{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:TFRQBZNCZ3JVP4UWNPFEZYAGHK","short_pith_number":"pith:TFRQBZNC","canonical_record":{"source":{"id":"1401.4108","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2014-01-16T18:04:52Z","cross_cats_sorted":[],"title_canon_sha256":"f61dca10cc3168645e3b2bc4b18b1e2c253d9f0debe899360f331831b459c7d3","abstract_canon_sha256":"85c062a37f1176ffe5e3a9654028af335cc4093962108a61193d65bbea0cd2da"},"schema_version":"1.0"},"canonical_sha256":"996300e5a2ced357f2966bca4ce0063a9d8154b240d4ce3e22a92731a3f343f4","source":{"kind":"arxiv","id":"1401.4108","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1401.4108","created_at":"2026-05-18T01:45:24Z"},{"alias_kind":"arxiv_version","alias_value":"1401.4108v1","created_at":"2026-05-18T01:45:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.4108","created_at":"2026-05-18T01:45:24Z"},{"alias_kind":"pith_short_12","alias_value":"TFRQBZNCZ3JV","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_16","alias_value":"TFRQBZNCZ3JVP4UW","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_8","alias_value":"TFRQBZNC","created_at":"2026-05-18T12:28:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:TFRQBZNCZ3JVP4UWNPFEZYAGHK","target":"record","payload":{"canonical_record":{"source":{"id":"1401.4108","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2014-01-16T18:04:52Z","cross_cats_sorted":[],"title_canon_sha256":"f61dca10cc3168645e3b2bc4b18b1e2c253d9f0debe899360f331831b459c7d3","abstract_canon_sha256":"85c062a37f1176ffe5e3a9654028af335cc4093962108a61193d65bbea0cd2da"},"schema_version":"1.0"},"canonical_sha256":"996300e5a2ced357f2966bca4ce0063a9d8154b240d4ce3e22a92731a3f343f4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:45:24.754476Z","signature_b64":"Di0a70Hks1Ju5XhaTgueMgGcEONq4ZYF5h88YvjHSg5e+eTn7GFFwNB/QDx4VbLWd8gLdL58ebZBU9hK8b25BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"996300e5a2ced357f2966bca4ce0063a9d8154b240d4ce3e22a92731a3f343f4","last_reissued_at":"2026-05-18T01:45:24.754063Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:45:24.754063Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1401.4108","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":"2026-05-18T01:45:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1IayEKWS28OdUK3qznQsGLqKZqbgQ6WjE3EbTSGmpRVG/qFGUnJWFWRA6MqZWdxHO+X9yfkc7UjYP7MEbHdlBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T03:45:44.020542Z"},"content_sha256":"51cf867d95d94f13cbb495878698ba8d1fab415ab0f3a1dde91a77253ba046d0","schema_version":"1.0","event_id":"sha256:51cf867d95d94f13cbb495878698ba8d1fab415ab0f3a1dde91a77253ba046d0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:TFRQBZNCZ3JVP4UWNPFEZYAGHK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The influence of the matter along the line of sight and in the lens environment on the strong gravitational lensing","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"astro-ph.CO","authors_text":"M. Jaroszynski, Z. Kostrzewa-Rutkowska","submitted_at":"2014-01-16T18:04:52Z","abstract_excerpt":"We investigate the influence of the matter along the line of sight and in the lens environment on the image configurations, relative time delays, and the resulting models of strong gravitational lensing. The distribution of matter in space and properties of gravitationally bound haloes are based on the Millennium Simulation. In our numerical experiments we consider isolated lens in a uniform universe model and the same lens surrounded by close neighbours and/or objects close to the line of sight which gives four different descriptions of the light propagation. We compare the results of the len"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.4108","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":"2026-05-18T01:45:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RnrZy2tONbS4hMBEZDkAgGNmA+XlgEFnwAA6CWiLfWPiOwFIMak05NRPjJkheLh/0m3DthdKmd0bzqgtcCX1AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-13T03:45:44.021357Z"},"content_sha256":"8f0ddad5254e519acc5836bf29e8baecdf863b91c72ca78a1a8dfd7eaca456f4","schema_version":"1.0","event_id":"sha256:8f0ddad5254e519acc5836bf29e8baecdf863b91c72ca78a1a8dfd7eaca456f4"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TFRQBZNCZ3JVP4UWNPFEZYAGHK/bundle.json","state_url":"https://