{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2020:CZ6RB5OZ7E2K3DVP27EBUJPJPN","short_pith_number":"pith:CZ6RB5OZ","canonical_record":{"source":{"id":"2002.02243","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2020-02-06T13:17:08Z","cross_cats_sorted":["physics.space-ph"],"title_canon_sha256":"e4b04bd8548f79fb88211d4d8c2bd3f32a12cbe2183ae86611f145a4498590cf","abstract_canon_sha256":"dab71b4fc1c8b3afc2a14269f09e5bad7131aa7b46b92a710653ca9d92fd91b7"},"schema_version":"1.0"},"canonical_sha256":"167d10f5d9f934ad8eafd7c81a25e97b56d0de9e3b92e7e0a4b39e3287b53c91","source":{"kind":"arxiv","id":"2002.02243","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2002.02243","created_at":"2026-07-05T00:45:22Z"},{"alias_kind":"arxiv_version","alias_value":"2002.02243v1","created_at":"2026-07-05T00:45:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2002.02243","created_at":"2026-07-05T00:45:22Z"},{"alias_kind":"pith_short_12","alias_value":"CZ6RB5OZ7E2K","created_at":"2026-07-05T00:45:22Z"},{"alias_kind":"pith_short_16","alias_value":"CZ6RB5OZ7E2K3DVP","created_at":"2026-07-05T00:45:22Z"},{"alias_kind":"pith_short_8","alias_value":"CZ6RB5OZ","created_at":"2026-07-05T00:45:22Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2020:CZ6RB5OZ7E2K3DVP27EBUJPJPN","target":"record","payload":{"canonical_record":{"source":{"id":"2002.02243","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2020-02-06T13:17:08Z","cross_cats_sorted":["physics.space-ph"],"title_canon_sha256":"e4b04bd8548f79fb88211d4d8c2bd3f32a12cbe2183ae86611f145a4498590cf","abstract_canon_sha256":"dab71b4fc1c8b3afc2a14269f09e5bad7131aa7b46b92a710653ca9d92fd91b7"},"schema_version":"1.0"},"canonical_sha256":"167d10f5d9f934ad8eafd7c81a25e97b56d0de9e3b92e7e0a4b39e3287b53c91","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:45:22.798088Z","signature_b64":"PgKgxxpnxjWOjC31NzhQilpRn788b+fCr7OrhHZKh0ubisAp9pWDPP7xvG94Jy8G8ZpHcqZyYwGo9lBW19RQAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"167d10f5d9f934ad8eafd7c81a25e97b56d0de9e3b92e7e0a4b39e3287b53c91","last_reissued_at":"2026-07-05T00:45:22.797591Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:45:22.797591Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2002.02243","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":"2026-07-05T00:45:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"U35kMPrKy13wRwGcTJyFH5capr+L2eHH2Ac+7c7/gK8nKaGNCIcDoQeateod+91z2cSre4OYSBPt1xQnI5tNCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T22:09:18.941713Z"},"content_sha256":"2c39a3f97ba7f932fbbfdd5b01bac021daf13f8d1843591b59fb4204142032c2","schema_version":"1.0","event_id":"sha256:2c39a3f97ba7f932fbbfdd5b01bac021daf13f8d1843591b59fb4204142032c2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2020:CZ6RB5OZ7E2K3DVP27EBUJPJPN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Simulation of plasmaspheric plume impact on dayside magnetic reconnection","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.space-ph"],"primary_cat":"physics.plasm-ph","authors_text":"Beno\\^it Lavraud, Francesco Califano, J\\'er\\'emy Dargent, Nicolas Aunai, Sergio Toledo-Redondo","submitted_at":"2020-02-06T13:17:08Z","abstract_excerpt":"During periods of strong magnetic activity, cold dense plasma from the plasmasphere typically forms a plume extending towards the dayside magnetopause, eventually reaching it. In this work, we present a large-scale two-dimensional fully kinetic Particle-In-Cell simulation of a reconnecting magnetopause hit by a propagating plasmaspheric plume. The simulation is designed so that it undergoes four distinct phases: initial unsteady state, steady state prior to plume arrival at the magnetospause, plume interaction and steady state once the plume is well engulfed in the reconnection site. We show t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2002.02243","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/2002.02243/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":"2026-07-05T00:45:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wESL4/ctQzED/17UsEVHhiIKoeCS0bM3tLSzDjGbqlc5WHsDnxvzIBQ0VSjpbd0rybWmW/O/iZ4PWqn1XKudBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T22:09:18.942312Z"},"content_sha256":"2511c9e1ab0a687c0c7ac47b9a53b3d46115b5a67fda435e9055dd3fff7e6525","schema_version":"1.0","event_id":"sha256:2511c9e1ab0a687c0c7ac47b9a53b3d46115b5a67fda435e9055dd3fff7e6525"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/CZ6RB5OZ7E2K3DVP27EBUJPJPN/bundle.json","state_url":"https://pith.science/pith