{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:6A4N4EOI52QD2IJSMYJ5YGUT33","short_pith_number":"pith:6A4N4EOI","canonical_record":{"source":{"id":"1604.08165","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2016-04-27T18:23:40Z","cross_cats_sorted":["physics.comp-ph"],"title_canon_sha256":"b630dd31eb24a35f7d32c7d98d7e1c3205882e17586904ecc658dc8b01861166","abstract_canon_sha256":"0ef5e96c89b742c9a15f3c9e6f96ba39d57b4719400c22f784a4faea360f56b3"},"schema_version":"1.0"},"canonical_sha256":"f038de11c8eea03d21326613dc1a93ded76b757ae6119056cc3e83c65cb0f655","source":{"kind":"arxiv","id":"1604.08165","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.08165","created_at":"2026-05-18T01:00:35Z"},{"alias_kind":"arxiv_version","alias_value":"1604.08165v2","created_at":"2026-05-18T01:00:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.08165","created_at":"2026-05-18T01:00:35Z"},{"alias_kind":"pith_short_12","alias_value":"6A4N4EOI52QD","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_16","alias_value":"6A4N4EOI52QD2IJS","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_8","alias_value":"6A4N4EOI","created_at":"2026-05-18T12:30:01Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:6A4N4EOI52QD2IJSMYJ5YGUT33","target":"record","payload":{"canonical_record":{"source":{"id":"1604.08165","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2016-04-27T18:23:40Z","cross_cats_sorted":["physics.comp-ph"],"title_canon_sha256":"b630dd31eb24a35f7d32c7d98d7e1c3205882e17586904ecc658dc8b01861166","abstract_canon_sha256":"0ef5e96c89b742c9a15f3c9e6f96ba39d57b4719400c22f784a4faea360f56b3"},"schema_version":"1.0"},"canonical_sha256":"f038de11c8eea03d21326613dc1a93ded76b757ae6119056cc3e83c65cb0f655","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:00:35.314710Z","signature_b64":"4JGELkGm0nyDYUd4twmWmTS7z8LWSuC+hiYhW7PJYlnzWkQcplmt86T7eKH/OyD07gin5UyJJUjI+mkqb8x0BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f038de11c8eea03d21326613dc1a93ded76b757ae6119056cc3e83c65cb0f655","last_reissued_at":"2026-05-18T01:00:35.313901Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:00:35.313901Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1604.08165","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":"2026-05-18T01:00:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BI3RMdj1I+iKXE24f+WB82nIJkQtIpBclrwJnpx/ZfunLRUFcOcN/Svia9w9Xw1sfmhRUOoJOVPp8qRqkUCZCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-26T00:50:27.343752Z"},"content_sha256":"3a267af914402fd8d161b6ce05f1e1c32cf55bdf81e2c8812dcd8697a8176615","schema_version":"1.0","event_id":"sha256:3a267af914402fd8d161b6ce05f1e1c32cf55bdf81e2c8812dcd8697a8176615"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:6A4N4EOI52QD2IJSMYJ5YGUT33","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Numerical solution of the quantum Lenard-Balescu equation for a one-component plasma","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.comp-ph"],"primary_cat":"physics.plasm-ph","authors_text":"Andrew P. Belt, Christian R. Scullard, Frank R. Graziani, Marija R. Jankovi\\'c, Nathan Ng, Susana Serna, Susan C. Fennell","submitted_at":"2016-04-27T18:23:40Z","abstract_excerpt":"We present a numerical solution of the quantum Lenard-Balescu equation using a spectral method, namely an expansion in Laguerre polynomials. This method exactly conserves both particles and energy and facilitates the integration over the dielectric function. To demonstrate the method, we solve the equilibration problem for a spatially homogeneous one-component plasma with various initial conditions. Unlike the more usual Landau/Fokker-Planck system, this method requires no input Coulomb logarithm; the logarithmic terms in the collision integral arise naturally from the equation along with