{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2006:EE7VHMKXNRQSCWS5ZE4HPZKHQ7","short_pith_number":"pith:EE7VHMKX","canonical_record":{"source":{"id":"physics/0602155","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"physics.plasm-ph","submitted_at":"2006-02-23T01:33:41Z","cross_cats_sorted":["cond-mat.other"],"title_canon_sha256":"781c8505bdb1c40efd900799e5a80848501d078316c07448bfbe783a36b208ec","abstract_canon_sha256":"76855dbee66e8f1d5d57aae44e56e3afe70a08559385b80663382fdeb9ba13a0"},"schema_version":"1.0"},"canonical_sha256":"213f53b1576c61215a5dc93877e54787e3528f019d9e00dba319feee2aa884b5","source":{"kind":"arxiv","id":"physics/0602155","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"physics/0602155","created_at":"2026-07-04T17:02:25Z"},{"alias_kind":"arxiv_version","alias_value":"physics/0602155v1","created_at":"2026-07-04T17:02:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.physics/0602155","created_at":"2026-07-04T17:02:25Z"},{"alias_kind":"pith_short_12","alias_value":"EE7VHMKXNRQS","created_at":"2026-07-04T17:02:25Z"},{"alias_kind":"pith_short_16","alias_value":"EE7VHMKXNRQSCWS5","created_at":"2026-07-04T17:02:25Z"},{"alias_kind":"pith_short_8","alias_value":"EE7VHMKX","created_at":"2026-07-04T17:02:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2006:EE7VHMKXNRQSCWS5ZE4HPZKHQ7","target":"record","payload":{"canonical_record":{"source":{"id":"physics/0602155","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"physics.plasm-ph","submitted_at":"2006-02-23T01:33:41Z","cross_cats_sorted":["cond-mat.other"],"title_canon_sha256":"781c8505bdb1c40efd900799e5a80848501d078316c07448bfbe783a36b208ec","abstract_canon_sha256":"76855dbee66e8f1d5d57aae44e56e3afe70a08559385b80663382fdeb9ba13a0"},"schema_version":"1.0"},"canonical_sha256":"213f53b1576c61215a5dc93877e54787e3528f019d9e00dba319feee2aa884b5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:02:25.771989Z","signature_b64":"Yz/1BzAE+mwTv3LgL4LaTgp/ljKze1ih/QusGMdiHHgDDcIxoQosUaZfkpshHoTSfPtoxdjVsRrjSqVmLcesAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"213f53b1576c61215a5dc93877e54787e3528f019d9e00dba319feee2aa884b5","last_reissued_at":"2026-07-04T17:02:25.771622Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:02:25.771622Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"physics/0602155","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":"2026-07-04T17:02:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tNlrDwcyh6bCj506OqKqBE2eMAxpHDFKqxswj8gvecbMVtqZ5Be+t8kqcnh1mQrIjWtbwWYAcgQwHpZBRGNdBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T01:48:14.698202Z"},"content_sha256":"adead8d6e5005b495d638354f5d2d8c027f3b129e80c67e300eea255e8f6428c","schema_version":"1.0","event_id":"sha256:adead8d6e5005b495d638354f5d2d8c027f3b129e80c67e300eea255e8f6428c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2006:EE7VHMKXNRQSCWS5ZE4HPZKHQ7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Invariant imbedding theory of mode conversion in inhomogeneous plasmas. II. Mode conversion in cold, magnetized plasmas with perpendicular inhomogeneity","license":"","headline":"","cross_cats":["cond-mat.other"],"primary_cat":"physics.plasm-ph","authors_text":"Dong-Hun Lee, Kihong Kim","submitted_at":"2006-02-23T01:33:41Z","abstract_excerpt":"A new version of the invariant imbedding theory for the propagation of coupled waves in inhomogeneous media is applied to the mode conversion of high frequency electromagnetic waves into electrostatic modes in cold, magnetized and stratified plasmas. The cases where the external magnetic field is applied perpendicularly to the direction of inhomogeneity and the electron density profile is linear are considered. Extensive and numerically exact results for the mode conversion coefficients, the reflectances and the wave electric and magnetic field profiles inside the inhomogeneous plasma are obta"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"physics/0602155","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/physics/0602155/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T17:02:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"i36SIwIlfgkkERlB+49GF7w0R0dNL+Mpwc6wRmGMhp+/NsbPQ05X6lU9B4yeGywFoN0+jpVYufr9aqGZZvcwCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T01:48:14.698700Z"},"content_sha256":"6c5e3ba0b672f03b12e44342d2a95c63747b58fd0e5631dea7d65b8ce7315ed3","schema_version":"1.0","event_id":"sha256:6c5e3ba0b672f03b12e44342d2a95c63747b58fd0e5631dea7d65b8ce7315ed3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/EE7VHMKXNRQSCWS5ZE4HPZKHQ7/bundle.json","state_url":"https://pith.science