{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:6UPYBY43QUQJASIBISMR4HQQXL","short_pith_number":"pith:6UPYBY43","canonical_record":{"source":{"id":"1003.1523","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2010-03-07T21:22:04Z","cross_cats_sorted":["cond-mat.quant-gas","quant-ph"],"title_canon_sha256":"7341c4ab29410c7f45865c719e64b16d183bae32feecb95823d30fdc3407ddec","abstract_canon_sha256":"5ae24729a89698fe12e1ee0bf3d52828343d3499c0b3f83cce1036be58a6156c"},"schema_version":"1.0"},"canonical_sha256":"f51f80e39b852090490144991e1e10baf6f135526b170b85410e4ed738987bbf","source":{"kind":"arxiv","id":"1003.1523","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1003.1523","created_at":"2026-05-18T02:08:45Z"},{"alias_kind":"arxiv_version","alias_value":"1003.1523v2","created_at":"2026-05-18T02:08:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1003.1523","created_at":"2026-05-18T02:08:45Z"},{"alias_kind":"pith_short_12","alias_value":"6UPYBY43QUQJ","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_16","alias_value":"6UPYBY43QUQJASIB","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_8","alias_value":"6UPYBY43","created_at":"2026-05-18T12:26:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:6UPYBY43QUQJASIBISMR4HQQXL","target":"record","payload":{"canonical_record":{"source":{"id":"1003.1523","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2010-03-07T21:22:04Z","cross_cats_sorted":["cond-mat.quant-gas","quant-ph"],"title_canon_sha256":"7341c4ab29410c7f45865c719e64b16d183bae32feecb95823d30fdc3407ddec","abstract_canon_sha256":"5ae24729a89698fe12e1ee0bf3d52828343d3499c0b3f83cce1036be58a6156c"},"schema_version":"1.0"},"canonical_sha256":"f51f80e39b852090490144991e1e10baf6f135526b170b85410e4ed738987bbf","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:08:45.163956Z","signature_b64":"5PX4G3cQFxeeodCYeS6rCOs0h8vXgNYAcl4ZfbItYs/5BqYj8cVYQAWL5iqjg7ejsPyzU4vPg8FnYxiGMw4+DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f51f80e39b852090490144991e1e10baf6f135526b170b85410e4ed738987bbf","last_reissued_at":"2026-05-18T02:08:45.163109Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:08:45.163109Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1003.1523","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":"2026-05-18T02:08:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1gsLpSJzF8y6VMOY77rJsvgTLcFuOv4Njwsnl+ItniEtVgPkkqJ49IJs2vIZymJfuSyLJXn8ygOpqMx4tFzvBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T10:59:47.731913Z"},"content_sha256":"7cf7f2477ecce41b6ccd832c580c57448d515deac6842fe05f3c9490c049ff28","schema_version":"1.0","event_id":"sha256:7cf7f2477ecce41b6ccd832c580c57448d515deac6842fe05f3c9490c049ff28"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:6UPYBY43QUQJASIBISMR4HQQXL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Theory of plasmon decay in dense plasmas and warm dense matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","quant-ph"],"primary_cat":"physics.plasm-ph","authors_text":"S. Ku, S. Son, Sung Joon Moon","submitted_at":"2010-03-07T21:22:04Z","abstract_excerpt":"The decay of the Langmuir waves in dense plasmas is not accurately predicted by the prevalent Landau damping theory. A dielectric function theory is introduced, predicting much higher damping than the Landau damping theory. This strong damping is in better agreement with the experimentally observed data in metals. It is shown that the strong plasmon decay leads to the existence of a parameter regime where the backward Raman scattering is unstable while the forward Raman scattering is stable.  This regime may be used to create intense x-ray pulses, by means of the the backward Raman compression"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1003.1523","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":"2026-05-18T02:08:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"D3yYtM1Z+MWXda2NLhX7w7lLEd7Ze5WNQH3OQeLb2+jFTm8Zfay/8uRBkD9HFwRYhxhNfv+3zuzJvnyyhfohDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T10:59:47.732266Z"},"content_sha256":"bf05e2cb2f2578512ea14533a7dfcaa410e88169bffe3d3f705f51523612532a","schema_version":"1.0","event_id":"sha256:bf05e2cb2f2578512ea14533a7dfcaa410e88169bffe3d3f705f51523612532a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6UPYBY43QUQJASIBISMR4HQQXL/bundle.json","state_url":"https://pith.science/pith