{"as_of":"2026-08-10T19:36:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:5cf596431997ac6ca06ffbe757ee8784016939e928370be8121e04cd75c53e36","coverage":[{"denominator":59,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":59,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-09T10:26:39.622401Z","state":"measured"},{"denominator":61,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":61,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-10T06:31:04.303077+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":"2026-08-07T10:45:08.664229Z","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":"2026-05-21T14:30:13.667752Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2502.03003","snapshot_observed_at":"2026-08-07T10:45:08.664229Z","title":"Non-uniquenessoftheshockwavedynamicsineffectiveloopquantumgravity,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2506.04589","last_updated":"2025-08-24T09:56:15Z","snapshot_observed_at":"2026-08-09T06:42:31.163816Z","submitted_at":"2025-06-05T03:10:19Z","title":"Dust shell in effective loop quantum black hole model","version":3},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-07T10:45:08.664229Z"},"links":{"cited_paper":"/paper/2502.03003","citing_paper":"/paper/2506.04589"},"observation_digest":"sha256:905d8a494fd06212e350bb2b7ca9f1b5e7aebedb66b107b9af87efaf0a1136fb","observation_id":"386e8fb6-960c-4f95-b919-6dfb3d3b7615","resolution":{"observed_at":"2026-08-07T10:45:08.664229Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"cited_work":{"arxiv_id":"2502.03003","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2502.03003","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Non-uniqueness of shockwave evolution in a loop quantum gravity inspired model","venue":null,"work_id":"15a6a6de-8d8c-4471-b599-adcf51ae47e7","year":2025},"citing_paper":{"arxiv_id":"2601.18618","last_updated":"2026-05-15T08:42:01Z","snapshot_observed_at":"2026-08-01T19:23:10.009696Z","submitted_at":"2026-01-26T15:57:34Z","title":"Quantum gravitational stellar evolution beyond shell-crossing singularities","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-05-21T14:29:56.522601Z"},"links":{"cited_paper":"/paper/2502.03003","citing_paper":"/paper/2601.18618"},"observation_digest":"sha256:3f9ad084b857332a411fc0b56d91a36fc4d1f664c80ce3042c3e1275aee466ee","observation_id":"7d081748-a397-45c7-a1df-1f290cbb8881","resolution":{"observed_at":"2026-05-21T14:30:13.669830Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2502.03003/citation-record","integrity":"/paper/2502.03003/integrity","json":"/paper/2502.03003/citation-record.json","paper":"/paper/2502.03003"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-09T10:26:40.906021Z","title":"(26) Let’s look ﬁrst at the denominator computed in the inte- rior ( − term)","venue":null,"work_id":"a67e2a01-1a2a-46e7-ad55-419e5e280b90","year":null},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.356016Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:ca957b6c25071d9bdc0e8d9c661a35121226a7ffa6f667e40b3389f4a7be59dc","observation_id":"2686a7bb-df9b-48d2-92f2-fef90252be63","resolution":{"observed_at":"2026-08-09T10:26:40.912067Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-09T10:26:41.072443Z","title":"(5) In order to write the ﬁrst term in the required form (4), we use the following identity: sinn ( B r2 ) = n∑ k=0 (−1)k 2n (n k ) cos [ (n − 2k)B r2 − π 2 n ]","venue":null,"work_id":"8d9cecba-096c-44d7-967d-69d971a916dc","year":null},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.307052Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:bf7142c7e7de9abdc83a55006d736466970122634d52e6eed58b68f2b2005983","observation_id":"1f1629a4-cf98-4d83-b7e1-6e4ea082a174","resolution":{"observed_at":"2026-08-09T10:26:41.077804Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-09T10:26:41.089758Z","title":"(4) To achieve this goal, we multiply (","venue":null,"work_id":"2c679fba-cc82-4f1a-88f0-7c50f5dd4f11","year":null},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.301291Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:38ae96c08e81186203b70a30e9921d9f037fc48be24898e0e5d0a6064861cb9b","observation_id":"16cb5ba2-03c3-4d70-9d16-891e4d4baa16","resolution":{"observed_at":"2026-08-09T10:26:41.094945Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-09T10:26:41.038712Z","title":"The analytic solution of the previous equation reads r(R, t ) = [2 Gm(R)] 1 