{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:NBFFPJQQM7GQ3PDKOHSS6FFQV6","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":"6794ea4adc79ece54b28a5b24fcc68b9c965eb26e459e3abe8530d8f1d239a27","cross_cats_sorted":["physics.space-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"astro-ph.SR","submitted_at":"2023-12-21T17:04:16Z","title_canon_sha256":"7ebc7418d958d90cc4e4a09daf25644e18ebd4ee9b883aba7c0073944a16d12f"},"schema_version":"1.0","source":{"id":"2312.14039","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2312.14039","created_at":"2026-07-05T07:26:59Z"},{"alias_kind":"arxiv_version","alias_value":"2312.14039v1","created_at":"2026-07-05T07:26:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2312.14039","created_at":"2026-07-05T07:26:59Z"},{"alias_kind":"pith_short_12","alias_value":"NBFFPJQQM7GQ","created_at":"2026-07-05T07:26:59Z"},{"alias_kind":"pith_short_16","alias_value":"NBFFPJQQM7GQ3PDK","created_at":"2026-07-05T07:26:59Z"},{"alias_kind":"pith_short_8","alias_value":"NBFFPJQQ","created_at":"2026-07-05T07:26:59Z"}],"graph_snapshots":[{"event_id":"sha256:be4222f9c8133d19db8a0b9b36983b17ec9cda392ae69c2e460d1cd1819a7f29","target":"graph","created_at":"2026-07-05T07:26:59Z","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/2312.14039/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present a study of the influence of solar UV anisotropy on the heliospheric backscatter helioglow generated by resonant scattering of solar Lyman-alpha photons on interstellar hydrogen atoms around the Sun. Simulations based on the WawHelioGlow model suggest that the response of the helioglow pole-to-ecliptic ratio to the anisotropy is linear, but 15% of the anisotropy (polar darkening) generates 30-40% change in the ratio in the solar minimum and 15-20% in the solar maximum. We attribute this difference to an interplay between the solar UV anisotropy and the latitudinal structure of the so","authors_text":"M. A. Kubiak, M. Bzowski, M. Strumik","cross_cats":["physics.space-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"astro-ph.SR","submitted_at":"2023-12-21T17:04:16Z","title":"Effects of Heliolatitudinal Anisotropy of Solar FUV/EUV Emissions on Lyman-alpha Helioglow"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2312.14039","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:ffd808badfe7fe64f2e4f853daca8f57f65b919d70dc3bae64964091c48fd84a","target":"record","created_at":"2026-07-05T07:26:59Z","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":"6794ea4adc79ece54b28a5b24fcc68b9c965eb26e459e3abe8530d8f1d239a27","cross_cats_sorted":["physics.space-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"astro-ph.SR","submitted_at":"2023-12-21T17:04:16Z","title_canon_sha256":"7ebc7418d958d90cc4e4a09daf25644e18ebd4ee9b883aba7c0073944a16d12f"},"schema_version":"1.0","source":{"id":"2312.14039","kind":"arxiv","version":1}},"canonical_sha256":"684a57a61067cd0dbc6a71e52f14b0af8f61ec0fe6d5987837cfa49944b07d3b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"684a57a61067cd0dbc6a71e52f14b0af8f61ec0fe6d5987837cfa49944b07d3b","first_computed_at":"2026-07-05T07:26:59.583882Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T07:26:59.583882Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"0UBe04LefFJDLyDp/hi4SKORZSgNaY97crBfOxEYz42+l8M2soeY76yPietGeXIB5O/hVUxx+znc+sM//nAyAQ==","signature_status":"signed_v1","signed_at":"2026-07-05T07:26:59.584298Z","signed_message":"canonical_sha256_bytes"},"source_id":"2312.14039","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ffd808badfe7fe64f2e4f853daca8f57f65b919d70dc3bae64964091c48fd84a","sha256:be4222f9c8133d19db8a0b9b36983b17ec9cda392ae69c2e460d1cd1819a7f29"],"state_sha256":"57a488eacee5817c13d5456fb28ceea6a880d001c07d003cc60718cfa3b5c0b3"}