the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.08165","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":"2026-05-18T01:00:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dePoos58LxHAgM9X2Ct06P7NjPaJepLt+1U4GmM/7cgduHHwMBv9HRZhjpE22ca+0C5RehhBiRcqTrEXdsIPAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-26T00:50:27.344112Z"},"content_sha256":"0639a24021b81d5f7b8075609517c9403eb4c29c84c82a942b3fd7dd257eba6c","schema_version":"1.0","event_id":"sha256:0639a24021b81d5f7b8075609517c9403eb4c29c84c82a942b3fd7dd257eba6c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6A4N4EOI52QD2IJSMYJ5YGUT33/bundle.json","state_url":"https://pith.science/pith/6A4N4EOI52QD2IJSMYJ5YGUT33/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6A4N4EOI52QD2IJSMYJ5YGUT33/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":"2026-06-26T00:50:27Z","links":{"resolver":"https://pith.science/pith/6A4N4EOI52QD2IJSMYJ5YGUT33","bundle":"https://pith.science/pith/6A4N4EOI52QD2IJSMYJ5YGUT33/bundle.json","state":"https://pith.science/pith/6A4N4EOI52QD2IJSMYJ5YGUT33/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6A4N4EOI52QD2IJSMYJ5YGUT33/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:6A4N4EOI52QD2IJSMYJ5YGUT33","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":"0ef5e96c89b742c9a15f3c9e6f96ba39d57b4719400c22f784a4faea360f56b3","cross_cats_sorted":["physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2016-04-27T18:23:40Z","title_canon_sha256":"b630dd31eb24a35f7d32c7d98d7e1c3205882e17586904ecc658dc8b01861166"},"schema_version":"1.0","source":{"id":"1604.08165","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.08165","created_at":"2026-05-18T01:00:35Z"},{"alias_kind":"arxiv_version","alias_value":"1604.08165v2","created_at":"2026-05-18T01:00:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.08165","created_at":"2026-05-18T01:00:35Z"},{"alias_kind":"pith_short_12","alias_value":"6A4N4EOI52QD","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_16","alias_value":"6A4N4EOI52QD2IJS","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_8","alias_value":"6A4N4EOI","created_at":"2026-05-18T12:30:01Z"}],"graph_snapshots":[{"event_id":"sha256:0639a24021b81d5f7b8075609517c9403eb4c29c84c82a942b3fd7dd257eba6c","target":"graph","created_at":"2026-05-18T01:00:35Z","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 numerical solution of the quantum Lenard-Balescu equation using a spectral method, namely an expansion in Laguerre polynomials. This method exactly conserves both particles and energy and facilitates the integration over the dielectric function. To demonstrate the method, we solve the equilibration problem for a spatially homogeneous one-component plasma with various initial conditions. Unlike the more usual Landau/Fokker-Planck system, this method requires no input Coulomb logarithm; the logarithmic terms in the collision integral arise naturally from the equation along with the ","authors_text":"Andrew P. Belt, Christian R. Scullard, Frank R. Graziani, Marija R. Jankovi\\'c, Nathan Ng, Susana Serna, Susan C. Fennell","cross_cats":["physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2016-04-27T18:23:40Z","title":"Numerical solution of the quantum Lenard-Balescu equation for a one-component plasma"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.08165","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":"sha256:3a267af914402fd8d161b6ce05f1e1c32cf55bdf81e2c8812dcd8697a8176615","target":"record","created_at":"2026-05-18T01:00:35Z","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":"0ef5e96c89b742c9a15f3c9e6f96ba39d57b4719400c22f784a4faea360f56b3","cross_cats_sorted":["physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2016-04-27T18:23:40Z","title_canon_sha256":"b630dd31eb24a35f7d32c7d98d7e1c3205882e17586904ecc658dc8b01861166"},"schema_version":"1.0","source":{"id":"1604.08165","kind":"arxiv","version":2}},"canonical_sha256":"f038de11c8eea03d21326613dc1a93ded76b757ae6119056cc3e83c65cb0f655","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f038de11c8eea03d21326613dc1a93ded76b757ae6119056cc3e83c65cb0f655","first_computed_at":"2026-05-18T01:00:35.313901Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:00:35.313901Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4JGELkGm0nyDYUd4twmWmTS7z8LWSuC+hiYhW7PJYlnzWkQcplmt86T7eKH/OyD07gin5UyJJUjI+mkqb8x0BQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:00:35.314710Z","signed_message":"canonical_sha256_bytes"},"source_id":"1604.08165","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3a267af914402fd8d161b6ce05f1e1c32cf55bdf81e2c8812dcd8697a8176615","sha256:0639a24021b81d5f7b8075609517c9403eb4c29c84c82a942b3fd7dd257eba6c"],"state_sha256":"247b92d2492fd773ea791a9b2c9b4f72504e0175a187c7bc58e0d15af23950a7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GLjhJPfbPZfch0VKWqeL5R3LhT4wt7jQFmYzqQtdZjlYmQkWOGMEFxlbzxHe08haMkUmHF5S8fWzktUDF/dCAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-26T00:50:27.346111Z","bundle_sha256":"d64813ad522a3b19495c21dcbd0d4e289e769351ab772ec781d70c01af9cc1d3"}}