3 { [t − α (R)]2 + ∆ } 1 3 , (12) where α (R) is ﬁxed by the initial condition","venue":null,"work_id":"e31e6ac8-c754-414e-a527-db46c56060a6","year":null},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.317753Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:c5a4ed56a293f3005f0c23a2d35f2f2f4873288c86dd86e4cf481c13172e3af7","observation_id":"c6ffdcfd-136e-4e53-8593-0c70474faaf8","resolution":{"observed_at":"2026-08-09T10:26:41.044226Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-09T10:26:41.056164Z","title":null,"venue":null,"work_id":"0f29467f-2710-4012-a3c9-f604356f4940","year":null},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.312596Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:d214baee66f1c1eebdab1eb3194e712c1afefde4fe43ed998e9a7d0324700304","observation_id":"81c12d20-a8af-4706-b164-314c0f0d6e3f","resolution":{"observed_at":"2026-08-09T10:26:41.061657Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-09T10:26:41.018943Z","title":null,"venue":null,"work_id":"d7d9365f-3c42-4659-b1cb-9ac0fde0eaaa","year":null},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.323547Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:a3f6c27cbf169b5b7e69516f00e97e8ef60d925328589bd998476839c13e058a","observation_id":"9fd97fcb-a9e4-451e-9756-54cbaed06eec","resolution":{"observed_at":"2026-08-09T10:26:41.026009Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-09T10:26:40.997989Z","title":null,"venue":null,"work_id":"9874763a-f5da-439f-9ea1-5efbcb88e8ff","year":null},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.329199Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:108e70745f37fa3933883e05458c23e06ceaca7571fa9fbed98c8062183898a0","observation_id":"bcad6647-6e87-4c4d-9059-6defe34ae012","resolution":{"observed_at":"2026-08-09T10:26:41.003592Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-09T10:26:40.979734Z","title":"This comes from having required that the interior is almost homogeneous","venue":null,"work_id":"3bb586d5-b387-4a59-a712-da44f7af2c50","year":null},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.334805Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:4b13fe2decc3ae023b1086525ced0f4f7b7aaf9272dcda058e4e8d2f43929872","observation_id":"e6f3e50a-5bc1-4ab9-9b26-04f933025450","resolution":{"observed_at":"2026-08-09T10:26:40.985497Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-09T10:26:40.962354Z","title":"Since the same holds also for the pre- bounce dynamics [8], and this range is the one in which the function v(B, r ) is invertible, the equations (","venue":null,"work_id":"b3aab240-923f-44ca-b24b-723b35982f50","year":null},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.339833Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:33741f505aca488a74cf634448e978b3ea9da43d1286b3fa32c26f5bcbe2c773","observation_id":"a8433bc7-6a30-4745-bbdb-9cb5468a12ee","resolution":{"observed_at":"2026-08-09T10:26:40.968204Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-09T10:26:40.943569Z","title":"Even if ﬁnding the inverse of ( 9) for generic n is a non-trivial task, it is outside the aim of this work since not necessary to derive the analytic shockwave dy- namics","venue":null,"work_id":"cf84bb64-6631-45b8-8a07-249c401f9fac","year":null},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.344318Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:253467043546c09ab374ee4a947de83bf949bf05d11d874bdace224a9d5a27da","observation_id":"c778d555-766e-4a13-acc3-81e30611babb","resolution":{"observed_at":"2026-08-09T10:26:40.949825Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2107.05797","last_updated":"2021-07-13T00:56:22Z","snapshot_observed_at":"2026-08-10T00:59:29.455413Z","submitted_at":"2021-07-13T00:56:22Z","title":"Non-singular quantum gravitational dynamics of an LTB dust shell model: the role of quantization prescriptions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2107.05797","snapshot_observed_at":"2026-08-09T10:26:39.438503Z","title":"Nonsingular quantum gravitational dynamics of an Lemaˆ ıtre-Tolman-Bondi dust shell model: The role of quantization prescriptions,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.438503Z"},"links":{"cited_paper":"/paper/2107.05797","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:fd93cb276d487485520ea58d232a943a26a5eee18f2b698558d337b358ac411c","observation_id":"1be37169-1c7b-40f9-9fe1-ba7fddd8b7ec","resolution":{"observed_at":"2026-08-09T10:26:39.438503Z","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":"2026-08-09T10:26:40.889013Z","title":"Let’s