{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:LDPBAVG4MKGMX7UIRLCB3IK6D2","short_pith_number":"pith:LDPBAVG4","canonical_record":{"source":{"id":"1402.7230","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2014-02-28T12:53:31Z","cross_cats_sorted":["physics.space-ph"],"title_canon_sha256":"e7bcdadd05c33a257c46804ed074fa817124e5d23b402b6caf17c107898e0d70","abstract_canon_sha256":"4f4661b1246981a999029be4137d0063c4b351fb2a9df3f31594a1846d1a1d99"},"schema_version":"1.0"},"canonical_sha256":"58de1054dc628ccbfe888ac41da15e1ea34ab230457cd929e46929fa22416a22","source":{"kind":"arxiv","id":"1402.7230","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1402.7230","created_at":"2026-05-18T02:29:55Z"},{"alias_kind":"arxiv_version","alias_value":"1402.7230v2","created_at":"2026-05-18T02:29:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.7230","created_at":"2026-05-18T02:29:55Z"},{"alias_kind":"pith_short_12","alias_value":"LDPBAVG4MKGM","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"LDPBAVG4MKGMX7UI","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"LDPBAVG4","created_at":"2026-05-18T12:28:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:LDPBAVG4MKGMX7UIRLCB3IK6D2","target":"record","payload":{"canonical_record":{"source":{"id":"1402.7230","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2014-02-28T12:53:31Z","cross_cats_sorted":["physics.space-ph"],"title_canon_sha256":"e7bcdadd05c33a257c46804ed074fa817124e5d23b402b6caf17c107898e0d70","abstract_canon_sha256":"4f4661b1246981a999029be4137d0063c4b351fb2a9df3f31594a1846d1a1d99"},"schema_version":"1.0"},"canonical_sha256":"58de1054dc628ccbfe888ac41da15e1ea34ab230457cd929e46929fa22416a22","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:29:55.110456Z","signature_b64":"HvJkeHN7sxQz7Yd6um6ZQfZy+v2LnxHWq7U97tcRlgeu3/et/tFxRKspiyDbwbECvk3LUuP90kxq15plkTvEDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"58de1054dc628ccbfe888ac41da15e1ea34ab230457cd929e46929fa22416a22","last_reissued_at":"2026-05-18T02:29:55.109997Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:29:55.109997Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1402.7230","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":"2026-05-18T02:29:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Sk6moQgAYVB8Daulm1bgU6kZoYKdJy6FBymnpRY1az6HUY4gYhcV/dhNARGuC4xFaR9g5yjg1U2I3j274fWWAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T11:02:48.467935Z"},"content_sha256":"088648c29f1997e4e15d414701cae06204e5348f041a69d4bb311952625fc68d","schema_version":"1.0","event_id":"sha256:088648c29f1997e4e15d414701cae06204e5348f041a69d4bb311952625fc68d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:LDPBAVG4MKGMX7UIRLCB3IK6D2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Irreversible energy flow in forced Vlasov dynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.space-ph"],"primary_cat":"physics.plasm-ph","authors_text":"G. G. Plunk, J. T. Parker","submitted_at":"2014-02-28T12:53:31Z","abstract_excerpt":"A recent paper [Phys. Plasmas 20, 032304 (2013)] considered the forced linear Vlasov equation as a model for the quasi-steady state of a single stable plasma wavenumber interacting with a bath of turbulent fluctuations. This approach gives some insight into possible energy flows without solving for nonlinear dynamics. The central result of the present work is that the forced linear Vlasov equation exhibits asymptotically zero (irreversible) dissipation to all orders under a detuning of the forcing frequency and the characteristic frequency associated with particle streaming. We first prove thi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.7230","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":"2026-05-18T02:29:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gC2M1qCBaf0CKxOYBt+T85EkJdNE8cHVPdewFIojP8kyY5TSZmh29bRFNINFpRGPEjje3rbY5LqON+CAgKDUCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T11:02:48.468502Z"},"content_sha256":"ed32db3c6492285d48d13feb8fb70bddda5de2e50c892f5abb8db428129d4807","schema_version":"1.0","event_id":"sha256:ed32db3c6492285d48d13feb8fb70bddda5de2e50c892f5abb8db428129d4807"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LDPBAVG4MKGMX7UIRLCB3IK6D2/bundle.json","state_url":"https://pith.science/pith/LDPBAVG4MKGMX7UIRLCB3IK6D2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LDPBAVG4MKGMX7UIRLCB3IK6D2/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":"2026-06-07T11:02:48Z","links":{"resolver":"https://pith.science/pith/LDPBAVG4MKGMX7UIRLCB3IK6D2","bundle":"https://pith.science/pith/LDPBAVG4MKGMX7UIRLCB3IK6D2/bundle.json","state":"https://pith.science/pith/LDPBAVG4MKGMX7UIRLCB3IK6D2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LDPBAVG4MKGMX7UIRLCB3IK6D2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:LDPBAVG4MKGMX7UIRLCB3IK6D2","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":"4f4661b1246981a999029be4137d0063c4b351fb2a9df3f31594a1846d1a1d99","cross_cats_sorted":["physics.space-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2014-02-28T12:53:31Z","title_canon_sha256":"e7bcdadd05c33a257c46804ed074fa817124e5d23b402b6caf17c107898e0d70"},"schema_version":"1.0","source":{"id":"1402.7230","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1402.7230","created_at":"2026-05-18T02:29:55Z"},{"alias_kind":"arxiv_version","alias_value":"1402.7230v2","created_at":"2026-05-18T02:29:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.7230","created_at":"2026-05-18T02:29:55Z"},{"alias_kind":"pith_short_12","alias_value":"LDPBAVG4MKGM","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"LDPBAVG4MKGMX7UI","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"LDPBAVG4","created_at":"2026-05-18T12:28:38Z"}],"graph_snapshots":[{"event_id":"sha256:ed32db3c6492285d48d13feb8fb70bddda5de2e50c892f5abb8db428129d4807","target":"graph","created_at":"2026-05-18T02:29:55Z","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":"A recent paper [Phys. Plasmas 20, 032304 (2013)] considered the forced linear Vlasov equation as a model for the quasi-steady state of a single stable plasma wavenumber interacting with a bath of turbulent fluctuations. This approach gives some insight into possible energy flows without solving for nonlinear dynamics. The central result of the present work is that the forced linear Vlasov equation exhibits asymptotically zero (irreversible) dissipation to all orders under a detuning of the forcing frequency and the characteristic frequency associated with particle streaming. We first prove thi","authors_text":"G. G. Plunk, J. T. Parker","cross_cats":["physics.space-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2014-02-28T12:53:31Z","title":"Irreversible energy flow in forced Vlasov dynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.7230","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":"sha256:088648c29f1997e4e15d414701cae06204e5348f041a69d4bb311952625fc68d","target":"record","created_at":"2026-05-18T02:29:55Z","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":"4f4661b1246981a999029be4137d0063c4b351fb2a9df3f31594a1846d1a1d99","cross_cats_sorted":["physics.space-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2014-02-28T12:53:31Z","title_canon_sha256":"e7bcdadd05c33a257c46804ed074fa817124e5d23b402b6caf17c107898e0d70"},"schema_version":"1.0","source":{"id":"1402.7230","kind":"arxiv","version":2}},"canonical_sha256":"58de1054dc628ccbfe888ac41da15e1ea34ab230457cd929e46929fa22416a22","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"58de1054dc628ccbfe888ac41da15e1ea34ab230457cd929e46929fa22416a22","first_computed_at":"2026-05-18T02:29:55.109997Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:29:55.109997Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"HvJkeHN7sxQz7Yd6um6ZQfZy+v2LnxHWq7U97tcRlgeu3/et/tFxRKspiyDbwbECvk3LUuP90kxq15plkTvEDA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:29:55.110456Z","signed_message":"canonical_sha256_bytes"},"source_id":"1402.7230","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:088648c29f1997e4e15d414701cae06204e5348f041a69d4bb311952625fc68d","sha256:ed32db3c6492285d48d13feb8fb70bddda5de2e50c892f5abb8db428129d4807"],"state_sha256":"1f956e5705ed8a1833344bafb7dbfc53b09c9773735bab01f40d1b27b6e1417c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vI5ZNdrCVJpOn57CsluTHMnmUAF/LeM7ozd1M5peC6P3x7FeOU1eA8n2UHAkUzTMNB1mQyZuDuHQSCFFvSLlAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-07T11:02:48.471220Z","bundle_sha256":"6122f56d7addfc78b7faef847cde981fee750157d6ee91598fc703d46705cbbc"}}