{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1999:FNULU3Z6AX5YT27V7EFIHBLDT2","short_pith_number":"pith:FNULU3Z6","canonical_record":{"source":{"id":"nucl-th/9905028","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1999-05-14T13:25:56Z","cross_cats_sorted":["astro-ph","cond-mat.stat-mech","hep-ph"],"title_canon_sha256":"19a25585ba6beabd1a3f0c2174c3928c370c83d2c93dbb72678d37375cfdd8f8","abstract_canon_sha256":"2f3c558f147ac933c0135f5d36b003ec57bbeaa795315e028c49dcd506ee3bed"},"schema_version":"1.0"},"canonical_sha256":"2b68ba6f3e05fb89ebf5f90a8385639ea76a102cc0f07fbd988e315ca160a7a6","source":{"kind":"arxiv","id":"nucl-th/9905028","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/9905028","created_at":"2026-05-18T04:17:26Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/9905028v1","created_at":"2026-05-18T04:17:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/9905028","created_at":"2026-05-18T04:17:26Z"},{"alias_kind":"pith_short_12","alias_value":"FNULU3Z6AX5Y","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_16","alias_value":"FNULU3Z6AX5YT27V","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_8","alias_value":"FNULU3Z6","created_at":"2026-05-18T12:25:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1999:FNULU3Z6AX5YT27V7EFIHBLDT2","target":"record","payload":{"canonical_record":{"source":{"id":"nucl-th/9905028","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1999-05-14T13:25:56Z","cross_cats_sorted":["astro-ph","cond-mat.stat-mech","hep-ph"],"title_canon_sha256":"19a25585ba6beabd1a3f0c2174c3928c370c83d2c93dbb72678d37375cfdd8f8","abstract_canon_sha256":"2f3c558f147ac933c0135f5d36b003ec57bbeaa795315e028c49dcd506ee3bed"},"schema_version":"1.0"},"canonical_sha256":"2b68ba6f3e05fb89ebf5f90a8385639ea76a102cc0f07fbd988e315ca160a7a6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:17:26.117757Z","signature_b64":"pPjIypnOrPRnNKqa8AgrwJgc/AT7H93IWYBMlGP74hWaDhoHzzy3Ep8o7iQmdY5gthR2vIR11HKsLm6f6h+nDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2b68ba6f3e05fb89ebf5f90a8385639ea76a102cc0f07fbd988e315ca160a7a6","last_reissued_at":"2026-05-18T04:17:26.117069Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:17:26.117069Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"nucl-th/9905028","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":"2026-05-18T04:17:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mKEf4WB5p4gr9Oz9uUSEwRJykUqxy5XfBmosNz25rNB8PfqNNMrZPToHqoCrKGN+OwypmxgZZqWZejm5sab6CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T13:18:35.057958Z"},"content_sha256":"2614b8c4731c12a9baa086724aee4245282fda75773133cd899d64e8a92e3248","schema_version":"1.0","event_id":"sha256:2614b8c4731c12a9baa086724aee4245282fda75773133cd899d64e8a92e3248"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1999:FNULU3Z6AX5YT27V7EFIHBLDT2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Resonance Transport and Kinetic Entropy","license":"","headline":"","cross_cats":["astro-ph","cond-mat.stat-mech","hep-ph"],"primary_cat":"nucl-th","authors_text":"D. N. Voskresensky, J. Knoll, Yu. B. Ivanov","submitted_at":"1999-05-14T13:25:56Z","abstract_excerpt":"Within the real-time formulation of nonequilibrium field theory, generalized transport equations are derived avoiding the standard quasiparticle approximation. They permit to include unstable particles into the transport scheme. In order to achieve a self-consistent, conserving and thermodynamically consistent description, we generalize the Baym's $\\Phi$-functional method to genuine nonequilibrium processes. The developed transport description naturally includes all those quantum features already inherent in the corresponding equilibrium limit. Memory effects appearing in collision term diagra"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9905028","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":""},"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":"2026-05-18T04:17:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4omSTB6XS/w6WuhqOC04sMa+vNryDXxA1tIqmSK9BSi/HQpyZJhs3M4KIoz+SrB7f4P5keYaDy1Sa4l8zD+/Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T13:18:35.058300Z"},"content_sha256":"b8dda9cd4c3ffd6d24e0c684e87ad5820f5a1091d9d3b120bba4692805e9ffd6","schema_version":"1.0","event_id":"sha256:b8dda9cd4c3ffd6d24e0c684e87ad5820f5a1091d9d3b120bba4692805e9ffd6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FNULU3Z6AX5YT27V7EFIHBLDT2/bundle.json","state_url":"https://pith