pith.science/pith/TFRQBZNCZ3JVP4UWNPFEZYAGHK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TFRQBZNCZ3JVP4UWNPFEZYAGHK/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":"2026-08-13T03:45:44Z","links":{"resolver":"https://pith.science/pith/TFRQBZNCZ3JVP4UWNPFEZYAGHK","bundle":"https://pith.science/pith/TFRQBZNCZ3JVP4UWNPFEZYAGHK/bundle.json","state":"https://pith.science/pith/TFRQBZNCZ3JVP4UWNPFEZYAGHK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TFRQBZNCZ3JVP4UWNPFEZYAGHK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:TFRQBZNCZ3JVP4UWNPFEZYAGHK","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":"85c062a37f1176ffe5e3a9654028af335cc4093962108a61193d65bbea0cd2da","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2014-01-16T18:04:52Z","title_canon_sha256":"f61dca10cc3168645e3b2bc4b18b1e2c253d9f0debe899360f331831b459c7d3"},"schema_version":"1.0","source":{"id":"1401.4108","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1401.4108","created_at":"2026-05-18T01:45:24Z"},{"alias_kind":"arxiv_version","alias_value":"1401.4108v1","created_at":"2026-05-18T01:45:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.4108","created_at":"2026-05-18T01:45:24Z"},{"alias_kind":"pith_short_12","alias_value":"TFRQBZNCZ3JV","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_16","alias_value":"TFRQBZNCZ3JVP4UW","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_8","alias_value":"TFRQBZNC","created_at":"2026-05-18T12:28:49Z"}],"graph_snapshots":[{"event_id":"sha256:8f0ddad5254e519acc5836bf29e8baecdf863b91c72ca78a1a8dfd7eaca456f4","target":"graph","created_at":"2026-05-18T01:45:24Z","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 investigate the influence of the matter along the line of sight and in the lens environment on the image configurations, relative time delays, and the resulting models of strong gravitational lensing. The distribution of matter in space and properties of gravitationally bound haloes are based on the Millennium Simulation. In our numerical experiments we consider isolated lens in a uniform universe model and the same lens surrounded by close neighbours and/or objects close to the line of sight which gives four different descriptions of the light propagation. We compare the results of the len","authors_text":"M. Jaroszynski, Z. Kostrzewa-Rutkowska","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2014-01-16T18:04:52Z","title":"The influence of the matter along the line of sight and in the lens environment on the strong gravitational lensing"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.4108","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":"sha256:51cf867d95d94f13cbb495878698ba8d1fab415ab0f3a1dde91a77253ba046d0","target":"record","created_at":"2026-05-18T01:45:24Z","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":"85c062a37f1176ffe5e3a9654028af335cc4093962108a61193d65bbea0cd2da","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2014-01-16T18:04:52Z","title_canon_sha256":"f61dca10cc3168645e3b2bc4b18b1e2c253d9f0debe899360f331831b459c7d3"},"schema_version":"1.0","source":{"id":"1401.4108","kind":"arxiv","version":1}},"canonical_sha256":"996300e5a2ced357f2966bca4ce0063a9d8154b240d4ce3e22a92731a3f343f4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"996300e5a2ced357f2966bca4ce0063a9d8154b240d4ce3e22a92731a3f343f4","first_computed_at":"2026-05-18T01:45:24.754063Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:45:24.754063Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Di0a70Hks1Ju5XhaTgueMgGcEONq4ZYF5h88YvjHSg5e+eTn7GFFwNB/QDx4VbLWd8gLdL58ebZBU9hK8b25BQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:45:24.754476Z","signed_message":"canonical_sha256_bytes"},"source_id":"1401.4108","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:51cf867d95d94f13cbb495878698ba8d1fab415ab0f3a1dde91a77253ba046d0","sha256:8f0ddad5254e519acc5836bf29e8baecdf863b91c72ca78a1a8dfd7eaca456f4"],"state_sha256":"6847a32dbe5adcc100a38c6506b7626fef1e003be905696d410577879035c130"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tNbtKxtXhSWN3ETtZSgVgRbGIdc6A+F67DFJ9exv1DS7K0HhVkqJvyWhctGt+ayvc1I22bcL2PiiyZRAEAzFAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-13T03:45:44.033176Z","bundle_sha256":"2df779264dca3f65e42e5d608b475487f25e2e9bb2ea30c89253e7f491b1135b"}}