/pith/EE7VHMKXNRQSCWS5ZE4HPZKHQ7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/EE7VHMKXNRQSCWS5ZE4HPZKHQ7/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":"2026-08-05T01:48:14Z","links":{"resolver":"https://pith.science/pith/EE7VHMKXNRQSCWS5ZE4HPZKHQ7","bundle":"https://pith.science/pith/EE7VHMKXNRQSCWS5ZE4HPZKHQ7/bundle.json","state":"https://pith.science/pith/EE7VHMKXNRQSCWS5ZE4HPZKHQ7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/EE7VHMKXNRQSCWS5ZE4HPZKHQ7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2006:EE7VHMKXNRQSCWS5ZE4HPZKHQ7","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":"76855dbee66e8f1d5d57aae44e56e3afe70a08559385b80663382fdeb9ba13a0","cross_cats_sorted":["cond-mat.other"],"license":"","primary_cat":"physics.plasm-ph","submitted_at":"2006-02-23T01:33:41Z","title_canon_sha256":"781c8505bdb1c40efd900799e5a80848501d078316c07448bfbe783a36b208ec"},"schema_version":"1.0","source":{"id":"physics/0602155","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"physics/0602155","created_at":"2026-07-04T17:02:25Z"},{"alias_kind":"arxiv_version","alias_value":"physics/0602155v1","created_at":"2026-07-04T17:02:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.physics/0602155","created_at":"2026-07-04T17:02:25Z"},{"alias_kind":"pith_short_12","alias_value":"EE7VHMKXNRQS","created_at":"2026-07-04T17:02:25Z"},{"alias_kind":"pith_short_16","alias_value":"EE7VHMKXNRQSCWS5","created_at":"2026-07-04T17:02:25Z"},{"alias_kind":"pith_short_8","alias_value":"EE7VHMKX","created_at":"2026-07-04T17:02:25Z"}],"graph_snapshots":[{"event_id":"sha256:6c5e3ba0b672f03b12e44342d2a95c63747b58fd0e5631dea7d65b8ce7315ed3","target":"graph","created_at":"2026-07-04T17:02:25Z","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/physics/0602155/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"A new version of the invariant imbedding theory for the propagation of coupled waves in inhomogeneous media is applied to the mode conversion of high frequency electromagnetic waves into electrostatic modes in cold, magnetized and stratified plasmas. The cases where the external magnetic field is applied perpendicularly to the direction of inhomogeneity and the electron density profile is linear are considered. Extensive and numerically exact results for the mode conversion coefficients, the reflectances and the wave electric and magnetic field profiles inside the inhomogeneous plasma are obta","authors_text":"Dong-Hun Lee, Kihong Kim","cross_cats":["cond-mat.other"],"headline":"","license":"","primary_cat":"physics.plasm-ph","submitted_at":"2006-02-23T01:33:41Z","title":"Invariant imbedding theory of mode conversion in inhomogeneous plasmas. II. Mode conversion in cold, magnetized plasmas with perpendicular inhomogeneity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"physics/0602155","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:adead8d6e5005b495d638354f5d2d8c027f3b129e80c67e300eea255e8f6428c","target":"record","created_at":"2026-07-04T17:02:25Z","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":"76855dbee66e8f1d5d57aae44e56e3afe70a08559385b80663382fdeb9ba13a0","cross_cats_sorted":["cond-mat.other"],"license":"","primary_cat":"physics.plasm-ph","submitted_at":"2006-02-23T01:33:41Z","title_canon_sha256":"781c8505bdb1c40efd900799e5a80848501d078316c07448bfbe783a36b208ec"},"schema_version":"1.0","source":{"id":"physics/0602155","kind":"arxiv","version":1}},"canonical_sha256":"213f53b1576c61215a5dc93877e54787e3528f019d9e00dba319feee2aa884b5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"213f53b1576c61215a5dc93877e54787e3528f019d9e00dba319feee2aa884b5","first_computed_at":"2026-07-04T17:02:25.771622Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T17:02:25.771622Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Yz/1BzAE+mwTv3LgL4LaTgp/ljKze1ih/QusGMdiHHgDDcIxoQosUaZfkpshHoTSfPtoxdjVsRrjSqVmLcesAQ==","signature_status":"signed_v1","signed_at":"2026-07-04T17:02:25.771989Z","signed_message":"canonical_sha256_bytes"},"source_id":"physics/0602155","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:adead8d6e5005b495d638354f5d2d8c027f3b129e80c67e300eea255e8f6428c","sha256:6c5e3ba0b672f03b12e44342d2a95c63747b58fd0e5631dea7d65b8ce7315ed3"],"state_sha256":"70cfc62000c8a589d21349c61a2dc05684835036930222e714276d40314cb5e7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lDk6kteKMYcmirp4GhGhd9UDL+0gkBGSGOobHtAuXISyEp2CmTc1iRDGaxqcyx9Wcw5VO+u9D2OSUuDYY+PQBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-05T01:48:14.703544Z","bundle_sha256":"7a158850d70b099de441a70c45035a8b7806de39db90159a288bd04cac6fddec"}}