{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:W2O2GEA7HRHFASFFO2G2G24BIU","short_pith_number":"pith:W2O2GEA7","canonical_record":{"source":{"id":"1707.07842","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-07-25T07:55:05Z","cross_cats_sorted":[],"title_canon_sha256":"1efecb9282b14bd2602b74ab09915cfee3d0169b454eab604bfd07d70e4c199f","abstract_canon_sha256":"e172e5eedc81233165e3e8dd5a6cfd24adf7afbbde485ded6d8db01bef4eeadb"},"schema_version":"1.0"},"canonical_sha256":"b69da3101f3c4e5048a5768da36b8145280cd1b023818b52ef382959e5139bac","source":{"kind":"arxiv","id":"1707.07842","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1707.07842","created_at":"2026-05-18T00:28:53Z"},{"alias_kind":"arxiv_version","alias_value":"1707.07842v3","created_at":"2026-05-18T00:28:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.07842","created_at":"2026-05-18T00:28:53Z"},{"alias_kind":"pith_short_12","alias_value":"W2O2GEA7HRHF","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_16","alias_value":"W2O2GEA7HRHFASFF","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_8","alias_value":"W2O2GEA7","created_at":"2026-05-18T12:31:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:W2O2GEA7HRHFASFFO2G2G24BIU","target":"record","payload":{"canonical_record":{"source":{"id":"1707.07842","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-07-25T07:55:05Z","cross_cats_sorted":[],"title_canon_sha256":"1efecb9282b14bd2602b74ab09915cfee3d0169b454eab604bfd07d70e4c199f","abstract_canon_sha256":"e172e5eedc81233165e3e8dd5a6cfd24adf7afbbde485ded6d8db01bef4eeadb"},"schema_version":"1.0"},"canonical_sha256":"b69da3101f3c4e5048a5768da36b8145280cd1b023818b52ef382959e5139bac","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:28:53.300300Z","signature_b64":"8zfEBk8OM6Ix0wYLl0M/Uy1J79yJhQBIegv0JAVIdxzi9UbgTtNqMFQs0HvvUsrkztx4+R2T+Tn7eYUr3erbAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b69da3101f3c4e5048a5768da36b8145280cd1b023818b52ef382959e5139bac","last_reissued_at":"2026-05-18T00:28:53.299831Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:28:53.299831Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1707.07842","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":"2026-05-18T00:28:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OgZJYRWHHkFIuE8svj4/1yr98Y6Bt+TInmVSx9ZN8jsGc0HjCoroZxdeUXs2gcd/rsLaJ9I58InrHthlLTziAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T15:56:41.270957Z"},"content_sha256":"60c671685f3cc2eb55d34923697f2f0af85c5c5f0a8f68fa171ea5032cb5d110","schema_version":"1.0","event_id":"sha256:60c671685f3cc2eb55d34923697f2f0af85c5c5f0a8f68fa171ea5032cb5d110"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:W2O2GEA7HRHFASFFO2G2G24BIU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Self-consistent theory for the linear and nonlinear propagation of a sinusoidal electron plasma wave. Application to stimulated Raman scattering in a non-uniform and non-stationary plasma","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"Didier Benisti","submitted_at":"2017-07-25T07:55:05Z","abstract_excerpt":"In this paper, we address the theoretical resolution of the Vlasov-Gauss system from the linear regime to the strongly nonlinear one, when significant trapping has occurred. The electric field is that of a sinusoidal electron plasma wave (EPW) which is assumed to grow from the noise level, and to keep growing at least up to the amplitude when linear theory in no longer valid (while the wave evolution in the nonlinear regime may be arbitrary). The ions are considered as a neutralizing fluid, while the electron response to the wave is derived by matching two different techniques. We make use of "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.07842","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":"2026-05-18T00:28:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oA/PXXgSen6//D7LhVDi3oEoOs4TXb+ltGyi+0iU98g5Q7+CYrvctOARHsIqW34UuRkaOp3cYUy22Opt3gY0CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T15:56:41.271414Z"},"content_sha256":"126ff2ffc8c5dd5801e6cc7d47296310438bd4eb25f7326ebe39a0d9d82d8241","schema_version":"1.0","event_id":"sha256:126ff2ffc8c5dd5801e6cc7d47296310438bd4eb25f7326ebe39a0d9d82d8241"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/W2O2GEA7HRHFASFFO2G2G24BIU/bundle.json","state_url":"https://pith.science/pith