{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:YEJQYOTN36K4NKDY2D7ZMF46NW","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":"d1f095675bf6d3091c99c81cf4960ec616fa9149a77ec21c4c0b2850cb2ed9c7","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2024-11-19T22:02:03Z","title_canon_sha256":"8627168466d3d8d91b059652cd3d78b748f6337791bea45af43ab8c8d489cf81"},"schema_version":"1.0","source":{"id":"2411.12883","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2411.12883","created_at":"2026-07-05T09:50:54Z"},{"alias_kind":"arxiv_version","alias_value":"2411.12883v2","created_at":"2026-07-05T09:50:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.12883","created_at":"2026-07-05T09:50:54Z"},{"alias_kind":"pith_short_12","alias_value":"YEJQYOTN36K4","created_at":"2026-07-05T09:50:54Z"},{"alias_kind":"pith_short_16","alias_value":"YEJQYOTN36K4NKDY","created_at":"2026-07-05T09:50:54Z"},{"alias_kind":"pith_short_8","alias_value":"YEJQYOTN","created_at":"2026-07-05T09:50:54Z"}],"graph_snapshots":[{"event_id":"sha256:dcc5a853cde9a0f078fafa0cae3d92c5200aa8c0bd67e52621a532f243fbfeec","target":"graph","created_at":"2026-07-05T09:50:54Z","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/2411.12883/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The usual approach on electrostatic wave decay process for a weak beam-plasma system considers two different wave modes interplaying, the Langmuir and ion-sound mode. In the present paper, a single-mode approach is shown to be feasible for conditions where the respective dispersion relations undergo topological changes. Numerical solutions for the dispersion relation of a beam-plasma system are presented, supporting the modeling of an analytic dispersion relation of a single wave mode. This wave mode is accounted for in the kinetic equations for particles and waves, which rule the evolution of","authors_text":"Guilherme T. Irum\\'e, Joel Pavan, Rudi Gaelzer","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2024-11-19T22:02:03Z","title":"Single-Mode Wave Decay"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.12883","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":"sha256:1be9b70d7789705b6be006924d7417bb4eac8884827c01d4cf4e5b5286a7dad9","target":"record","created_at":"2026-07-05T09:50:54Z","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":"d1f095675bf6d3091c99c81cf4960ec616fa9149a77ec21c4c0b2850cb2ed9c7","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2024-11-19T22:02:03Z","title_canon_sha256":"8627168466d3d8d91b059652cd3d78b748f6337791bea45af43ab8c8d489cf81"},"schema_version":"1.0","source":{"id":"2411.12883","kind":"arxiv","version":2}},"canonical_sha256":"c1130c3a6ddf95c6a878d0ff96179e6d921cf651bb7530b4def33dcd29161e4e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c1130c3a6ddf95c6a878d0ff96179e6d921cf651bb7530b4def33dcd29161e4e","first_computed_at":"2026-07-05T09:50:54.419125Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T09:50:54.419125Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"IDXbKt5L1gjOwQKX/Rpuz+L1iLHXBOH1soXWcTgdknjW+CGZuHFYAa+nE0qeipMpOSQL34tUmuOBJyTDP570Dg==","signature_status":"signed_v1","signed_at":"2026-07-05T09:50:54.419704Z","signed_message":"canonical_sha256_bytes"},"source_id":"2411.12883","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1be9b70d7789705b6be006924d7417bb4eac8884827c01d4cf4e5b5286a7dad9","sha256:dcc5a853cde9a0f078fafa0cae3d92c5200aa8c0bd67e52621a532f243fbfeec"],"state_sha256":"6783a1812f25d4183d839d27376a00d919038f626c0353b72d4a4f7e4c6320e8"}