{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:4TDPCBAG2CWTOCQWJMTQWVRQDS","short_pith_number":"pith:4TDPCBAG","schema_version":"1.0","canonical_sha256":"e4c6f10406d0ad370a164b270b56301c8ce1676b0f114e80cac603a776973e9a","source":{"kind":"arxiv","id":"2505.24607","version":1},"attestation_state":"computed","paper":{"title":"Resonance density range governs two-plasmon decay saturation and enables hot-electron prediction in inertial confinement fusion","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"C.Yao, G-N.Zheng, J. Li, J. Zheng, L. Hao, Q.Jia, R. Yan, T.Tao, Y-K. Ding","submitted_at":"2025-05-30T13:55:12Z","abstract_excerpt":"The saturation level of parametric instabilities critically determines their impact on fusion plasmas. We identify the resonance density range of two-plasmon decay as the critical parameter governing nonlinear saturation of ion density fluctuations and Langmuir waves, which drive hot-electron generation. Using this insight, we develop a predictive scaling model for the hot-electron energy fraction f_{hot} that depends only on the laser intensity I, with plasma conditions encoded via plasma ablation theory. The model can work for various experimental configurations-requiring only two (I, f_{hot"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2505.24607","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-05-30T13:55:12Z","cross_cats_sorted":[],"title_canon_sha256":"486cd68b9d511549b5be3e34e5e99a66fd539ad92025e1d82ec1696351d91ac1","abstract_canon_sha256":"5bd286fb129281a01ef806fbb248b8656a02cc691a2224e825824c4fde5f0097"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:12:53.245601Z","signature_b64":"/1USGj9ffJ6+Z286ams7pAMN08Tfwq9UNRiU+ZskLmBxS9o1bDM1Ap00NFgxDlGR+q9XnkLEu3B9XRkHUrniDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e4c6f10406d0ad370a164b270b56301c8ce1676b0f114e80cac603a776973e9a","last_reissued_at":"2026-07-05T11:12:53.245031Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:12:53.245031Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Resonance density range governs two-plasmon decay saturation and enables hot-electron prediction in inertial confinement fusion","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"C.Yao, G-N.Zheng, J. Li, J. Zheng, L. Hao, Q.Jia, R. Yan, T.Tao, Y-K. Ding","submitted_at":"2025-05-30T13:55:12Z","abstract_excerpt":"The saturation level of parametric instabilities critically determines their impact on fusion plasmas. We identify the resonance density range of two-plasmon decay as the critical parameter governing nonlinear saturation of ion density fluctuations and Langmuir waves, which drive hot-electron generation. Using this insight, we develop a predictive scaling model for the hot-electron energy fraction f_{hot} that depends only on the laser intensity I, with plasma conditions encoded via plasma ablation theory. The model can work for various experimental configurations-requiring only two (I, f_{hot"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.24607","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2505.24607/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2505.24607","created_at":"2026-07-05T11:12:53.245099+00:00"},{"alias_kind":"arxiv_version","alias_value":"2505.24607v1","created_at":"2026-07-05T11:12:53.245099+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.24607","created_at":"2026-07-05T11:12:53.245099+00:00"},{"alias_kind":"pith_short_12","alias_value":"4TDPCBAG2CWT","created_at":"2026-07-05T11:12:53.245099+00:00"},{"alias_kind":"pith_short_16","alias_value":"4TDPCBAG2CWTOCQW","created_at":"2026-07-05T11:12:53.245099+00:00"},{"alias_kind":"pith_short_8","alias_value":"4TDPCBAG","created_at":"2026-07-05T11:12:53.245099+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2509.06021","citing_title":"Resonance density range of absolute two-plasmon decay instability","ref_index":37,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4TDPCBAG2CWTOCQWJMTQWVRQDS","json":"https://pith.science/pith/4TDPCBAG2CWTOCQWJMTQWVRQDS.json","graph_json":"https://pith.science/api/pith-number/4TDPCBAG2CWTOCQWJMTQWVRQDS/graph.json","events_json":"https://pith.science/api/pith-number/4TDPCBAG2CWTOCQWJMTQWVRQDS/events.json","paper":"https://pith.science/paper/4TDPCBAG"},"agent_actions":{"view_html":"https://pith.science/pith/4TDPCBAG2CWTOCQWJMTQWVRQDS","download_json":"https://pith.science/pith/4TDPCBAG2CWTOCQWJMTQWVRQDS.json","view_paper":"https://pith.science/paper/4TDPCBAG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2505.24607&json=true","fetch_graph":"https://pith.science/api/pith-number/4TDPCBAG2CWTOCQWJMTQWVRQDS/graph.json","fetch_events":"https://pith.science/api/pith-number/4TDPCBAG2CWTOCQWJMTQWVRQDS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4TDPCBAG2CWTOCQWJMTQWVRQDS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4TDPCBAG2CWTOCQWJMTQWVRQDS/action/storage_attestation","attest_author":"https://pith.science/pith/4TDPCBAG2CWTOCQWJMTQWVRQDS/action/author_attestation","sign_citation":"https://pith.science/pith/4TDPCBAG2CWTOCQWJMTQWVRQDS/action/citation_signature","submit_replication":"https://pith.science/pith/4TDPCBAG2CWTOCQWJMTQWVRQDS/action/replication_record"}},"created_at":"2026-07-05T11:12:53.245099+00:00","updated_at":"2026-07-05T11:12:53.245099+00:00"}