{"as_of":"2026-08-13T19:51:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:f4d0503b5fdabab62fa71ca0bd0665751f9cf4e671708265da43218e7d68ea95","coverage":[{"denominator":78,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":78,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-11T13:29:04.918735Z","state":"measured"},{"denominator":80,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":80,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-13T06:32:02.005865+00:00","state":"measured"},{"denominator":2,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":2,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-03T18:51:50.902518Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-05-20T03:03:21.489212Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.13162","snapshot_observed_at":"2026-08-03T18:51:50.902518Z","title":"von Hausegger and C","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2512.03867","last_updated":"2025-12-03T15:19:44Z","snapshot_observed_at":"2026-08-06T05:49:41.390408Z","submitted_at":"2025-12-03T15:19:44Z","title":"The Cosmological Dipole in Tilted Anisotropic Universes","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-03T18:51:50.902518Z"},"links":{"cited_paper":"/paper/2412.13162","citing_paper":"/paper/2512.03867"},"observation_digest":"sha256:8b907cc80d65a3215e8c06226a05879accaadc6c74b0bc9ef7c39f509ac63e3b","observation_id":"9a434013-ece3-4df7-8268-5a4b969aa372","resolution":{"observed_at":"2026-08-03T18:51:50.902518Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"cited_work":{"arxiv_id":"2412.13162","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2412.13162","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"von Hausegger and C","venue":null,"work_id":"3ba46e77-cc37-4f28-8d96-78597b69e015","year":2025},"citing_paper":{"arxiv_id":"2605.19476","last_updated":"2026-07-14T05:19:43Z","snapshot_observed_at":"2026-08-01T14:11:35.513868Z","submitted_at":"2026-05-19T07:28:18Z","title":"Prospect of Measuring the Cosmic Dipole by Associating Strongly Lensed Gravitational Waves with Galaxy Surveys","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-05-20T03:03:06.326603Z"},"links":{"cited_paper":"/paper/2412.13162","citing_paper":"/paper/2605.19476"},"observation_digest":"sha256:fbd638603ed910b5bd284f70d7b551ebf52adba081d1affffe9d2b32135f8043","observation_id":"edd215a7-848d-44eb-b0d1-45a62612f2bc","resolution":{"observed_at":"2026-05-20T03:03:21.492365Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2412.13162/citation-record","integrity":"/paper/2412.13162/integrity","json":"/paper/2412.13162/citation-record.json","paper":"/paper/2412.13162"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:06.580922Z","title":"Generally, however, boundary terms are functions of the bin edges𝑧1 and 𝑧2","venue":null,"work_id":"7f74d614-8df6-4405-a1a9-ba1a6b09ccf9","year":null},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.562250Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:7ce89eb724e47558c63f793a61e630abfd50b56bd69fc64ecc12a2deb2ce9146","observation_id":"8aeeb195-162d-4413-93e0-8106846c733d","resolution":{"observed_at":"2026-08-11T13:29:06.584922Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:06.568059Z","title":"Boundary terms 𝐵 (left panel) and effective redshift𝑧𝑏 (rightpanel)perchoiceof(photometric)binedges [𝑧′ 1,𝑧′ 2],computed according to Eq","venue":null,"work_id":"871b9f66-5939-413a-a455-bda0b4043a56","year":null},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.567284Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:2b32af9b39b0a77a5d653a845bb6c2aeca509bf205c197bf1b1488a04ab47385","observation_id":"e157e26a-63b7-4dd0-b122-b416d1d838c1","resolution":{"observed_at":"2026-08-11T13:29:06.572224Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:06.553750Z","title":null,"venue":null,"work_id":"97c9dc45-c4aa-4534-812c-4699a5d43853","year":null},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.571724Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:5ea7b38e5fd31d9e8384f8602d945ff73f320a664e7a61fc9ed362ea89357d47","observation_id":"fd1d0f00-2699-4ea1-b369-8a7a17da3b57","resolution":{"observed_at":"2026-08-11T13:29:06.558844Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:06.534640Z","title":"Lastly, varying𝜎𝑧 for chosen narrow bins does not change the functional form of the boundary terms much, whereas the presence of redshift bias can","venue":null,"work_id":"2a908225-412b-4b70-8723-32565c8810c4","year":null},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.576085Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:f256bdf44ad75f21ad3d5919a0da746cac1c09a0f218ffde3bcc4b764c073d54","observation_id":"dc2a97d2-c787-4f20-ba36-b9af78b59c4a","resolution":{"observed_at":"2026-08-11T13:29:06.542779Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:06.520761Z","title":"−0.5 𝑧′−𝑚𝑧−𝑎 𝜎𝑧 2# + 𝑓𝑜 (2𝜋𝜎2𝑧)0.5 exp","venue":null,"work_id":"116ca4b1-5943-4c17-8a2d-562d59076644","year":null},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.580717Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:d4a3f138427c94f6e602b7eb07f21055be6b32dcfba03e3d566ae74b57293270","observation_id":"b2c4eb14-1af8-40fc-991b-b3103c55bb0d","resolution":{"observed_at":"2026-08-11T13:29:06.525857Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:06.502488Z","title":"Each point is assigned a cosmological redshift ¯𝑧, sampled from Eq","venue":null,"work_id":"4ef23750-357c-433b-a581-416970b5339d","year":null},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.585628Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:ae1b73e4e4a54a26f24fb5f67dec5d24773b97312c33e2c7e019bd645fdc7a1a","observation_id":"261f0f02-949a-41ca-9ede-03617fb539c2","resolution":{"observed_at":"2026-08-11T13:29:06.510087Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:06.489095Z","title":null,"venue":null,"work_id":"c64ff18b-4119-403d-a875-dc24f625a121","year":null},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.590196Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:d2c8ab5656c0aea6d8ffe92848fc6f222171443555e08b237abd36decf2989af","observation_id":"871f8c61-784e-4d1f-843c-539a3126b94b","resolution":{"observed_at":"2026-08-11T13:29:06.493728Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:06.473157Z","title":"Then, a color cut may affect the source countsdifferentlyindifferentdirectionsrelativetothedirection of