{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:KREB6ISUDWKL644XXP3O4XXHY2","short_pith_number":"pith:KREB6ISU","canonical_record":{"source":{"id":"1710.02541","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-10-06T18:20:54Z","cross_cats_sorted":[],"title_canon_sha256":"8037e919790398bf19ef87bfa245fc8a71300835020199f6994f7b2430a963e1","abstract_canon_sha256":"5fbea9d4290b9d734c323001f612ca05b640b9fbc11227136509f47fe43fb960"},"schema_version":"1.0"},"canonical_sha256":"54481f22541d94bf7397bbf6ee5ee7c6b21e848b6ba5fadcae780173b9f80438","source":{"kind":"arxiv","id":"1710.02541","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.02541","created_at":"2026-05-18T00:33:29Z"},{"alias_kind":"arxiv_version","alias_value":"1710.02541v1","created_at":"2026-05-18T00:33:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.02541","created_at":"2026-05-18T00:33:29Z"},{"alias_kind":"pith_short_12","alias_value":"KREB6ISUDWKL","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_16","alias_value":"KREB6ISUDWKL644X","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_8","alias_value":"KREB6ISU","created_at":"2026-05-18T12:31:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:KREB6ISUDWKL644XXP3O4XXHY2","target":"record","payload":{"canonical_record":{"source":{"id":"1710.02541","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-10-06T18:20:54Z","cross_cats_sorted":[],"title_canon_sha256":"8037e919790398bf19ef87bfa245fc8a71300835020199f6994f7b2430a963e1","abstract_canon_sha256":"5fbea9d4290b9d734c323001f612ca05b640b9fbc11227136509f47fe43fb960"},"schema_version":"1.0"},"canonical_sha256":"54481f22541d94bf7397bbf6ee5ee7c6b21e848b6ba5fadcae780173b9f80438","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:33:29.538716Z","signature_b64":"vhMItV1FfTzHUeFVhurzubgju+YSBveMggrlItNAQpQGm7+blrFJlY72c22Mf+8FnuBTG5NlqNeJGIW3YLhOAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"54481f22541d94bf7397bbf6ee5ee7c6b21e848b6ba5fadcae780173b9f80438","last_reissued_at":"2026-05-18T00:33:29.538115Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:33:29.538115Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1710.02541","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":"2026-05-18T00:33:29Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"t9l8d+0ig6JjkR9Pc1lbn27pJja4kLi+f4TvwEb0544STFOS9ULUz7DqVG+qg0UzI3bd+7L/BtAGjgTtWw5eCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-29T07:26:06.738794Z"},"content_sha256":"b5b63eba7c51dc96ada53b22553f8972f64ecf7c746a722cca2821d501f22d95","schema_version":"1.0","event_id":"sha256:b5b63eba7c51dc96ada53b22553f8972f64ecf7c746a722cca2821d501f22d95"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:KREB6ISUDWKL644XXP3O4XXHY2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Lower hybrid destabilization of trapped electron modes in tokamak and its consequences for anomalous diffusion","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"A. Kuley, C. S. Liu, V. K. Tripathi","submitted_at":"2017-10-06T18:20:54Z","abstract_excerpt":"Parametric coupling of lower hybrid pump wave with low frequency collisionless/weakly collisional trapped electron drift wave, with frequency lower than the electron bounce frequency is studied. The coupling produces two lower hybrid sidebands. The sidebands beat with the pump to exert a low frequency ponderomotive force on electrons that causes a frequency shift in the drift wave, leading to the growth of the latter. The short wavelength modes are destabilized and they enhance the anomalous diffusion coefficient."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.02541","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":""},"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":"2026-05-18T00:33:29Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"R9ZPj0cjO+iIxQYbnAMB5zCWCbjY2hlAXU0AeKgucw64cIdlN7uEZZW3HpEZMuy05oUuiwgTM2QMAOf4mHaoAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-29T07:26:06.739124Z"},"content_sha256":"e8da6b2bc31f8b87073fd78691c6aa60fe96a11295ddf5f3a32d111e0f4d9f0d","schema_version":"1.0","event_id":"sha256:e8da6b2bc31f8b87073fd78691c6aa60fe96a11295ddf5f3a32d111e0f4d9f0d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KREB6ISUDWKL644XXP3O4XXHY2/bundle.json