{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:73NC65W56MNENDRQB67ZF3KZE7","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":"69a22cb182a333c45bfbd598304c8d206df617bd322dbca136ceab2ceecc7785","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2018-10-30T09:41:20Z","title_canon_sha256":"feb68d4f86251f13fd0a10f380cf4cb365278340e92ae751593cad267b83da2a"},"schema_version":"1.0","source":{"id":"1810.12605","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1810.12605","created_at":"2026-05-17T23:54:10Z"},{"alias_kind":"arxiv_version","alias_value":"1810.12605v1","created_at":"2026-05-17T23:54:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1810.12605","created_at":"2026-05-17T23:54:10Z"},{"alias_kind":"pith_short_12","alias_value":"73NC65W56MNE","created_at":"2026-05-18T12:32:11Z"},{"alias_kind":"pith_short_16","alias_value":"73NC65W56MNENDRQ","created_at":"2026-05-18T12:32:11Z"},{"alias_kind":"pith_short_8","alias_value":"73NC65W5","created_at":"2026-05-18T12:32:11Z"}],"graph_snapshots":[{"event_id":"sha256:aabd05eec9c9ae43138a2cb203285006df8fc5adde1a4d09c157186db66ff19c","target":"graph","created_at":"2026-05-17T23:54:10Z","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":"Nonlinear and low-frequency solitary waves are investigated in the framework of the one-dimensional Hall-magnetohydrodynamic model with finite Larmor effects and a double adiabatic model for plasma pressures. The organization of these localized structures in terms of the propagation angle with respect to the ambient magnetic field $\\theta$ and the propagation velocity $C$ is discussed. There are three types of regions in the $\\theta-C$ plane that correspond to domains where either solitary waves cannot exist, are organized in branches, or have a continuous spectrum. A numerical method valid fo","authors_text":"D. Laveder, E. Bello-Ben\\'itez, E. Siminos, G. S\\'anchez-Arriaga, T. Passot","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2018-10-30T09:41:20Z","title":"Structure and evolution of magnetohydrodynamic solitary waves with Hall and finite Larmor radius effects"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1810.12605","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:c470afc76aecb1793704ee627f12eed038176e0e122af79c9323f08446bbfabd","target":"record","created_at":"2026-05-17T23:54:10Z","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":"69a22cb182a333c45bfbd598304c8d206df617bd322dbca136ceab2ceecc7785","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2018-10-30T09:41:20Z","title_canon_sha256":"feb68d4f86251f13fd0a10f380cf4cb365278340e92ae751593cad267b83da2a"},"schema_version":"1.0","source":{"id":"1810.12605","kind":"arxiv","version":1}},"canonical_sha256":"feda2f76ddf31a468e300fbf92ed5927cfba19fdb6361d4d3f2d5a268fc26d18","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"feda2f76ddf31a468e300fbf92ed5927cfba19fdb6361d4d3f2d5a268fc26d18","first_computed_at":"2026-05-17T23:54:10.639637Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:54:10.639637Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Ehs4+Jfr8PdXhhjuxP5G+1aRnwXvw5qDWfefs4HjuVbzVapx901CuH8z6bnZWXexBwqpPlNzDcnqPjpUwiP5BQ==","signature_status":"signed_v1","signed_at":"2026-05-17T23:54:10.640103Z","signed_message":"canonical_sha256_bytes"},"source_id":"1810.12605","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c470afc76aecb1793704ee627f12eed038176e0e122af79c9323f08446bbfabd","sha256:aabd05eec9c9ae43138a2cb203285006df8fc5adde1a4d09c157186db66ff19c"],"state_sha256":"d5742206804d70a74639649dbadd45e40396c310f16f6da616db32caba1e2ac7"}