motion","venue":null,"work_id":"2866799f-9c77-47a9-9ed0-731cae55a58f","year":null},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.594562Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:a326d1ec12197cd1b5fbb47515ac8bc06de53d50c04e5a532a16479dbcdd0061","observation_id":"88b90766-8cde-4ee9-b2bc-ddf05f23d326","resolution":{"observed_at":"2026-08-11T13:29:06.479714Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:06.456158Z","title":null,"venue":null,"work_id":"9a7140f9-7909-4b16-91cb-033ea41191af","year":null},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.599732Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:9b94e3e13b486f077cbbed5310bc7e0f561709ddce6f7032747f849f01b63e5d","observation_id":"73651f88-c0c3-4e8a-8aee-5418d4491470","resolution":{"observed_at":"2026-08-11T13:29:06.461439Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:06.442267Z","title":"Ehlers, P","venue":null,"work_id":"2e40373f-a69f-40a8-b699-e96d1a1b4f2e","year":1968},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.604673Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:2064d6e64de24df53af233212109517c26bf2be4f5cd270b983a3377b5b563cb","observation_id":"b3bab9c5-e313-4e2f-ae7e-948b069d14e3","resolution":{"observed_at":"2026-08-11T13:29:06.446405Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:06.428676Z","title":null,"venue":null,"work_id":"8adf7a41-3154-436b-b19e-c29af1a6d124","year":1995},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.608765Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:c57e90ea6c6f4b8debb7869408e93b2c7a81b0481cce9b96e7bdde966c80a03a","observation_id":"b458d001-0125-44d2-8ebf-402337b1f858","resolution":{"observed_at":"2026-08-11T13:29:06.432759Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2208.05018","last_updated":"2022-08-09T19:47:54Z","snapshot_observed_at":"2026-08-13T14:48:05.518833Z","submitted_at":"2022-08-09T19:47:54Z","title":"Anomalies in Physical Cosmology","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2208.05018","snapshot_observed_at":"2026-08-11T13:29:04.613280Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.613280Z"},"links":{"cited_paper":"/paper/2208.05018","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:47875edfc2c7cd6ea1472a55462142c2557ad27b01d8735d71e5b45ad513160f","observation_id":"2040f6bd-cc55-4d08-9216-78df11121475","resolution":{"observed_at":"2026-08-11T13:29:04.613280Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.05765","last_updated":"2023-02-27T19:00:00Z","snapshot_observed_at":"2026-08-13T15:05:28.513936Z","submitted_at":"2022-07-12T18:00:01Z","title":"Is the Observable Universe Consistent with the Cosmological Principle?","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.05765","snapshot_observed_at":"2026-08-11T13:29:04.618779Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.618779Z"},"links":{"cited_paper":"/paper/2207.05765","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:a276af8893d89a5a489a4f376149e1313647f7da7090dba28374f0a934e71c97","observation_id":"c51e4003-e892-4cfe-9bbd-090f90590d49","resolution":{"observed_at":"2026-08-11T13:29:04.618779Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:06.413845Z","title":null,"venue":null,"work_id":"3dba4872-e93a-4cb5-add0-77896aabf871","year":1967},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.624532Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:d3b1cff62e07040106ba4bace3ca95cdca8237748367db2fd05503a79231f62f","observation_id":"f59c101c-5082-4e3b-83e5-e4833c12ec0b","resolution":{"observed_at":"2026-08-11T13:29:06.419055Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1807.06205","last_updated":"2019-12-03T18:36:28Z","snapshot_observed_at":"2026-08-06T20:42:17.427266Z","submitted_at":"2018-07-17T04:05:03Z","title":"Planck 2018 results. I. Overview and the cosmological legacy of Planck","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1807.06205","snapshot_observed_at":"2026-08-11T13:29:04.628853Z","title":"(Planck),Astron.Astrophys","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.628853Z"},"links":{"cited_paper":"/paper/1807.06205","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:a3fb752b5224b8bc22ea838705e679ef3502fd56747ef849324ab29214ad0415","observation_id":"4448a0dd-1406-4389-83d4-cede64891ea7","resolution":{"observed_at":"2026-08-11T13:29:04.628853Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/0112457","last_updated":"2001-12-19T17:17:05Z","snapshot_observed_at":"2026-07-07T00:24:11.343769Z","submitted_at":"2001-12-19T17:17:05Z","title":"Peculiar velocity effects in high-resolution microwave background experiments","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"astro-ph/0112457","snapshot_observed_at":"2026-08-11T13:29:04.633919Z","title":"Challinor and F","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.633919Z"},"links":{"cited_paper":"/paper/astro-ph/0112457","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:a648f4ade071f11956ae773f2a7fb96545484e54d801202a6ea340b3c23144a6","observation_id":"06db5db8-546a-4d5a-a793-9661d8295a73","resolution":{"observed_at":"2026-08-11T13:29:04.633919Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1303.5087","last_updated":"2015-07-22T05:02:11Z","snapshot_observed_at":"2026-07-06T03:09:14.953676Z","submitted_at":"2013-03-20T20:10:27Z","title":"Planck 2013 results. XXVII. Doppler boosting of the CMB: Eppur si muove","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1303.5087","snapshot_observed_at":"2026-08-11T13:29:04.638720Z","title":"(Planck),Astron.Astrophys","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.638720Z"},"links":{"cited_paper":"/paper/1303.5087","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:795cd8cc8bcb87a5605300f8328bd216f02d1b88d49e92e10f892bae6c434700","observation_id":"093411f2-deb4-45bd-b242-8f966ac5d413","resolution":{"observed_at":"2026-08-11T13:29:04.638720Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2011.08385","last_updated":"2021-07-23T17:54:07Z","snapshot_observed_at":"2026-08-13T05:53:14.840432Z","submitted_at":"2020-11-17T02:49:15Z","title":"First constraints on the intrinsic CMB dipole and our velocity with Doppler and aberration","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2011.08385","snapshot_observed_at":"2026-08-11T13:29:04.643849Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.643849Z"},"links":{"cited_paper":"/paper/2011.08385","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:8650c4777dcde4e97b58f06ca92fd7079fc1c9c27de7c17a1515cf237950ba4e","observation_id":"c4273a70-0460-4d41-bcc6-f3561191a722","resolution":{"observed_at":"2026-08-11T13:29:04.643849Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2106.07666","last_updated":"2021-11-18T07:20:34Z","snapshot_observed_at":"2026-08-13T19:03:57.645857Z","submitted_at":"2021-06-14T18:00:04Z","title":"Bayesian estimation of our local motion from the Planck-2018 CMB temperature map","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2106.07666","snapshot_observed_at":"2026-08-11T13:29:04.648319Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.648319Z"},"links":{"cited_paper":"/paper/2106.07666","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:87dfaca803227a9b86005a1a4b73642924348e77a5837cf2c276fff6fa220b7b","observation_id":"9ca7de4f-62b7-4936-93db-069a94dca681","resolution":{"observed_at":"2026-08-11T13:29:04.648319Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:06.401109Z","title":null,"venue":null,"work_id":"cd182990-3bd7-4365-8f6c-47e161c7520f","year":1988},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.652605Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:8f6e0941662a1ca00fa9efdae12585edf2e71fcaacccec91a00a3be1ba73061e","observation_id":"4e42751b-1faa-41d0-8e35-e71c9e007205","resolution":{"observed_at":"2026-08-11T13:29:06.405284Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:06.386939Z","title":null,"venue":null,"work_id":"84ae322f-547b-4dde-95c8-b19124dcf2ea","year":1991},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.656796Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:cd2cce43aa04546f5cf9858d117e870560c4d31c1c61280fe6b0a85a59d195b4","observation_id":"99627447-1031-4976-86eb-fe32e358a916","resolution":{"observed_at":"2026-08-11T13:29:06.391816Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/9507094","last_updated":"1995-07-24T11:14:49Z","snapshot_observed_at":"2026-08-13T08:40:08.636998Z","submitted_at":"1995-07-24T11:14:49Z","title":"Dipole