"5917251e216687d1f51c2bde4e924b934a2d7f4753095812219c5818183cac76","abstract_canon_sha256":"321f12140c81675e8e841c3f9889ff567112c38e883481142bb54f3583e0dfd8"},"schema_version":"1.0"},"canonical_sha256":"efa8c633f80c7bbce43475d3eee6d395907a88be323171c7f8a3847c8452b3b3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:41:07.559772Z","signature_b64":"0hzSQvPbtjRHVy4zyriye1SCC+oz5wFXpafl+YB9cHvDH23XM3QfXprBc2PXwXw0+eoMjrZHfsCoW8Ij0LrkBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"efa8c633f80c7bbce43475d3eee6d395907a88be323171c7f8a3847c8452b3b3","last_reissued_at":"2026-05-17T23:41:07.559014Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:41:07.559014Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1906.08883","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":"2026-05-17T23:41:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BGE/NE5O5/xnnL8hMRgrRGOlQiEww697L6dm43EdiaIr6l9F+2wJCQTxq6pfflmV+t+Nb6dy5nONwrj/V7UQAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T19:35:08.773607Z"},"content_sha256":"622cebeb34a14fb98eaed9d41c48d1ffd1f2a5db26e8d18e7c644ff10670c84d","schema_version":"1.0","event_id":"sha256:622cebeb34a14fb98eaed9d41c48d1ffd1f2a5db26e8d18e7c644ff10670c84d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2019:56UMMM7YBR53ZZBUOXJ65ZWTSW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Influence of atomic kinetics on inverse Bremsstrahlung heating and non-local thermal transport","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"H. A. Scott, H. P. Le, M. Sherlock","submitted_at":"2019-06-20T22:35:06Z","abstract_excerpt":"This paper describes a computational model that self-consistently combines physics of kinetic electrons and atomic processes in a single framework. The formulation consists of a kinetic Vlasov- Boltzmann-Fokker-Planck equation for free electrons and a non-Maxwellian collisional-radiative model for atomic state populations. We utilize this model to examine the influence of atomic kinetics on inverse Bremsstrahlung (IB) heating and non-local thermal transport. We show that atomic kinetics affects non-linear IB absorption rates by further modifying the electron distribution in addition to laser h"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1906.08883","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":""},"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":"2026-05-17T23:41:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Yzk9nWA7VbE2pQKPfl6Ci0wlkDC0uXCFB/U5XOMrb2gPvh/dcBuss6s2OYdXUkbeLFS88KAtILaDIoSJGKjlBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T19:35:08.773976Z"},"content_sha256":"dc276956166d84e3ef868735b0a707de02f4e4a409e812fa6387b7cba5ff6d59","schema_version":"1.0","event_id":"sha256:dc276956166d84e3ef868735b0a707de02f4e4a409e812fa6387b7cba5ff6d59"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/56UMMM7YBR53ZZBUOXJ65ZWTSW/bundle.json","state_url":"https://pith.science/pith/56UMMM7YBR53ZZBUOXJ65ZWTSW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/56UMMM7YBR53ZZBUOXJ65ZWTSW/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":"2026-05-26T19:35:08Z","links":{"resolver":"https://pith.science/pith/56UMMM7YBR53ZZBUOXJ65ZWTSW","bundle":"https://pith.science/pith/56UMMM7YBR53ZZBUOXJ65ZWTSW/bundle.json","state":"https://pith.science/pith/56UMMM7YBR53ZZBUOXJ65ZWTSW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/56UMMM7YBR53ZZBUOXJ65ZWTSW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:56UMMM7YBR53ZZBUOXJ65ZWTSW","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":"321f12140c81675e8e841c3f9889ff567112c38e883481142bb54f3583e0dfd8","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2019-06-20T22:35:06Z","title_canon_sha256":"5917251e216687d1f51c2bde4e924b934a2d7f4753095812219c5818183cac76"},"schema_version":"1.0","source":{"id":"1906.08883","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1906.08883","created_at":"2026-05-17T23:41:07Z"},{"alias_kind":"arxiv_version","alias_value":"1906.08883v2","created_at":"2026-05-17T23:41:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1906.08883","created_at":"2026-05-17T23:41:07Z"},{"alias_kind":"pith_short_12","alias_value":"56UMMM7YBR53","created_at":"2026-05-18T12:33:10Z"},{"alias_kind":"pith_short_16","alias_value":"56UMMM7YBR53ZZBU","created_at":"2026-05-18T12:33:10Z"},{"alias_kind":"pith_short_8","alias_value":"56UMMM7Y","created_at":"2026-05-18T12:33:10Z"}],"graph_snapshots":[{"event_id":"sha256:dc276956166d84e3ef868735b0a707de02f4e4a409e812fa6387b7cba5ff6d59","target":"graph","created_at":"2026-05-17T23:41:07Z","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":"This paper describes a computational model that self-consistently combines physics of kinetic electrons and atomic processes in a single framework. The formulation consists of a kinetic Vlasov- Boltzmann-Fokker-Planck equation for free electrons and a non-Maxwellian collisional-radiative model for atomic state populations. We utilize this model to examine the influence of atomic kinetics on inverse Bremsstrahlung (IB) heating and non-local thermal transport. We show that atomic kinetics affects non-linear IB absorption rates by further modifying the electron distribution in addition to laser h","authors_text":"H. A. Scott, H. P. Le, M. Sherlock","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2019-06-20T22:35:06Z","title":"Influence of atomic kinetics on inverse Bremsstrahlung heating and non-local thermal transport"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1906.08883","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":"sha256:622cebeb34a14fb98eaed9d41c48d1ffd1f2a5db26e8d18e7c644ff10670c84d","target":"record","created_at":"2026-05-17T23:41:07Z","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":"321f12140c81675e8e841c3f9889ff567112c38e883481142bb54f3583e0dfd8","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2019-06-20T22:35:06Z","title_canon_sha256":"5917251e216687d1f51c2bde4e924b934a2d7f4753095812219c5818183cac76"},"schema_version":"1.0","source":{"id":"1906.08883","kind":"arxiv","version":2}},"canonical_sha256":"efa8c633f80c7bbce43475d3eee6d395907a88be323171c7f8a3847c8452b3b3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"efa8c633f80c7bbce43475d3eee6d395907a88be323171c7f8a3847c8452b3b3","first_computed_at":"2026-05-17T23:41:07.559014Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:41:07.559014Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"0hzSQvPbtjRHVy4zyriye1SCC+oz5wFXpafl+YB9cHvDH23XM3QfXprBc2PXwXw0+eoMjrZHfsCoW8Ij0LrkBQ==","signature_status":"signed_v1","signed_at":"2026-05-17T23:41:07.559772Z","signed_message":"canonical_sha256_bytes"},"source_id":"1906.08883","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:622cebeb34a14fb98eaed9d41c48d1ffd1f2a5db26e8d18e7c644ff10670c84d","sha256:dc276956166d84e3ef868735b0a707de02f4e4a409e812fa6387b7cba5ff6d59"],"state_sha256":"820ae96a1202f1461192e12d7929d25747f3ea22a25047c98f2a8e522bb756cb"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LDPzwpKIlJx+8Os2alMszbeMwsu0vpCrsU3HUTFq/oF4EHCXcJ4tkK++nXXw8tI62JY9Xe7mgIPOm9KCs+fkCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T19:35:08.776883Z","bundle_sha256":"e222c2b704d04238903139d2f97f868206a21013489d49d7f84e4e4955aeab1b"}}