/CZ6RB5OZ7E2K3DVP27EBUJPJPN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/CZ6RB5OZ7E2K3DVP27EBUJPJPN/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":"2026-08-13T22:09:18Z","links":{"resolver":"https://pith.science/pith/CZ6RB5OZ7E2K3DVP27EBUJPJPN","bundle":"https://pith.science/pith/CZ6RB5OZ7E2K3DVP27EBUJPJPN/bundle.json","state":"https://pith.science/pith/CZ6RB5OZ7E2K3DVP27EBUJPJPN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/CZ6RB5OZ7E2K3DVP27EBUJPJPN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2020:CZ6RB5OZ7E2K3DVP27EBUJPJPN","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":"dab71b4fc1c8b3afc2a14269f09e5bad7131aa7b46b92a710653ca9d92fd91b7","cross_cats_sorted":["physics.space-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2020-02-06T13:17:08Z","title_canon_sha256":"e4b04bd8548f79fb88211d4d8c2bd3f32a12cbe2183ae86611f145a4498590cf"},"schema_version":"1.0","source":{"id":"2002.02243","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2002.02243","created_at":"2026-07-05T00:45:22Z"},{"alias_kind":"arxiv_version","alias_value":"2002.02243v1","created_at":"2026-07-05T00:45:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2002.02243","created_at":"2026-07-05T00:45:22Z"},{"alias_kind":"pith_short_12","alias_value":"CZ6RB5OZ7E2K","created_at":"2026-07-05T00:45:22Z"},{"alias_kind":"pith_short_16","alias_value":"CZ6RB5OZ7E2K3DVP","created_at":"2026-07-05T00:45:22Z"},{"alias_kind":"pith_short_8","alias_value":"CZ6RB5OZ","created_at":"2026-07-05T00:45:22Z"}],"graph_snapshots":[{"event_id":"sha256:2511c9e1ab0a687c0c7ac47b9a53b3d46115b5a67fda435e9055dd3fff7e6525","target":"graph","created_at":"2026-07-05T00:45:22Z","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/2002.02243/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"During periods of strong magnetic activity, cold dense plasma from the plasmasphere typically forms a plume extending towards the dayside magnetopause, eventually reaching it. In this work, we present a large-scale two-dimensional fully kinetic Particle-In-Cell simulation of a reconnecting magnetopause hit by a propagating plasmaspheric plume. The simulation is designed so that it undergoes four distinct phases: initial unsteady state, steady state prior to plume arrival at the magnetospause, plume interaction and steady state once the plume is well engulfed in the reconnection site. We show t","authors_text":"Beno\\^it Lavraud, Francesco Califano, J\\'er\\'emy Dargent, Nicolas Aunai, Sergio Toledo-Redondo","cross_cats":["physics.space-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2020-02-06T13:17:08Z","title":"Simulation of plasmaspheric plume impact on dayside magnetic reconnection"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2002.02243","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":"sha256:2c39a3f97ba7f932fbbfdd5b01bac021daf13f8d1843591b59fb4204142032c2","target":"record","created_at":"2026-07-05T00:45:22Z","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":"dab71b4fc1c8b3afc2a14269f09e5bad7131aa7b46b92a710653ca9d92fd91b7","cross_cats_sorted":["physics.space-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2020-02-06T13:17:08Z","title_canon_sha256":"e4b04bd8548f79fb88211d4d8c2bd3f32a12cbe2183ae86611f145a4498590cf"},"schema_version":"1.0","source":{"id":"2002.02243","kind":"arxiv","version":1}},"canonical_sha256":"167d10f5d9f934ad8eafd7c81a25e97b56d0de9e3b92e7e0a4b39e3287b53c91","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"167d10f5d9f934ad8eafd7c81a25e97b56d0de9e3b92e7e0a4b39e3287b53c91","first_computed_at":"2026-07-05T00:45:22.797591Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T00:45:22.797591Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"PgKgxxpnxjWOjC31NzhQilpRn788b+fCr7OrhHZKh0ubisAp9pWDPP7xvG94Jy8G8ZpHcqZyYwGo9lBW19RQAw==","signature_status":"signed_v1","signed_at":"2026-07-05T00:45:22.798088Z","signed_message":"canonical_sha256_bytes"},"source_id":"2002.02243","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2c39a3f97ba7f932fbbfdd5b01bac021daf13f8d1843591b59fb4204142032c2","sha256:2511c9e1ab0a687c0c7ac47b9a53b3d46115b5a67fda435e9055dd3fff7e6525"],"state_sha256":"95e4206d7c8fb6bf2860e5c34b9abca69aeddf03e39713ab96ecc8927e874f74"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Z+fHpgtVzgJbIlDkMSZk/qqbLTaMzbA7yjsj2nJiIoDsDznNC6+BeNMM1UmNd06eTfMW5xH2w1fQI/qTsRyqBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-13T22:09:18.954016Z","bundle_sha256":"af59862739671d5d91a2ae1e4358b3fa5299cd6093294db65493d7f1f883bcbe"}}