Anisotropy from an Entropy Gradient","version":1},"cited_work":{"arxiv_id":"astro-ph/9507094","doi":null,"metadata_source":"pith","pith_arxiv_id":"astro-ph/9507094","snapshot_observed_at":"2026-08-11T13:29:06.212632Z","title":"Dipole Anisotropy from an Entropy Gradient","venue":"astro-ph","work_id":"e972501b-158a-4be2-8cc9-fdea8f08854e","year":1995},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.661652Z"},"links":{"cited_paper":"/paper/astro-ph/9507094","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:ed57123e11fac874df9df73e3e9625190a6d15a461ccbbf1e7b659aba9b526f8","observation_id":"7b3f8fd3-bd7c-4687-844e-2c57814bab18","resolution":{"observed_at":"2026-08-11T13:29:06.217383Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0808.1570","last_updated":"2008-08-11T20:00:13Z","snapshot_observed_at":"2026-07-06T01:43:39.780382Z","submitted_at":"2008-08-11T20:00:13Z","title":"Superhorizon Perturbations and the Cosmic Microwave Background","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0808.1570","snapshot_observed_at":"2026-08-11T13:29:04.665702Z","title":null,"venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.665702Z"},"links":{"cited_paper":"/paper/0808.1570","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:a6182a743d32ef7acad4efa2beed6ab0b69b0719a2d3c8aa8eab402ae5675bf8","observation_id":"b6c63048-e8d7-4aef-b92c-6ec778c3289a","resolution":{"observed_at":"2026-08-11T13:29:04.665702Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.01569","last_updated":"2022-07-04T16:41:23Z","snapshot_observed_at":"2026-08-13T15:10:49.480581Z","submitted_at":"2022-07-04T16:41:23Z","title":"Galaxy number-count dipole and superhorizon fluctuations","version":1},"cited_work":{"arxiv_id":"2207.01569","doi":null,"metadata_source":"pith","pith_arxiv_id":"2207.01569","snapshot_observed_at":"2026-08-11T13:29:06.179541Z","title":"Galaxy number-count dipole and superhorizon fluctuations","venue":"astro-ph.CO","work_id":"5910e17b-1c5f-4a22-bc91-e2ed9ff3132d","year":2022},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.670697Z"},"links":{"cited_paper":"/paper/2207.01569","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:933717e01bcc6cb872cdb4f3f11c754ea924fa6612d4dfe3f992a62f7cb491c2","observation_id":"4698ca45-3e04-43c7-ade9-5245801d8668","resolution":{"observed_at":"2026-08-11T13:29:06.184616Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:04.676270Z","title":null,"venue":null,"work_id":null,"year":1984},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.676270Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:63cf21c39d5b14acb50f789fb8dc6f44e3504671516349a1fd45b468b867caf0","observation_id":"0365b152-d493-435b-9b9d-3a234514453f","resolution":{"observed_at":"2026-08-11T13:29:04.676270Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.18438","last_updated":"2024-02-28T16:06:02Z","snapshot_observed_at":"2026-08-13T04:08:07.257731Z","submitted_at":"2024-02-28T16:06:02Z","title":"Fast and spurious: a robust determination of our peculiar velocity with future galaxy surveys","version":1},"cited_work":{"arxiv_id":"2402.18438","doi":null,"metadata_source":"pith","pith_arxiv_id":"2402.18438","snapshot_observed_at":"2026-08-11T13:29:06.162896Z","title":"Fast and spurious: a robust determination of our peculiar velocity with future galaxy surveys","venue":"astro-ph.CO","work_id":"4b9e09dd-a423-4e0f-ac85-980a03ab116e","year":2024},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.680688Z"},"links":{"cited_paper":"/paper/2402.18438","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:fa68bdce8a0f6477920228661d612ab4937ca7be5aa7d7376c317768bb75869d","observation_id":"460d7cd6-08c7-453f-b67b-ed36259edeeb","resolution":{"observed_at":"2026-08-11T13:29:06.167431Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0810.4520","last_updated":"2008-10-24T18:43:52Z","snapshot_observed_at":"2026-07-06T01:45:38.172333Z","submitted_at":"2008-10-24T18:43:52Z","title":"Detecting the Cosmic Dipole Anisotropy in Large-Scale Radio Surveys","version":1},"cited_work":{"arxiv_id":"0810.4520","doi":null,"metadata_source":"pith","pith_arxiv_id":"0810.4520","snapshot_observed_at":"2026-08-11T13:29:06.145939Z","title":"Detecting the Cosmic Dipole Anisotropy in Large-Scale Radio Surveys","venue":"astro-ph","work_id":"f5f73b0f-30bb-48f3-a947-d30a72963bf1","year":2008},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.685183Z"},"links":{"cited_paper":"/paper/0810.4520","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:0f4a11c111cfbdb19eae281d85e3ae6e7a74db8df12753ce9b943b35dcb08fae","observation_id":"757701c1-ac84-452f-bc3a-4610ae3fcecf","resolution":{"observed_at":"2026-08-11T13:29:06.150624Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:06.367025Z","title":null,"venue":null,"work_id":"d46a6492-d773-4be3-ba00-16a639c270cb","year":2025},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.690591Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:383dd11ce8f94e246805340aa35a6bed01eb680c09147ddc365d7b5f38787e8e","observation_id":"e03020e1-ee63-428b-b24b-ad955384be27","resolution":{"observed_at":"2026-08-11T13:29:06.370845Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:04.695053Z","title":"Blake and J","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.695053Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:46b2415cf9a6a6f276fbadb83a64bd37bdc397abc4d0e1971011cea5cd2f5b95","observation_id":"2b75eacc-f7a3-411b-a6d2-13851f21599d","resolution":{"observed_at":"2026-08-11T13:29:04.695053Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1110.6260","last_updated":"2011-10-28T06:54:57Z","snapshot_observed_at":"2026-08-10T05:05:37.137704Z","submitted_at":"2011-10-28T06:54:57Z","title":"Large peculiar motion of the solar system from the dipole anisotropy in sky brightness due to distant radio sources","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1110.6260","snapshot_observed_at":"2026-08-11T13:29:04.700037Z","title":null,"venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.700037Z"},"links":{"cited_paper":"/paper/1110.6260","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:c6c2506b485c069c35522b47454bc9e4da225b16d277cb304b70053451d32f2d","observation_id":"b4d106be-ba37-4123-a1aa-08e22e966ecb","resolution":{"observed_at":"2026-08-11T13:29:04.700037Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1301.5559","last_updated":"2013-07-24T11:20:07Z","snapshot_observed_at":"2026-08-01T15:22:35.824211Z","submitted_at":"2013-01-23T16:42:34Z","title":"Cosmic radio dipole from NVSS and WENSS","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1301.5559","snapshot_observed_at":"2026-08-11T13:29:04.704204Z","title":"Rubart and