/W2O2GEA7HRHFASFFO2G2G24BIU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/W2O2GEA7HRHFASFFO2G2G24BIU/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":"2026-05-31T15:56:41Z","links":{"resolver":"https://pith.science/pith/W2O2GEA7HRHFASFFO2G2G24BIU","bundle":"https://pith.science/pith/W2O2GEA7HRHFASFFO2G2G24BIU/bundle.json","state":"https://pith.science/pith/W2O2GEA7HRHFASFFO2G2G24BIU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/W2O2GEA7HRHFASFFO2G2G24BIU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:W2O2GEA7HRHFASFFO2G2G24BIU","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":"e172e5eedc81233165e3e8dd5a6cfd24adf7afbbde485ded6d8db01bef4eeadb","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-07-25T07:55:05Z","title_canon_sha256":"1efecb9282b14bd2602b74ab09915cfee3d0169b454eab604bfd07d70e4c199f"},"schema_version":"1.0","source":{"id":"1707.07842","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1707.07842","created_at":"2026-05-18T00:28:53Z"},{"alias_kind":"arxiv_version","alias_value":"1707.07842v3","created_at":"2026-05-18T00:28:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.07842","created_at":"2026-05-18T00:28:53Z"},{"alias_kind":"pith_short_12","alias_value":"W2O2GEA7HRHF","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_16","alias_value":"W2O2GEA7HRHFASFF","created_at":"2026-05-18T12:31:49Z"},{"alias_kind":"pith_short_8","alias_value":"W2O2GEA7","created_at":"2026-05-18T12:31:49Z"}],"graph_snapshots":[{"event_id":"sha256:126ff2ffc8c5dd5801e6cc7d47296310438bd4eb25f7326ebe39a0d9d82d8241","target":"graph","created_at":"2026-05-18T00:28:53Z","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":"In this paper, we address the theoretical resolution of the Vlasov-Gauss system from the linear regime to the strongly nonlinear one, when significant trapping has occurred. The electric field is that of a sinusoidal electron plasma wave (EPW) which is assumed to grow from the noise level, and to keep growing at least up to the amplitude when linear theory in no longer valid (while the wave evolution in the nonlinear regime may be arbitrary). The ions are considered as a neutralizing fluid, while the electron response to the wave is derived by matching two different techniques. We make use of ","authors_text":"Didier Benisti","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-07-25T07:55:05Z","title":"Self-consistent theory for the linear and nonlinear propagation of a sinusoidal electron plasma wave. Application to stimulated Raman scattering in a non-uniform and non-stationary plasma"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.07842","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":"sha256:60c671685f3cc2eb55d34923697f2f0af85c5c5f0a8f68fa171ea5032cb5d110","target":"record","created_at":"2026-05-18T00:28:53Z","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":"e172e5eedc81233165e3e8dd5a6cfd24adf7afbbde485ded6d8db01bef4eeadb","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-07-25T07:55:05Z","title_canon_sha256":"1efecb9282b14bd2602b74ab09915cfee3d0169b454eab604bfd07d70e4c199f"},"schema_version":"1.0","source":{"id":"1707.07842","kind":"arxiv","version":3}},"canonical_sha256":"b69da3101f3c4e5048a5768da36b8145280cd1b023818b52ef382959e5139bac","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b69da3101f3c4e5048a5768da36b8145280cd1b023818b52ef382959e5139bac","first_computed_at":"2026-05-18T00:28:53.299831Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:28:53.299831Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"8zfEBk8OM6Ix0wYLl0M/Uy1J79yJhQBIegv0JAVIdxzi9UbgTtNqMFQs0HvvUsrkztx4+R2T+Tn7eYUr3erbAw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:28:53.300300Z","signed_message":"canonical_sha256_bytes"},"source_id":"1707.07842","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:60c671685f3cc2eb55d34923697f2f0af85c5c5f0a8f68fa171ea5032cb5d110","sha256:126ff2ffc8c5dd5801e6cc7d47296310438bd4eb25f7326ebe39a0d9d82d8241"],"state_sha256":"aeda01e9418201d4ef0f5ef15ebf5962643a2ec541821086dbc9e303f00baf27"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5VdwSDFTRtXMxZe8AtWJrf4CeE6aPX2Rcx4Lso+pqsRePzKXuVFSNypXl4AAt9dJC+M75nuyXgItGkkVFWvPCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T15:56:41.275685Z","bundle_sha256":"9c47e8a68b365c5832ec5fe7ac8951fb7e1c06d58bb4bdd8f833295e31b7ec3b"}}