.science/pith/FNULU3Z6AX5YT27V7EFIHBLDT2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FNULU3Z6AX5YT27V7EFIHBLDT2/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":"2026-06-05T13:18:35Z","links":{"resolver":"https://pith.science/pith/FNULU3Z6AX5YT27V7EFIHBLDT2","bundle":"https://pith.science/pith/FNULU3Z6AX5YT27V7EFIHBLDT2/bundle.json","state":"https://pith.science/pith/FNULU3Z6AX5YT27V7EFIHBLDT2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FNULU3Z6AX5YT27V7EFIHBLDT2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1999:FNULU3Z6AX5YT27V7EFIHBLDT2","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":"2f3c558f147ac933c0135f5d36b003ec57bbeaa795315e028c49dcd506ee3bed","cross_cats_sorted":["astro-ph","cond-mat.stat-mech","hep-ph"],"license":"","primary_cat":"nucl-th","submitted_at":"1999-05-14T13:25:56Z","title_canon_sha256":"19a25585ba6beabd1a3f0c2174c3928c370c83d2c93dbb72678d37375cfdd8f8"},"schema_version":"1.0","source":{"id":"nucl-th/9905028","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/9905028","created_at":"2026-05-18T04:17:26Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/9905028v1","created_at":"2026-05-18T04:17:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/9905028","created_at":"2026-05-18T04:17:26Z"},{"alias_kind":"pith_short_12","alias_value":"FNULU3Z6AX5Y","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_16","alias_value":"FNULU3Z6AX5YT27V","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_8","alias_value":"FNULU3Z6","created_at":"2026-05-18T12:25:49Z"}],"graph_snapshots":[{"event_id":"sha256:b8dda9cd4c3ffd6d24e0c684e87ad5820f5a1091d9d3b120bba4692805e9ffd6","target":"graph","created_at":"2026-05-18T04:17:26Z","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":"Within the real-time formulation of nonequilibrium field theory, generalized transport equations are derived avoiding the standard quasiparticle approximation. They permit to include unstable particles into the transport scheme. In order to achieve a self-consistent, conserving and thermodynamically consistent description, we generalize the Baym's $\\Phi$-functional method to genuine nonequilibrium processes. The developed transport description naturally includes all those quantum features already inherent in the corresponding equilibrium limit. Memory effects appearing in collision term diagra","authors_text":"D. N. Voskresensky, J. Knoll, Yu. B. Ivanov","cross_cats":["astro-ph","cond-mat.stat-mech","hep-ph"],"headline":"","license":"","primary_cat":"nucl-th","submitted_at":"1999-05-14T13:25:56Z","title":"Resonance Transport and Kinetic Entropy"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9905028","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":"sha256:2614b8c4731c12a9baa086724aee4245282fda75773133cd899d64e8a92e3248","target":"record","created_at":"2026-05-18T04:17:26Z","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":"2f3c558f147ac933c0135f5d36b003ec57bbeaa795315e028c49dcd506ee3bed","cross_cats_sorted":["astro-ph","cond-mat.stat-mech","hep-ph"],"license":"","primary_cat":"nucl-th","submitted_at":"1999-05-14T13:25:56Z","title_canon_sha256":"19a25585ba6beabd1a3f0c2174c3928c370c83d2c93dbb72678d37375cfdd8f8"},"schema_version":"1.0","source":{"id":"nucl-th/9905028","kind":"arxiv","version":1}},"canonical_sha256":"2b68ba6f3e05fb89ebf5f90a8385639ea76a102cc0f07fbd988e315ca160a7a6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2b68ba6f3e05fb89ebf5f90a8385639ea76a102cc0f07fbd988e315ca160a7a6","first_computed_at":"2026-05-18T04:17:26.117069Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:17:26.117069Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"pPjIypnOrPRnNKqa8AgrwJgc/AT7H93IWYBMlGP74hWaDhoHzzy3Ep8o7iQmdY5gthR2vIR11HKsLm6f6h+nDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T04:17:26.117757Z","signed_message":"canonical_sha256_bytes"},"source_id":"nucl-th/9905028","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2614b8c4731c12a9baa086724aee4245282fda75773133cd899d64e8a92e3248","sha256:b8dda9cd4c3ffd6d24e0c684e87ad5820f5a1091d9d3b120bba4692805e9ffd6"],"state_sha256":"525659ecd0d4fa5e6b39d10a2787ec67cc8873ef86fd31973f99ca445bd651ec"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"phR8E2Y0eL/fJ0JTeDlv1k6oZzq1w0E8E0sKRTlcYU1BH6q4/n+AOevJyBsiVw3GQkSdk2G0zw2b4fmjdXoODg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-05T13:18:35.060234Z","bundle_sha256":"8fa0251e8f7e76451e04a6dca953955cfa9cd33a34e53d959d5383109c27fc69"}}