D","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.704204Z"},"links":{"cited_paper":"/paper/1301.5559","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:69748f455af32141cb379c125d274513d2bca17accf0a45d53df4a34a3118469","observation_id":"7cf216ff-e9f4-4145-8145-a7ffaa001cc1","resolution":{"observed_at":"2026-08-11T13:29:04.704204Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2009.14826","last_updated":"2021-01-18T19:00:00Z","snapshot_observed_at":"2026-08-08T20:38:14.787582Z","submitted_at":"2020-09-30T17:56:05Z","title":"A Test of the Cosmological Principle with Quasars","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2009.14826","snapshot_observed_at":"2026-08-11T13:29:04.709545Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.709545Z"},"links":{"cited_paper":"/paper/2009.14826","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:7c80e0dd3fa88db263379a4ee8a91139015f8f3830c3f2c53007f96a6d9c5ab8","observation_id":"7340da65-2a6d-4799-babb-e0814913d779","resolution":{"observed_at":"2026-08-11T13:29:04.709545Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2206.05624","last_updated":"2022-08-12T17:58:55Z","snapshot_observed_at":"2026-08-13T15:25:29.609143Z","submitted_at":"2022-06-11T22:06:05Z","title":"A Challenge to the Standard Cosmological Model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2206.05624","snapshot_observed_at":"2026-08-11T13:29:04.714418Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.714418Z"},"links":{"cited_paper":"/paper/2206.05624","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:ae5cd9f36120368a2f4356d8f3b0613582c2be8703d117552ca7cc5f7fc7eb00","observation_id":"0a134118-2074-4c8b-9c8e-dd5a5961554b","resolution":{"observed_at":"2026-08-11T13:29:04.714418Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.07733","last_updated":"2023-08-07T16:53:38Z","snapshot_observed_at":"2026-08-13T13:20:55.342681Z","submitted_at":"2022-12-15T11:29:23Z","title":"Testing the Cosmological Principle with CatWISE Quasars: A Bayesian Analysis of the Number-Count Dipole","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.07733","snapshot_observed_at":"2026-08-11T13:29:04.719221Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.719221Z"},"links":{"cited_paper":"/paper/2212.07733","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:8369387b9ac0ea4c90a9eca2596e2a22a0b5a47e326e9e9d3fa29c30403175e5","observation_id":"e68b8b5d-04d5-4b8a-a305-0a66749cd96c","resolution":{"observed_at":"2026-08-11T13:29:04.719221Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2305.15335","last_updated":"2023-05-24T16:49:42Z","snapshot_observed_at":"2026-08-13T11:34:14.546327Z","submitted_at":"2023-05-24T16:49:42Z","title":"The cosmic radio dipole: Bayesian estimators on new and old radio surveys","version":1},"cited_work":{"arxiv_id":"2305.15335","doi":null,"metadata_source":"pith","pith_arxiv_id":"2305.15335","snapshot_observed_at":"2026-08-11T13:29:05.989719Z","title":"The cosmic radio dipole: Bayesian estimators on new and old radio surveys","venue":"astro-ph.CO","work_id":"1995762d-acc7-4c6b-a093-8d8f7173c8e3","year":2023},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.723996Z"},"links":{"cited_paper":"/paper/2305.15335","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:016edfb4ebd99237a111f364bb23be9dfce0ea8e4ad0feae07984dcbee0a3ff5","observation_id":"e19714c5-7af9-4cf4-aa0d-a488a0c95df8","resolution":{"observed_at":"2026-08-11T13:29:05.994533Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2406.01871","last_updated":"2024-06-04T00:48:58Z","snapshot_observed_at":"2026-08-13T16:11:58.353157Z","submitted_at":"2024-06-04T00:48:58Z","title":"A Bayesian approach to the cosmic dipole in radio galaxy surveys: Joint analysis of NVSS & RACS","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2406.01871","snapshot_observed_at":"2026-08-11T13:29:04.728792Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.728792Z"},"links":{"cited_paper":"/paper/2406.01871","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:4f85d8550c94fd4ee6c846f063aad5fd150bfeac1b0722b7132056f0ee69e183","observation_id":"d8a71beb-4f7a-4256-9e56-d1bd65aaf7d5","resolution":{"observed_at":"2026-08-11T13:29:04.728792Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1709.04165","last_updated":"2017-12-11T11:13:36Z","snapshot_observed_at":"2026-07-06T05:59:24.024807Z","submitted_at":"2017-09-13T07:24:09Z","title":"The kinematic dipole in galaxy redshift surveys","version":2},"cited_work":{"arxiv_id":"1709.04165","doi":null,"metadata_source":"pith","pith_arxiv_id":"1709.04165","snapshot_observed_at":"2026-08-11T13:29:05.958581Z","title":"The kinematic dipole in galaxy redshift surveys","venue":"astro-ph.CO","work_id":"baab3be0-ad48-4508-8f68-cf4a8a8622ec","year":2017},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.733465Z"},"links":{"cited_paper":"/paper/1709.04165","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:9540a4b78665f4868590d884001aefd245be89738be602f3bd9e06cf1bd0f4b9","observation_id":"fbec1c67-3158-4ed1-8b80-a8382e3017d0","resolution":{"observed_at":"2026-08-11T13:29:05.963101Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2106.05284","last_updated":"2021-11-06T10:29:35Z","snapshot_observed_at":"2026-08-13T19:06:54.646361Z","submitted_at":"2021-06-09T18:00:02Z","title":"A new way to test the Cosmological Principle: measuring our peculiar velocity and the large scale anisotropy independently","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2106.05284","snapshot_observed_at":"2026-08-11T13:29:04.740630Z","title":"Nadolny, R","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.740630Z"},"links":{"cited_paper":"/paper/2106.05284","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:41f88779e34adec957048f965aca596436dffc32634401e2445b5442bb52b315","observation_id":"0847a537-e6e7-4797-b8f8-895c5bb2faaf","resolution":{"observed_at":"2026-08-11T13:29:04.740630Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2111.03616","last_updated":"2022-12-14T17:06:05Z","snapshot_observed_at":"2026-07-06T12:05:55.928795Z","submitted_at":"2021-11-05T17:05:44Z","title":"On the kinematic cosmic dipole tension","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2111.03616","snapshot_observed_at":"2026-08-11T13:29:04.745149Z","title":"Dalang and C","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.745149Z"},"links":{"cited_paper":"/paper/2111.03616","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:3bed2005d930580295c66a283b36523d658bac26f802c0b6f7442e3d76a45ff5","observation_id":"5e6491c7-3678-4db0-83a5-25ca0a73f9c1","resolution":{"observed_at":"2026-08-11T13:29:04.745149Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.04925","last_updated":"2023-08-12T16:48:47Z","snapshot_observed_at":"2026-08-13T13:24:37.857960Z","submitted_at":"2022-12-09T15:34:34Z","title":"Theoretical systematics in testing the Cosmological Principle with the kinematic quasar dipole","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.04925","snapshot_observed_at":"2026-08-11T13:29:04.750356Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.750356Z"},"links":{"cited_paper":"/paper/2212.04925","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:45f0bdd1aee5ca4b3280c3f4b720653a58123ccf9e281386ff427cb20b779be1","observation_id":"fb3ef07b-55b8-4f1b-a468-42a0a4f9c0f0","resolution":{"observed_at":"2026-08-11T13:29:04.750356Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2404.07929","last_updated":"2024-10-14T12:20:56Z","snapshot_observed_at":"2026-08-13T00:32:27.942967Z","submitted_at":"2024-04-11T17:26:37Z","title":"The