{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:GOSPW2DW7YCAR7MWUNFLACKXC7","short_pith_number":"pith:GOSPW2DW","schema_version":"1.0","canonical_sha256":"33a4fb6876fe0408fd96a34ab0095717dc638bc938b36a032e4e9b301a8f1be2","source":{"kind":"arxiv","id":"2506.05772","version":1},"attestation_state":"computed","paper":{"title":"The polarization of strongly lensed point-like radio sources","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["astro-ph.HE"],"primary_cat":"astro-ph.CO","authors_text":"XinZhong Er","submitted_at":"2025-06-06T05:58:12Z","abstract_excerpt":"Aims. The magnetized medium induces birefringence, splitting the light into two distinct wave modes. The differing propagation speeds of the two modes result in different trajectories. Strong gravitational lensing amplifies the birefringence and introduces an additional geometric rotation on top of the Faraday rotation. We compare the geometric rotation with the Faraday rotation. Methods. We construct the lens equation for massive objects in a magnetized plasma environment, and calculate the time delay difference between the two modes using two toy examples. We present that in the strong lense"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2506.05772","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"astro-ph.CO","submitted_at":"2025-06-06T05:58:12Z","cross_cats_sorted":["astro-ph.HE"],"title_canon_sha256":"49719ebc5854eb090074cd9d0fb1cc68ed4856db37c6bcb75522914d9c0022cd","abstract_canon_sha256":"10f7b55d3a032385d327eb693af96079292c3bd7538341357bf73a278d517d11"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:17:09.532929Z","signature_b64":"viB/q7bVfWXMCXT7pI24Sy797NIKeLa6jVIIcvdURHNRmTYBhk/e75qG8STwNGdvyO1Xb7oFpQhlQPj0QGSlBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"33a4fb6876fe0408fd96a34ab0095717dc638bc938b36a032e4e9b301a8f1be2","last_reissued_at":"2026-07-05T11:17:09.531601Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:17:09.531601Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The polarization of strongly lensed point-like radio sources","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["astro-ph.HE"],"primary_cat":"astro-ph.CO","authors_text":"XinZhong Er","submitted_at":"2025-06-06T05:58:12Z","abstract_excerpt":"Aims. The magnetized medium induces birefringence, splitting the light into two distinct wave modes. The differing propagation speeds of the two modes result in different trajectories. Strong gravitational lensing amplifies the birefringence and introduces an additional geometric rotation on top of the Faraday rotation. We compare the geometric rotation with the Faraday rotation. Methods. We construct the lens equation for massive objects in a magnetized plasma environment, and calculate the time delay difference between the two modes using two toy examples. We present that in the strong lense"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.05772","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2506.05772/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2506.05772","created_at":"2026-07-05T11:17:09.532333+00:00"},{"alias_kind":"arxiv_version","alias_value":"2506.05772v1","created_at":"2026-07-05T11:17:09.532333+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.05772","created_at":"2026-07-05T11:17:09.532333+00:00"},{"alias_kind":"pith_short_12","alias_value":"GOSPW2DW7YCA","created_at":"2026-07-05T11:17:09.532333+00:00"},{"alias_kind":"pith_short_16","alias_value":"GOSPW2DW7YCAR7MW","created_at":"2026-07-05T11:17:09.532333+00:00"},{"alias_kind":"pith_short_8","alias_value":"GOSPW2DW","created_at":"2026-07-05T11:17:09.532333+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GOSPW2DW7YCAR7MWUNFLACKXC7","json":"https://pith.science/pith/GOSPW2DW7YCAR7MWUNFLACKXC7.json","graph_json":"https://pith.science/api/pith-number/GOSPW2DW7YCAR7MWUNFLACKXC7/graph.json","events_json":"https://pith.science/api/pith-number/GOSPW2DW7YCAR7MWUNFLACKXC7/events.json","paper":"https://pith.science/paper/GOSPW2DW"},"agent_actions":{"view_html":"https://pith.science/pith/GOSPW2DW7YCAR7MWUNFLACKXC7","download_json":"https://pith.science/pith/GOSPW2DW7YCAR7MWUNFLACKXC7.json","view_paper":"https://pith.science/paper/GOSPW2DW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2506.05772&json=true","fetch_graph":"https://pith.science/api/pith-number/GOSPW2DW7YCAR7MWUNFLACKXC7/graph.json","fetch_events":"https://pith.science/api/pith-number/GOSPW2DW7YCAR7MWUNFLACKXC7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GOSPW2DW7YCAR7MWUNFLACKXC7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GOSPW2DW7YCAR7MWUNFLACKXC7/action/storage_attestation","attest_author":"https://pith.science/pith/GOSPW2DW7YCAR7MWUNFLACKXC7/action/author_attestation","sign_citation":"https://pith.science/pith/GOSPW2DW7YCAR7MWUNFLACKXC7/action/citation_signature","submit_replication":"https://pith.science/pith/GOSPW2DW7YCAR7MWUNFLACKXC7/action/replication_record"}},"created_at":"2026-07-05T11:17:09.532333+00:00","updated_at":"2026-07-05T11:17:09.532333+00:00"}