{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:CAPB6OPOLLWTUKROTZUPGKZ5A4","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":"efadee7ee92ba4f3c5a304daf6adbd2ffe4281842ae4ef1c4785075ce6cb1c5b","cross_cats_sorted":["hep-ex","physics.geo-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-01-13T17:45:33Z","title_canon_sha256":"a8e61fc8eac4c8e5889f7d603616b454dfb9e18ec94b9b0c235c082c3e9391a4"},"schema_version":"1.0","source":{"id":"2501.07621","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2501.07621","created_at":"2026-07-05T10:00:47Z"},{"alias_kind":"arxiv_version","alias_value":"2501.07621v1","created_at":"2026-07-05T10:00:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.07621","created_at":"2026-07-05T10:00:47Z"},{"alias_kind":"pith_short_12","alias_value":"CAPB6OPOLLWT","created_at":"2026-07-05T10:00:47Z"},{"alias_kind":"pith_short_16","alias_value":"CAPB6OPOLLWTUKRO","created_at":"2026-07-05T10:00:47Z"},{"alias_kind":"pith_short_8","alias_value":"CAPB6OPO","created_at":"2026-07-05T10:00:47Z"}],"graph_snapshots":[{"event_id":"sha256:1203cad9b9c38bab4d073c1ebaec85b2004541af8c55e50c17c328de34a7509e","target":"graph","created_at":"2026-07-05T10:00:47Z","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/2501.07621/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Atmospheric neutrinos, through their weak interactions, can serve as an independent tool for exploring the internal structure of Earth. The information obtained would be complementary to that provided by seismic and gravitational measurements. The Earth matter effects in neutrino oscillations depend upon the energy of neutrinos and the electron density distribution that they encounter during their journey through Earth, and hence, can be used to probe the inner structure of Earth. In this contribution, we demonstrate how well an atmospheric neutrino experiment, such as an iron calorimeter dete","authors_text":"Amol Dighe, Anil Kumar, Anuj Kumar Upadhyay, Sanjib Kumar Agarwalla","cross_cats":["hep-ex","physics.geo-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-01-13T17:45:33Z","title":"Exploring constraints on the core radius and density jumps inside Earth using atmospheric neutrino oscillations"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2501.07621","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":"sha256:37f7bc7945f4d168cc2ed2ece47a7f4c643467de26e78f94412591def56d492c","target":"record","created_at":"2026-07-05T10:00:47Z","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":"efadee7ee92ba4f3c5a304daf6adbd2ffe4281842ae4ef1c4785075ce6cb1c5b","cross_cats_sorted":["hep-ex","physics.geo-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-01-13T17:45:33Z","title_canon_sha256":"a8e61fc8eac4c8e5889f7d603616b454dfb9e18ec94b9b0c235c082c3e9391a4"},"schema_version":"1.0","source":{"id":"2501.07621","kind":"arxiv","version":1}},"canonical_sha256":"101e1f39ee5aed3a2a2e9e68f32b3d072f935f0ff799658371ab6e18e6fd739e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"101e1f39ee5aed3a2a2e9e68f32b3d072f935f0ff799658371ab6e18e6fd739e","first_computed_at":"2026-07-05T10:00:47.801021Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:00:47.801021Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"s/LRCIa/gsAfbNti0Sskk7aT4M1AsjdNNJVpbap8r7GqSGsa35OxVGCR9nAvylYlQRkAMBPI+aWCg72asGd5DQ==","signature_status":"signed_v1","signed_at":"2026-07-05T10:00:47.801516Z","signed_message":"canonical_sha256_bytes"},"source_id":"2501.07621","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:37f7bc7945f4d168cc2ed2ece47a7f4c643467de26e78f94412591def56d492c","sha256:1203cad9b9c38bab4d073c1ebaec85b2004541af8c55e50c17c328de34a7509e"],"state_sha256":"815896d9f1fff8289b6e2f10969047f0ec94ed23c19bf00dcb278bc1a84a0eb0"}