expected kinematic matter dipole is robust against source evolution","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2404.07929","snapshot_observed_at":"2026-08-11T13:29:04.755723Z","title":"von Hausegger, Monthly Notices of the Royal Astronomi- cal Society: Letters535, L49 (2024), arXiv:2404.07929 [astro- ph.CO]","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.755723Z"},"links":{"cited_paper":"/paper/2404.07929","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:4d91e4ad9792fb99b9c4fd7eff3708ef8629fb80acd15075826840ddf3138016","observation_id":"d4113a27-e5af-43e5-b037-33d9c8a0e9b6","resolution":{"observed_at":"2026-08-11T13:29:04.755723Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2007.01802","last_updated":"2020-10-13T15:19:59Z","snapshot_observed_at":"2026-08-05T02:41:39.151167Z","submitted_at":"2020-07-03T16:42:47Z","title":"Impact of Relativistic Effects on the Primordial Non-Gaussianity Signature in the Large-Scale Clustering of Quasars","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2007.01802","snapshot_observed_at":"2026-08-11T13:29:04.760176Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.760176Z"},"links":{"cited_paper":"/paper/2007.01802","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:094766f62aa2f0d0c54db70394bf97927b151e7f7c74a3ec8f5ed257e392857d","observation_id":"fc9b486f-9f69-400f-806c-056cc325b67f","resolution":{"observed_at":"2026-08-11T13:29:04.760176Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":"ph/9811189","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:05.878084Z","title":"Benítez, Astrophys","venue":null,"work_id":"6b1d3594-75da-421e-ad80-c9882d994c8c","year":2000},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.764657Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:9e74c116d04f5d33cf43525b8cd9aceb230bcc51dff22d007889828cdb75e53d","observation_id":"c307990d-2e8f-4093-a0a2-d72c775171ed","resolution":{"observed_at":"2026-08-11T13:29:05.885207Z","resolver_source":"raw_fallback","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:04.768484Z","title":"Le Fèvre, Y","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.768484Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:0b6854ae1280c75ac4513fd6ff89cd283329ab1464ea55f140ca1f852f04840b","observation_id":"308890b3-6fa2-41eb-a753-5db77bf889ee","resolution":{"observed_at":"2026-08-11T13:29:04.768484Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1908.00771","last_updated":"2019-08-02T09:28:03Z","snapshot_observed_at":"2026-08-13T05:45:06.641061Z","submitted_at":"2019-08-02T09:28:03Z","title":"MAGPHYS+photo-z: Constraining the Physical Properties of Galaxies with Unknown Redshifts","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1908.00771","snapshot_observed_at":"2026-08-11T13:29:04.772213Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.772213Z"},"links":{"cited_paper":"/paper/1908.00771","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:92656a4f2c4e69bd75439d9bfa72a4d4ab0900571bcda3a11902bdb0c5334865","observation_id":"6335e623-a5a4-4c83-8ed0-ced67eeaa440","resolution":{"observed_at":"2026-08-11T13:29:04.772213Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:04.776847Z","title":"Mellieret al","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.776847Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:18c1e156807d7a99a597b96face2b7757e0515f4f78f2a45c576c11190a833e0","observation_id":"49234a38-245c-4d44-940d-3de9ced44ec6","resolution":{"observed_at":"2026-08-11T13:29:04.776847Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1412.4872","last_updated":"2015-03-25T23:27:43Z","snapshot_observed_at":"2026-07-06T04:03:43.160099Z","submitted_at":"2014-12-16T03:59:10Z","title":"Cosmology with the SPHEREX All-Sky Spectral Survey","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1412.4872","snapshot_observed_at":"2026-08-11T13:29:04.780906Z","title":null,"venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.780906Z"},"links":{"cited_paper":"/paper/1412.4872","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:a6a3fe1b0fc6d6c0a6ac8b60dc6317159a638630f410a0bdec0cd0db446c682a","observation_id":"09067f89-b982-47d7-be7e-4af0bfcbfdb3","resolution":{"observed_at":"2026-08-11T13:29:04.780906Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.10688","last_updated":"2019-07-24T19:44:53Z","snapshot_observed_at":"2026-08-02T07:26:08.526896Z","submitted_at":"2019-07-24T19:44:53Z","title":"The Dark Energy Spectroscopic Instrument (DESI)","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.10688","snapshot_observed_at":"2026-08-11T13:29:04.785521Z","title":"Bolton, F","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.785521Z"},"links":{"cited_paper":"/paper/1907.10688","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:b7811f656df39f089f250ab61a7b8077c34194a6051b83d470139f2589defb79","observation_id":"e9e76bcf-9286-4180-9461-77e11bf892d3","resolution":{"observed_at":"2026-08-11T13:29:04.785521Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0805.2366","last_updated":"2018-05-23T19:18:23Z","snapshot_observed_at":"2026-08-12T13:36:12.529300Z","submitted_at":"2008-05-15T18:10:13Z","title":"LSST: from Science Drivers to Reference Design and Anticipated Data Products","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0805.2366","snapshot_observed_at":"2026-08-11T13:29:04.791385Z","title":"Ivezićet al","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.791385Z"},"links":{"cited_paper":"/paper/0805.2366","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:8a44c8eb70f2adbec35e263454284f12cb6f5eef0cde6a02adfa53f16dabfb28","observation_id":"d2baabb9-743c-4c90-a6db-a5105c9fa060","resolution":{"observed_at":"2026-08-11T13:29:04.791385Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.13632","last_updated":"2025-03-17T18:28:21Z","snapshot_observed_at":"2026-08-07T16:56:52.667475Z","submitted_at":"2025-03-17T18:28:21Z","title":"Dark Energy Survey Year 3 Results: Cosmological Constraints from Cluster Abundances, Weak Lensing, and Galaxy Clustering","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.13632","snapshot_observed_at":"2026-08-11T13:29:04.796287Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.796287Z"},"links":{"cited_paper":"/paper/2503.13632","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:047e2c72ae51c14cd624222b6160f92d019aba8981f3544239fc374bc22be1ba","observation_id":"6240d43e-a6b4-415a-85ba-4cef544b6864","resolution":{"observed_at":"2026-08-11T13:29:04.796287Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1811.02743","last_updated":"2018-11-07T03:12:27Z","snapshot_observed_at":"2026-08-08T16:21:28.572473Z","submitted_at":"2018-11-07T03:12:27Z","title":"Cosmology with Phase 1 of the Square Kilometre Array; Red Book 2018: Technical specifications and performance