","state_url":"https://pith.science/pith/KREB6ISUDWKL644XXP3O4XXHY2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KREB6ISUDWKL644XXP3O4XXHY2/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":"2026-06-29T07:26:06Z","links":{"resolver":"https://pith.science/pith/KREB6ISUDWKL644XXP3O4XXHY2","bundle":"https://pith.science/pith/KREB6ISUDWKL644XXP3O4XXHY2/bundle.json","state":"https://pith.science/pith/KREB6ISUDWKL644XXP3O4XXHY2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KREB6ISUDWKL644XXP3O4XXHY2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:KREB6ISUDWKL644XXP3O4XXHY2","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":"5fbea9d4290b9d734c323001f612ca05b640b9fbc11227136509f47fe43fb960","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-10-06T18:20:54Z","title_canon_sha256":"8037e919790398bf19ef87bfa245fc8a71300835020199f6994f7b2430a963e1"},"schema_version":"1.0","source":{"id":"1710.02541","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.02541","created_at":"2026-05-18T00:33:29Z"},{"alias_kind":"arxiv_version","alias_value":"1710.02541v1","created_at":"2026-05-18T00:33:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.02541","created_at":"2026-05-18T00:33:29Z"},{"alias_kind":"pith_short_12","alias_value":"KREB6ISUDWKL","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_16","alias_value":"KREB6ISUDWKL644X","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_8","alias_value":"KREB6ISU","created_at":"2026-05-18T12:31:28Z"}],"graph_snapshots":[{"event_id":"sha256:e8da6b2bc31f8b87073fd78691c6aa60fe96a11295ddf5f3a32d111e0f4d9f0d","target":"graph","created_at":"2026-05-18T00:33:29Z","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":"Parametric coupling of lower hybrid pump wave with low frequency collisionless/weakly collisional trapped electron drift wave, with frequency lower than the electron bounce frequency is studied. The coupling produces two lower hybrid sidebands. The sidebands beat with the pump to exert a low frequency ponderomotive force on electrons that causes a frequency shift in the drift wave, leading to the growth of the latter. The short wavelength modes are destabilized and they enhance the anomalous diffusion coefficient.","authors_text":"A. Kuley, C. S. Liu, V. K. Tripathi","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-10-06T18:20:54Z","title":"Lower hybrid destabilization of trapped electron modes in tokamak and its consequences for anomalous diffusion"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.02541","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:b5b63eba7c51dc96ada53b22553f8972f64ecf7c746a722cca2821d501f22d95","target":"record","created_at":"2026-05-18T00:33:29Z","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":"5fbea9d4290b9d734c323001f612ca05b640b9fbc11227136509f47fe43fb960","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2017-10-06T18:20:54Z","title_canon_sha256":"8037e919790398bf19ef87bfa245fc8a71300835020199f6994f7b2430a963e1"},"schema_version":"1.0","source":{"id":"1710.02541","kind":"arxiv","version":1}},"canonical_sha256":"54481f22541d94bf7397bbf6ee5ee7c6b21e848b6ba5fadcae780173b9f80438","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"54481f22541d94bf7397bbf6ee5ee7c6b21e848b6ba5fadcae780173b9f80438","first_computed_at":"2026-05-18T00:33:29.538115Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:33:29.538115Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vhMItV1FfTzHUeFVhurzubgju+YSBveMggrlItNAQpQGm7+blrFJlY72c22Mf+8FnuBTG5NlqNeJGIW3YLhOAw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:33:29.538716Z","signed_message":"canonical_sha256_bytes"},"source_id":"1710.02541","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b5b63eba7c51dc96ada53b22553f8972f64ecf7c746a722cca2821d501f22d95","sha256:e8da6b2bc31f8b87073fd78691c6aa60fe96a11295ddf5f3a32d111e0f4d9f0d"],"state_sha256":"10db3c7e2ea2fc1f8d2cb970d49651a081514f1260ac81704f7cc3337e72df74"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OPxHZvjyq2mtcqCLLKGTnbrBIZ8G8bRBVb509QlYceKLVatLalrkRDN4wT1Hztg52VZr4884DBb+ITYvXfhDAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-29T07:26:06.741036Z","bundle_sha256":"fea80f017ce5ffae7cb6cd3f0439fddc6c5a6848639132eac8c3e5633b178aaf"}}