{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:HYTI4GWN74MNEAIHV76HYEZODV","short_pith_number":"pith:HYTI4GWN","canonical_record":{"source":{"id":"1706.05110","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.SR","submitted_at":"2017-06-15T22:53:25Z","cross_cats_sorted":["astro-ph.HE"],"title_canon_sha256":"f2c1d756ab6b1b77dd59a28f483af76633f0bf7d66dd81420c49247fc5c8de51","abstract_canon_sha256":"ad45147b1fd2d3cb29a58ea2dab12ec071efd424bee74062c1736db83ccd64f9"},"schema_version":"1.0"},"canonical_sha256":"3e268e1acdff18d20107affc7c132e1d71a47f31c20851d0f8eefeb4bb33313a","source":{"kind":"arxiv","id":"1706.05110","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.05110","created_at":"2026-05-18T00:38:50Z"},{"alias_kind":"arxiv_version","alias_value":"1706.05110v1","created_at":"2026-05-18T00:38:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.05110","created_at":"2026-05-18T00:38:50Z"},{"alias_kind":"pith_short_12","alias_value":"HYTI4GWN74MN","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_16","alias_value":"HYTI4GWN74MNEAIH","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_8","alias_value":"HYTI4GWN","created_at":"2026-05-18T12:31:21Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:HYTI4GWN74MNEAIHV76HYEZODV","target":"record","payload":{"canonical_record":{"source":{"id":"1706.05110","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.SR","submitted_at":"2017-06-15T22:53:25Z","cross_cats_sorted":["astro-ph.HE"],"title_canon_sha256":"f2c1d756ab6b1b77dd59a28f483af76633f0bf7d66dd81420c49247fc5c8de51","abstract_canon_sha256":"ad45147b1fd2d3cb29a58ea2dab12ec071efd424bee74062c1736db83ccd64f9"},"schema_version":"1.0"},"canonical_sha256":"3e268e1acdff18d20107affc7c132e1d71a47f31c20851d0f8eefeb4bb33313a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:38:50.952120Z","signature_b64":"dLwJ3DmrTRc5XfO4RSByzfGfnVGOj2gpzLzVxXMLnxo8+6WeBwMet9cVebet3vQ4+FQ0JDMCOiGo6A76DozfDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3e268e1acdff18d20107affc7c132e1d71a47f31c20851d0f8eefeb4bb33313a","last_reissued_at":"2026-05-18T00:38:50.951609Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:38:50.951609Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1706.05110","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":"2026-05-18T00:38:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"eJ7VwRX6UP9SIIDyQF/BzeTythPuCHm8YRKL8MDqURV82PO7DlNLS4d2/RN7yZ6bexjyl94+jTCohSSXvxPUBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T17:46:40.376497Z"},"content_sha256":"4488bae7e4e914abac343fab3d7b23e90acc5f1f619f0582575881ade9c4e1a8","schema_version":"1.0","event_id":"sha256:4488bae7e4e914abac343fab3d7b23e90acc5f1f619f0582575881ade9c4e1a8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:HYTI4GWN74MNEAIHV76HYEZODV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"MAGNUS: A new resistive MHD code with heat flow terms","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.HE"],"primary_cat":"astro-ph.SR","authors_text":"Anamar\\'ia Navarro, F. D. Lora-Clavijo, Guillermo A. Gonz\\'alez","submitted_at":"2017-06-15T22:53:25Z","abstract_excerpt":"We present a new magnetohydrodynamic (MHD) code for the simulation of wave propagation in the solar atmosphere, under the effects of electrical resistivity, but not dominant, and heat transference in a uniform 3D grid. The code is based on the finite volume method combined with the HLLE and HLLC approximate Riemann solvers, which use different slope limiters like MINMOD, MC, and WENO5. In order to control the growth of the divergence of the magnetic field, due to numerical errors, we apply the Flux Constrained Transport method, which is described in detail to understand how the resistive terms"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.05110","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":"2026-05-18T00:38:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"clr1rkp7w5PNmzR++takGL39aVJiJAdjr1ZqF6bxZjp4S0vZn1DYUFSrjQ5DgoIsEKoDvJmIc+H4vdc5C/kLBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T17:46:40.377187Z"},"content_sha256":"fe2163645b4f04e91cb4ea1a9e5f14936ea277073a05234855ae44b21e6aab91","schema_version":"1.0","event_id":"sha256:fe2163645b4f04e91cb4ea1a9e5f14936ea277073a05234855ae44b21e6aab91"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HYTI4GWN74MNEAIHV76HYEZODV/bundle.json","state_url":"https://pith.science/pith/HYTI4GWN74MNEAIHV76HYEZODV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HYTI4GWN74MNEAIHV76HYEZODV/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":"2026-05-25T17:46:40Z","links":{"resolver":"https://pith.science/pith/HYTI4GWN74MNEAIHV76HYEZODV","bundle":"https://pith.science/pith/HYTI4GWN74MNEAIHV76HYEZODV/bundle.json","state":"https://pith.science/pith/HYTI4GWN74MNEAIHV76HYEZODV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HYTI4GWN74MNEAIHV76HYEZODV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:HYTI4GWN74MNEAIHV76HYEZODV","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":"ad45147b1fd2d3cb29a58ea2dab12ec071efd424bee74062c1736db83ccd64f9","cross_cats_sorted":["astro-ph.HE"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.SR","submitted_at":"2017-06-15T22:53:25Z","title_canon_sha256":"f2c1d756ab6b1b77dd59a28f483af76633f0bf7d66dd81420c49247fc5c8de51"},"schema_version":"1.0","source":{"id":"1706.05110","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.05110","created_at":"2026-05-18T00:38:50Z"},{"alias_kind":"arxiv_version","alias_value":"1706.05110v1","created_at":"2026-05-18T00:38:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.05110","created_at":"2026-05-18T00:38:50Z"},{"alias_kind":"pith_short_12","alias_value":"HYTI4GWN74MN","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_16","alias_value":"HYTI4GWN74MNEAIH","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_8","alias_value":"HYTI4GWN","created_at":"2026-05-18T12:31:21Z"}],"graph_snapshots":[{"event_id":"sha256:fe2163645b4f04e91cb4ea1a9e5f14936ea277073a05234855ae44b21e6aab91","target":"graph","created_at":"2026-05-18T00:38:50Z","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":"We present a new magnetohydrodynamic (MHD) code for the simulation of wave propagation in the solar atmosphere, under the effects of electrical resistivity, but not dominant, and heat transference in a uniform 3D grid. The code is based on the finite volume method combined with the HLLE and HLLC approximate Riemann solvers, which use different slope limiters like MINMOD, MC, and WENO5. In order to control the growth of the divergence of the magnetic field, due to numerical errors, we apply the Flux Constrained Transport method, which is described in detail to understand how the resistive terms","authors_text":"Anamar\\'ia Navarro, F. D. Lora-Clavijo, Guillermo A. Gonz\\'alez","cross_cats":["astro-ph.HE"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.SR","submitted_at":"2017-06-15T22:53:25Z","title":"MAGNUS: A new resistive MHD code with heat flow terms"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.05110","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":"sha256:4488bae7e4e914abac343fab3d7b23e90acc5f1f619f0582575881ade9c4e1a8","target":"record","created_at":"2026-05-18T00:38:50Z","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":"ad45147b1fd2d3cb29a58ea2dab12ec071efd424bee74062c1736db83ccd64f9","cross_cats_sorted":["astro-ph.HE"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.SR","submitted_at":"2017-06-15T22:53:25Z","title_canon_sha256":"f2c1d756ab6b1b77dd59a28f483af76633f0bf7d66dd81420c49247fc5c8de51"},"schema_version":"1.0","source":{"id":"1706.05110","kind":"arxiv","version":1}},"canonical_sha256":"3e268e1acdff18d20107affc7c132e1d71a47f31c20851d0f8eefeb4bb33313a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3e268e1acdff18d20107affc7c132e1d71a47f31c20851d0f8eefeb4bb33313a","first_computed_at":"2026-05-18T00:38:50.951609Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:38:50.951609Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"dLwJ3DmrTRc5XfO4RSByzfGfnVGOj2gpzLzVxXMLnxo8+6WeBwMet9cVebet3vQ4+FQ0JDMCOiGo6A76DozfDA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:38:50.952120Z","signed_message":"canonical_sha256_bytes"},"source_id":"1706.05110","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4488bae7e4e914abac343fab3d7b23e90acc5f1f619f0582575881ade9c4e1a8","sha256:fe2163645b4f04e91cb4ea1a9e5f14936ea277073a05234855ae44b21e6aab91"],"state_sha256":"8676bd6e8e06ae4cd7e07bd47cda75ac0f4d5054a1eb8eb96bd3ffa27e0e1c76"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fxdkWk5GrwFWu2Y4ky3RrN0swuUywz8ctnPFqJ9Q+Jizs7+7qXm51547o2Rxfxhhzmzj0YoSR2dAT94wDCbaAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T17:46:40.380944Z","bundle_sha256":"b68828f993b3a988f50a33214043aae05ba90377793d820bca0e2059aea36fad"}}