forecasts","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1811.02743","snapshot_observed_at":"2026-08-11T13:29:04.801228Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.801228Z"},"links":{"cited_paper":"/paper/1811.02743","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:18f46ac7dfce146bf4cd8a07d9f2d8c64795368adea54fc14be08051108b3c30","observation_id":"63a2ab8e-464e-4fa0-af30-26095c1c33c7","resolution":{"observed_at":"2026-08-11T13:29:04.801228Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1110.3193","last_updated":"2011-10-14T12:57:07Z","snapshot_observed_at":"2026-07-06T02:35:48.625634Z","submitted_at":"2011-10-14T12:57:07Z","title":"Euclid Definition Study Report","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1110.3193","snapshot_observed_at":"2026-08-11T13:29:04.805619Z","title":"Laureijs et al","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.805619Z"},"links":{"cited_paper":"/paper/1110.3193","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:3c6e799c90f47fd6430e1abae2344b3044d7f415f226be1c4b243de89f6e456e","observation_id":"1992a5c2-a2c2-4a73-8df5-5b78d52843f4","resolution":{"observed_at":"2026-08-11T13:29:04.805619Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.09273","last_updated":"2020-11-25T11:35:34Z","snapshot_observed_at":"2026-08-08T09:05:53.979629Z","submitted_at":"2019-10-21T11:49:59Z","title":"Euclid preparation: VII. Forecast validation for Euclid cosmological probes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.09273","snapshot_observed_at":"2026-08-11T13:29:04.810734Z","title":"Blanchard et al","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.810734Z"},"links":{"cited_paper":"/paper/1910.09273","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:635d6d86196347dedced99cd1ca6ecbce738c3feae888462fa27490dba60a39f","observation_id":"e46fd403-7d38-4443-a2a0-5b6022b78eec","resolution":{"observed_at":"2026-08-11T13:29:04.810734Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1809.01669","last_updated":"2021-09-06T19:01:58Z","snapshot_observed_at":"2026-08-09T21:26:10.827740Z","submitted_at":"2018-09-05T18:00:07Z","title":"The LSST Dark Energy Science Collaboration (DESC) Science Requirements Document","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1809.01669","snapshot_observed_at":"2026-08-11T13:29:04.815090Z","title":"Mandelbaum et al","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.815090Z"},"links":{"cited_paper":"/paper/1809.01669","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:b090410c687dd2cdf79cb0f02d8d31d571c219bbbdc02499abbcdf82f8ac552a","observation_id":"88771fd1-1f1f-4284-a34d-dd346d5669e8","resolution":{"observed_at":"2026-08-11T13:29:04.815090Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0805.3413","last_updated":"2008-05-22T09:14:35Z","snapshot_observed_at":"2026-07-06T01:38:39.726709Z","submitted_at":"2008-05-22T09:14:35Z","title":"A semi-empirical simulation of the extragalactic radio continuum sky for next generation radio telescopes","version":1},"cited_work":{"arxiv_id":"0805.3413","doi":null,"metadata_source":"pith","pith_arxiv_id":"0805.3413","snapshot_observed_at":"2026-08-11T13:29:05.410203Z","title":"A semi-empirical simulation of the extragalactic radio continuum sky for next generation radio telescopes","venue":"astro-ph","work_id":"79b544da-59f6-4669-8947-3cc9532a586e","year":2008},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.819518Z"},"links":{"cited_paper":"/paper/0805.3413","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:3a516bd6ffb09c57546a8de0f1b3c515474183f05a068dd6c1b2172402075704","observation_id":"cb6a7299-b0b3-4700-ba62-9b58809cf176","resolution":{"observed_at":"2026-08-11T13:29:05.415004Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1505.07596","last_updated":"2015-12-07T17:50:00Z","snapshot_observed_at":"2026-08-10T09:47:58.087486Z","submitted_at":"2015-05-28T08:45:02Z","title":"Ultra large-scale cosmology in next-generation experiments with single tracers","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1505.07596","snapshot_observed_at":"2026-08-11T13:29:04.823852Z","title":"814,145(2015),arXiv:1505.07596[astro-ph.CO]","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.823852Z"},"links":{"cited_paper":"/paper/1505.07596","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:b9b06663fc4bc5e8f2cd419a5baeb9d62e233589cd2c1d72aced135e99151af4","observation_id":"71101a30-e2d3-41c5-8bcf-af2b745155cb","resolution":{"observed_at":"2026-08-11T13:29:04.823852Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1601.03947","last_updated":"2016-10-25T16:49:46Z","snapshot_observed_at":"2026-08-07T21:43:37.615849Z","submitted_at":"2016-01-15T15:05:27Z","title":"SKA Weak Lensing I: Cosmological Forecasts and the Power of Radio-Optical Cross-Correlations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1601.03947","snapshot_observed_at":"2026-08-11T13:29:04.828811Z","title":"Harrison, S","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.828811Z"},"links":{"cited_paper":"/paper/1601.03947","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:e921f78ae5db207fbe9a5a19ba7aec5608bbf78660cbc1faa8b1aad76683088e","observation_id":"d12cdeda-6419-41f9-8aed-a2cda1f8a837","resolution":{"observed_at":"2026-08-11T13:29:04.828811Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1601.03948","last_updated":"2016-10-25T16:49:48Z","snapshot_observed_at":"2026-08-09T14:05:47.349777Z","submitted_at":"2016-01-15T15:05:30Z","title":"SKA Weak Lensing II: Simulated Performance and Survey Design Considerations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1601.03948","snapshot_observed_at":"2026-08-11T13:29:04.833239Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.833239Z"},"links":{"cited_paper":"/paper/1601.03948","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:e3cff8445ac6586de335afeef3e69f58db3a58803bb9d52d2dd13eb42d3ab30b","observation_id":"c60a56ea-7b01-41cb-bfcd-c82272094f4a","resolution":{"observed_at":"2026-08-11T13:29:04.833239Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.16619","last_updated":"2024-08-29T15:25:34Z","snapshot_observed_at":"2026-08-12T22:55:06.270430Z","submitted_at":"2024-08-29T15:25:34Z","title":"The MeerKAT Absorption Line Survey Data Release 2: Wideband continuum catalogues and a measurement of the cosmic radio dipole","version":1},"cited_work":{"arxiv_id":"2408.16619","doi":null,"metadata_source":"pith","pith_arxiv_id":"2408.16619","snapshot_observed_at":"2026-08-11T13:29:05.345207Z","title":"The MeerKAT Absorption Line Survey Data Release 2: Wideband continuum catalogues and a measurement of the cosmic radio dipole","venue":"astro-ph.CO","work_id":"f69bdd41-2fd3-4d66-88c8-d10e643d68e3","year":2024},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.837039Z"},"links":{"cited_paper":"/paper/2408.16619","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:bfc95e06eda92ee4cbc75253eba95161d9fef4e7242e3b3086655d42539583c9","observation_id":"0e04de16-985c-41c6-a0e2-cdf384548bb7","resolution":{"observed_at":"2026-08-11T13:29:05.349791Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1810.04960","last_updated":"2019-03-21T13:00:54Z","snapshot_observed_at":"2026-07-06T07:07:26.973155Z","submitted_at":"2018-10-11T11:37:20Z","title":"Testing the standard model of cosmology with the SKA: the cosmic radio