/6UPYBY43QUQJASIBISMR4HQQXL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6UPYBY43QUQJASIBISMR4HQQXL/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":"2026-06-24T10:59:47Z","links":{"resolver":"https://pith.science/pith/6UPYBY43QUQJASIBISMR4HQQXL","bundle":"https://pith.science/pith/6UPYBY43QUQJASIBISMR4HQQXL/bundle.json","state":"https://pith.science/pith/6UPYBY43QUQJASIBISMR4HQQXL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6UPYBY43QUQJASIBISMR4HQQXL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:6UPYBY43QUQJASIBISMR4HQQXL","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":"5ae24729a89698fe12e1ee0bf3d52828343d3499c0b3f83cce1036be58a6156c","cross_cats_sorted":["cond-mat.quant-gas","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2010-03-07T21:22:04Z","title_canon_sha256":"7341c4ab29410c7f45865c719e64b16d183bae32feecb95823d30fdc3407ddec"},"schema_version":"1.0","source":{"id":"1003.1523","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1003.1523","created_at":"2026-05-18T02:08:45Z"},{"alias_kind":"arxiv_version","alias_value":"1003.1523v2","created_at":"2026-05-18T02:08:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1003.1523","created_at":"2026-05-18T02:08:45Z"},{"alias_kind":"pith_short_12","alias_value":"6UPYBY43QUQJ","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_16","alias_value":"6UPYBY43QUQJASIB","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_8","alias_value":"6UPYBY43","created_at":"2026-05-18T12:26:04Z"}],"graph_snapshots":[{"event_id":"sha256:bf05e2cb2f2578512ea14533a7dfcaa410e88169bffe3d3f705f51523612532a","target":"graph","created_at":"2026-05-18T02:08:45Z","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":"The decay of the Langmuir waves in dense plasmas is not accurately predicted by the prevalent Landau damping theory. A dielectric function theory is introduced, predicting much higher damping than the Landau damping theory. This strong damping is in better agreement with the experimentally observed data in metals. It is shown that the strong plasmon decay leads to the existence of a parameter regime where the backward Raman scattering is unstable while the forward Raman scattering is stable.  This regime may be used to create intense x-ray pulses, by means of the the backward Raman compression","authors_text":"S. Ku, S. Son, Sung Joon Moon","cross_cats":["cond-mat.quant-gas","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2010-03-07T21:22:04Z","title":"Theory of plasmon decay in dense plasmas and warm dense matter"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1003.1523","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":"sha256:7cf7f2477ecce41b6ccd832c580c57448d515deac6842fe05f3c9490c049ff28","target":"record","created_at":"2026-05-18T02:08:45Z","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":"5ae24729a89698fe12e1ee0bf3d52828343d3499c0b3f83cce1036be58a6156c","cross_cats_sorted":["cond-mat.quant-gas","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2010-03-07T21:22:04Z","title_canon_sha256":"7341c4ab29410c7f45865c719e64b16d183bae32feecb95823d30fdc3407ddec"},"schema_version":"1.0","source":{"id":"1003.1523","kind":"arxiv","version":2}},"canonical_sha256":"f51f80e39b852090490144991e1e10baf6f135526b170b85410e4ed738987bbf","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f51f80e39b852090490144991e1e10baf6f135526b170b85410e4ed738987bbf","first_computed_at":"2026-05-18T02:08:45.163109Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:08:45.163109Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"5PX4G3cQFxeeodCYeS6rCOs0h8vXgNYAcl4ZfbItYs/5BqYj8cVYQAWL5iqjg7ejsPyzU4vPg8FnYxiGMw4+DQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:08:45.163956Z","signed_message":"canonical_sha256_bytes"},"source_id":"1003.1523","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7cf7f2477ecce41b6ccd832c580c57448d515deac6842fe05f3c9490c049ff28","sha256:bf05e2cb2f2578512ea14533a7dfcaa410e88169bffe3d3f705f51523612532a"],"state_sha256":"33f202f6d83eb42b81b017d4dfe161798d271508d13c0b789fac405b0fe72d6e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"n72Tk+jOtcB19GtFZ88hJO7NvBWTWMVQty+ou2v/uL1FgRJc2TlYiZz55ndf1G3otfc/haOyqXdJxl4JqLPiCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-24T10:59:47.734261Z","bundle_sha256":"64dd22e5ae42519bc30e0aefa67cf60d5c9e3412eb76e86cf2aaa29b30fdc8e7"}}