{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:NQE6WQQ2KXVZ5H3PFFKTEPZ4BQ","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":"b9eb25b6b60aae0d8c01f03a8c9818a31f3bc64f4eefcd97df01a921f5542ac3","cross_cats_sorted":["astro-ph.HE","physics.plasm-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-02-18T16:05:41Z","title_canon_sha256":"354433065f3b6322a571dfbe8f8a97581342be529fd1feaa2d55b55440351e0d"},"schema_version":"1.0","source":{"id":"2502.12983","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2502.12983","created_at":"2026-07-05T10:16:27Z"},{"alias_kind":"arxiv_version","alias_value":"2502.12983v1","created_at":"2026-07-05T10:16:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.12983","created_at":"2026-07-05T10:16:27Z"},{"alias_kind":"pith_short_12","alias_value":"NQE6WQQ2KXVZ","created_at":"2026-07-05T10:16:27Z"},{"alias_kind":"pith_short_16","alias_value":"NQE6WQQ2KXVZ5H3P","created_at":"2026-07-05T10:16:27Z"},{"alias_kind":"pith_short_8","alias_value":"NQE6WQQ2","created_at":"2026-07-05T10:16:27Z"}],"graph_snapshots":[{"event_id":"sha256:4159fc7204c4c4b53c5a78c88016e5571450f04cefff7bec5cd3bb021fe80eba","target":"graph","created_at":"2026-07-05T10:16:27Z","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/2502.12983/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Resonant axion-plasmon conversion in the magnetospheres of magnetars may substantially impact the landscape of dark-matter axion detection. This work explores how resonant axion-plasmon conversion, through a mechanism that is analogous to the Mikheyev-Smirnov-Wolfenstein (NSW) effect in neutrinos, modify the expected radio signals from axion-photon conversions observed on Earth. Critically, the resonant conversion radius lies within the region expected for axion-photon conversion, introducing a nonradiative power loss that diminishes the anticipated photon flux. Our analysis demonstrates that ","authors_text":"H. Ter\\c{c}as, J. T. Mendon\\c{c}a, R. Bingham","cross_cats":["astro-ph.HE","physics.plasm-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-02-18T16:05:41Z","title":"Resonant axion-plasmon conversion in neutron star magnetospheres"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.12983","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:ddc629b5e1f8ffc03181be638a0cd1d458fb801f515c6e13c6bddb20473d921f","target":"record","created_at":"2026-07-05T10:16:27Z","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":"b9eb25b6b60aae0d8c01f03a8c9818a31f3bc64f4eefcd97df01a921f5542ac3","cross_cats_sorted":["astro-ph.HE","physics.plasm-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-02-18T16:05:41Z","title_canon_sha256":"354433065f3b6322a571dfbe8f8a97581342be529fd1feaa2d55b55440351e0d"},"schema_version":"1.0","source":{"id":"2502.12983","kind":"arxiv","version":1}},"canonical_sha256":"6c09eb421a55eb9e9f6f2955323f3c0c2654b0d0db623d76e5a5aa9c3fd9bb21","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6c09eb421a55eb9e9f6f2955323f3c0c2654b0d0db623d76e5a5aa9c3fd9bb21","first_computed_at":"2026-07-05T10:16:27.522169Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:16:27.522169Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"67UOJbRdn9pgYNz04jyq4ug7GtT7fBtj/PWoQJ4LNO7i8eDOdTZ4ORZdK3/44QsPg1slskBIW+kIC2lAPq0GBw==","signature_status":"signed_v1","signed_at":"2026-07-05T10:16:27.522819Z","signed_message":"canonical_sha256_bytes"},"source_id":"2502.12983","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ddc629b5e1f8ffc03181be638a0cd1d458fb801f515c6e13c6bddb20473d921f","sha256:4159fc7204c4c4b53c5a78c88016e5571450f04cefff7bec5cd3bb021fe80eba"],"state_sha256":"4d6a3a452e5c7b385a5e44ee8d1611dcc8fc475505c45ae747e2d848667cde23"}