dipole","version":2},"cited_work":{"arxiv_id":"1810.04960","doi":null,"metadata_source":"pith","pith_arxiv_id":"1810.04960","snapshot_observed_at":"2026-08-11T13:29:05.326655Z","title":"Testing the standard model of cosmology with the SKA: the cosmic radio dipole","venue":"astro-ph.CO","work_id":"87e090e5-ff49-4f16-9dac-2bae5b755cfb","year":2018},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.841016Z"},"links":{"cited_paper":"/paper/1810.04960","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:106c9108f0b66846e2666688d03d84e4100b95861318c7ef87df3feea60ddf4f","observation_id":"7d2ee71a-bebb-4bb1-b73d-729e14e56c57","resolution":{"observed_at":"2026-08-11T13:29:05.331489Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2409.17377","last_updated":"2024-09-25T21:45:03Z","snapshot_observed_at":"2026-08-12T22:37:23.712108Z","submitted_at":"2024-09-25T21:45:03Z","title":"6x2pt: Forecasting gains from joint weak lensing and galaxy clustering analyses with spectroscopic-photometric galaxy cross-correlations","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2409.17377","snapshot_observed_at":"2026-08-11T13:29:04.845386Z","title":"Loureiro, C","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.845386Z"},"links":{"cited_paper":"/paper/2409.17377","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:2e6b88acf7ac50bd25ba8c09d09aa3bbf0e9262fd03c8f83e4987e6d3987fb42","observation_id":"3e99f80e-b650-4cde-99d6-4a60c3663e02","resolution":{"observed_at":"2026-08-11T13:29:04.845386Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:04.849713Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.849713Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:0d9efca1ceb70481e4234969097d4496854add8cdce79059463ac7c1bba61b78","observation_id":"99aad072-4640-470e-8ca7-0f78ca68541a","resolution":{"observed_at":"2026-08-11T13:29:04.849713Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2403.14580","last_updated":"2024-09-26T12:20:54Z","snapshot_observed_at":"2026-08-13T00:48:28.762027Z","submitted_at":"2024-03-21T17:33:35Z","title":"Tomographic redshift dipole: Testing the cosmological principle","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2403.14580","snapshot_observed_at":"2026-08-11T13:29:04.853645Z","title":"da Silveira Ferreira and V","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.853645Z"},"links":{"cited_paper":"/paper/2403.14580","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:af8f48972fccaa56ada15e28d27748f8e1d235c0b5a9c9a88b911c549653f3ec","observation_id":"f7b058e0-a693-4e4f-abdb-db9eb2883fc6","resolution":{"observed_at":"2026-08-11T13:29:04.853645Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2409.09946","last_updated":"2024-11-13T09:51:28Z","snapshot_observed_at":"2026-08-13T12:33:37.717546Z","submitted_at":"2024-09-16T02:38:29Z","title":"An Independent Measure of the Kinematic Dipole from SDSS","version":2},"cited_work":{"arxiv_id":"2409.09946","doi":null,"metadata_source":"pith","pith_arxiv_id":"2409.09946","snapshot_observed_at":"2026-08-11T13:29:05.125341Z","title":"An Independent Measure of the Kinematic Dipole from SDSS","venue":"astro-ph.CO","work_id":"467859fd-ae70-4d7b-87e7-463601ffa38c","year":2024},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.858213Z"},"links":{"cited_paper":"/paper/2409.09946","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:9865ab6d4112ee7d8eaa0171673717b4b9d7c9b9c001b37d5e5a12517c8c5e75","observation_id":"d41de628-aed1-4e57-9955-d0ba9cd7588d","resolution":{"observed_at":"2026-08-11T13:29:05.129729Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1911.12056","last_updated":"2021-03-23T17:47:52Z","snapshot_observed_at":"2026-07-06T08:40:20.153173Z","submitted_at":"2019-11-27T10:06:44Z","title":"Density Weighted Angular Redshift Fluctuations: a New Cosmological Observable","version":2},"cited_work":{"arxiv_id":"1911.12056","doi":null,"metadata_source":"pith","pith_arxiv_id":"1911.12056","snapshot_observed_at":"2026-08-11T13:29:05.107473Z","title":"Density Weighted Angular Redshift Fluctuations: a New Cosmological Observable","venue":"astro-ph.CO","work_id":"a37195f1-cdf6-4baa-84bb-b69dbeda1166","year":2019},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.862823Z"},"links":{"cited_paper":"/paper/1911.12056","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:20fe913838dfc86050b65cbd9ffc5098c81922290046505da56656749d07c78a","observation_id":"4b8079d0-c23a-4b2d-b577-092fdb2d3e7f","resolution":{"observed_at":"2026-08-11T13:29:05.112771Z","resolver_source":"local_arxiv","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2007.14412","last_updated":"2021-02-22T19:00:01Z","snapshot_observed_at":"2026-08-13T16:09:16.613356Z","submitted_at":"2020-07-28T18:00:17Z","title":"High resolution tomography for galaxy spectroscopic surveys with angular redshift fluctuations","version":2},"cited_work":{"arxiv_id":"2007.14412","doi":null,"metadata_source":"pith","pith_arxiv_id":"2007.14412","snapshot_observed_at":"2026-08-11T13:29:05.079786Z","title":"High resolution tomography for galaxy spectroscopic surveys with angular redshift fluctuations","venue":"astro-ph.CO","work_id":"9ba46967-003c-48c4-b971-1b8ccc87b80e","year":2020},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.867142Z"},"links":{"cited_paper":"/paper/2007.14412","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:aaa8e62ffadbf348bef474fae4f39b6386710426f1fcd0cc972e7acd51995c1a","observation_id":"ee5533fa-1c38-4d7c-91d7-6be661be8bea","resolution":{"observed_at":"2026-08-11T13:29:05.084297Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2203.07414","last_updated":"2022-10-17T07:01:55Z","snapshot_observed_at":"2026-08-13T16:23:19.458918Z","submitted_at":"2022-03-14T18:18:39Z","title":"Redshift weighted galaxy number counts","version":3},"cited_work":{"arxiv_id":"2203.07414","doi":null,"metadata_source":"pith","pith_arxiv_id":"2203.07414","snapshot_observed_at":"2026-08-11T13:29:05.057796Z","title":"Redshift weighted galaxy number counts","venue":"astro-ph.CO","work_id":"943cecd4-9c54-4c30-a24b-5b7a1230b536","year":2022},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.871079Z"},"links":{"cited_paper":"/paper/2203.07414","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:611a730a2bf81178208a755cba473e3124e68eb9016e9c16e4a6f95c58ec92ec","observation_id":"b459d9c5-4f84-4b98-a908-4170a892eb5f","resolution":{"observed_at":"2026-08-11T13:29:05.064831Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2302.02028","last_updated":"2023-02-03T23:23:07Z","snapshot_observed_at":"2026-08-13T12:51:06.804679Z","submitted_at":"2023-02-03T23:23:07Z","title":"Analyzing the Large-Scale Bulk Flow using CosmicFlows4: Increasing Tension with the Standard Cosmological Model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2302.02028","snapshot_observed_at":"2026-08-11T13:29:04.874810Z","title":"Watkins, T","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.874810Z"},"links":{"cited_paper":"/paper/2302.02028","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:52b2578027a9a5de7d2a8ff3680f2a6d2328fdf1028cbba2fada2684c860f5f2","observation_id":"6e76feca-b7cb-4df0-8d20-fcac7f6d95df","resolution":{"observed_at":"2026-08-11T13:29:04.874810Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2306.11269","last_updated":"2023-09-10T09:37:27Z","snapshot_observed_at":"2026-08-13T11:13:44.735534Z","submitted_at":"2023-06-20T03:48:39Z","title":"Evaluating bulk flow estimators for CosmicFlows-4 measurements","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.11269","snapshot_observed_at":"2026-08-11T13:29:04.879486Z","title":"Soc.526, 3051 (2023), arXiv:2306.11269 [astro-ph.CO]","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.879486Z"},"links":{"cited_paper":"/paper/2306.11269","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:be80cec14c7cb11bfbe29629f1cb553e8d55df36417da851cc74b046fd858161","observation_id":"5c25b679-e947-41f8-8a1e-ce5639588fb9","resolution":{"observed_at":"2026-08-11T13:29:04.879486Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.16853","last_updated":"2024-05-27T05:57:23Z","snapshot_observed_at":"2026-08-12T23:57:28.247392Z","submitted_at":"2024-05-27T05:57:23Z","title":"Color Dependence of Dipole in CatWISE2020 Data","version":1},"cited_work":{"arxiv_id":"2405.16853","doi":null,"metadata_source":"pith","pith_arxiv_id":"2405.16853","snapshot_observed_at":"2026-08-11T13:29:05.008536Z","title":"Color Dependence of Dipole in CatWISE2020 Data","venue":"astro-ph.CO","work_id":"dc289e5a-451f-4110-a6d0-e6aff13a46ad","year":2024},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.883500Z"},"links":{"cited_paper":"/paper/2405.16853","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:bd8f4c940947704e54920a4f73ea94228d1109c4b10ba7db0123718f17eab4e4","observation_id":"4f91a941-d14c-43cf-b61d-64c5778b8153","resolution":{"observed_at":"2026-08-11T13:29:05.016141Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2301.03065","last_updated":"2023-03-29T03:13:33Z","snapshot_observed_at":"2026-08-13T13:08:11.086272Z","submitted_at":"2023-01-08T15:35:36Z","title":"Probing Cosmology beyond $\\Lambda$CDM using the SKA","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2301.03065","snapshot_observed_at":"2026-08-11T13:29:04.887484Z","title":"Ghosh, P","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.887484Z"},"links":{"cited_paper":"/paper/2301.03065","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:26da905947f15de2174d06b6ca2fb6d314a3bf23e1671a2128285a57cb398668","observation_id":"c8e4f730-4075-4fb8-a0e3-71876c0d4604","resolution":{"observed_at":"2026-08-11T13:29:04.887484Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:06.354736Z","title":null,"venue":null,"work_id":"e6307e3a-6f13-49d9-814e-1787c572f0a0","year":2020},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.891744Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:4a896a8e43a6207d10e19a4da8c74abf925c2c8925a6f6a11a019a8549417276","observation_id":"1672442f-2559-48f9-8125-fd06f86a597c","resolution":{"observed_at":"2026-08-11T13:29:06.358886Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:06.342811Z","title":"Virtanen, R","venue":null,"work_id":"a8276e45-01b9-4e21-8430-3a8b93271b6c","year":2020},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.896246Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:427816aabc9fc7820f0dc21989f17764087aedaee6602b6c51e433507698d895","observation_id":"001eb699-9715-4b6e-a9bc-de9926d3ed26","resolution":{"observed_at":"2026-08-11T13:29:06.346915Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:06.330968Z","title":null,"venue":null,"work_id":"77e734b0-ed53-4d04-9711-a76d70e5d612","year":2007},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.900756Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:7352df11e5209216e33b6339080dd55b2c17dbac74b1901365f76d58a596c9d8","observation_id":"934964ae-b810-4526-b6c7-88e759a62138","resolution":{"observed_at":"2026-08-11T13:29:06.335200Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:29:06.317637Z","title":null,"venue":null,"work_id":"cdbe659a-c411-4049-a944-3e27dcc1a544","year":2019},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.904824Z"},"links":{"citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:7280d24f5b260247160df3eac3e031c729ad933a2ab35f1073a7162fbe763863","observation_id":"a421bc4e-8a2d-4571-8c57-4756439686f4","resolution":{"observed_at":"2026-08-11T13:29:06.321947Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/0409513","last_updated":"2004-09-21T18:00:00Z","snapshot_observed_at":"2026-07-07T00:44:53.460945Z","submitted_at":"2004-09-21T18:00:00Z","title":"HEALPix -- a Framework for High Resolution Discretization, and Fast Analysis of Data Distributed on the Sphere","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"astro-ph/0409513","snapshot_observed_at":"2026-08-11T13:29:04.909447Z","title":null,"venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.909447Z"},"links":{"cited_paper":"/paper/astro-ph/0409513","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:90bb105bf7fe5a9542358b8fc9e0ec4367001e038a89a0205131c9638bac31e9","observation_id":"0dba5372-9830-497a-8ba1-f8a0796d0bdb","resolution":{"observed_at":"2026-08-11T13:29:04.909447Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/0210394","last_updated":"2002-10-17T15:23:07Z","snapshot_observed_at":"2026-07-07T00:29:06.550340Z","submitted_at":"2002-10-17T15:23:07Z","title":"The K correction","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"astro-ph/0210394","snapshot_observed_at":"2026-08-11T13:29:04.914154Z","title":null,"venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.914154Z"},"links":{"cited_paper":"/paper/astro-ph/0210394","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:4bcefb44537a2106eb8cc7cc4938503f1009426dccfa4f095cc1a646bbd42729","observation_id":"8630f362-3c71-4620-9889-c0a6bf0cccb1","resolution":{"observed_at":"2026-08-11T13:29:04.914154Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2410.04705","last_updated":"2025-03-26T14:29:55Z","snapshot_observed_at":"2026-08-12T22:29:32.674762Z","submitted_at":"2024-10-07T02:51:03Z","title":"Doppler bias: impact of peculiar velocities on color selection and the large scale structure of galaxy surveys","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2410.04705","snapshot_observed_at":"2026-08-11T13:29:04.918735Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole","version":2},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-11T13:29:04.918735Z"},"links":{"cited_paper":"/paper/2410.04705","citing_paper":"/paper/2412.13162"},"observation_digest":"sha256:071550c06852a6ee0559174863ab4042cba6cc6d4f201fa3902cdfd8ee9e4b96","observation_id":"aa5c46ad-8a4c-4dcd-87c3-bc76aac504be","resolution":{"observed_at":"2026-08-11T13:29:04.918735Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2412.13162","last_updated":"2025-05-20T09:42:18Z","latest_version":2,"primary_category":"astro-ph.CO","snapshot_observed_at":"2026-08-11T19:09:58.760524Z","submitted_at":"2024-12-17T18:39:11Z","title":"Redshift tomography of the kinematic matter dipole"},"reference_resolution":{"displayed":78,"state_counts":{"malformed_identifier":0,"metadata_mismatch":1,"parse_uncertain":0,"unresolved":55,"verified_exact":14,"verified_fuzzy":8},"total_outbound_references":78},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"thesis":"As of 13 August 2026, this Paper Citation Record lists 78 of 78 outbound references and 2 inbound Pith citation observations for arXiv:2412.13162."}