look therefore at the denominator, in particular at the − term and call it D−","venue":null,"work_id":"2b56eef0-9a0a-4554-a5ca-c4cc664669be","year":null},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.360834Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:2cb5b5a95c33858e55a5cdd7c77a82afdebb8a7de786e7c1661397df70761df3","observation_id":"403af9fd-0c92-4999-8a3a-00890fcf6310","resolution":{"observed_at":"2026-08-09T10:26:40.894407Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-09T10:26:40.872074Z","title":null,"venue":null,"work_id":"21f2919d-fa39-47c3-ade3-3de33a1b3125","year":null},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.365792Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:49f583e07d8edc345667538595bafe96745ee4bef2996c6d30fd91b29e88eedf","observation_id":"c7fbfa0b-1eb0-4aa2-9b77-655ab53659a9","resolution":{"observed_at":"2026-08-09T10:26:40.877737Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-09T10:26:40.854781Z","title":"Despite this, from 6 a physical perspective, this ambiguity could enlarge the window of quantum gravitational signatures from black hole physics","venue":null,"work_id":"7d8669e2-2760-4b3a-968b-44a8b851eb95","year":null},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.370576Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:9bea20de205eb9748cc58988cdbede3fe0e8ddd2575e40087d61ce2837db4f10","observation_id":"c0db2586-ca9c-4e17-bf51-0f49ca96eb7a","resolution":{"observed_at":"2026-08-09T10:26:40.860570Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-09T10:26:40.837640Z","title":"Gravitational collapse and space-time sin- gularities,","venue":null,"work_id":"71ea35fa-3912-4cf3-84b3-91cf9eedcfff","year":1965},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.375686Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:0e9253774017e62fac7750070fd9f051035e0ea190c98ad57f20d39786deacd7","observation_id":"d53b0cae-b81a-497b-8925-583b1898afa0","resolution":{"observed_at":"2026-08-09T10:26:40.842972Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1401.6562","last_updated":"2014-02-08T23:28:03Z","snapshot_observed_at":"2026-08-02T21:30:43.838683Z","submitted_at":"2014-01-25T18:09:39Z","title":"Planck stars","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1401.6562","snapshot_observed_at":"2026-08-09T10:26:39.380839Z","title":"Planck stars,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.380839Z"},"links":{"cited_paper":"/paper/1401.6562","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:a6f5d14c0b4cb3c2c83d80f4cbb7ce89ce1da4df1bf25ac3a24b0b21f08213d2","observation_id":"24589f1a-c89c-47d8-b0dc-367a888ac918","resolution":{"observed_at":"2026-08-09T10:26:39.380839Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2109.08667","last_updated":"2022-03-22T15:17:41Z","snapshot_observed_at":"2026-08-10T17:03:46.075842Z","submitted_at":"2021-09-17T17:48:25Z","title":"Quantum gravity of dust collapse: shock waves from black holes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2109.08667","snapshot_observed_at":"2026-08-09T10:26:39.386515Z","title":"Quantum Gravity of Dust Collapse: Shock Waves from Black Holes,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.386515Z"},"links":{"cited_paper":"/paper/2109.08667","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:00c29291ddde69eeaeb4736b4d8fb38a1e9315ff215d65dde6415f310d2d4fdb","observation_id":"fd0fa301-d977-49a2-8d60-197d4a2d2b4b","resolution":{"observed_at":"2026-08-09T10:26:39.386515Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2302.03872","last_updated":"2023-02-08T04:14:43Z","snapshot_observed_at":"2026-08-10T10:55:56.798333Z","submitted_at":"2023-02-08T04:14:43Z","title":"On the geometry of the black-to-white hole transition within a single asymptotic region","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2302.03872","snapshot_observed_at":"2026-08-09T10:26:39.392264Z","title":"Geometry of the black-to-white hole transition within a single asymptotic region,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.392264Z"},"links":{"cited_paper":"/paper/2302.03872","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:ccd094b4d3de49fa08cfbe7ce8363f044b7847cce25f5796b03c0e787957c008","observation_id":"17de3638-b164-47e7-a7bf-7eefb61b6605","resolution":{"observed_at":"2026-08-09T10:26:39.392264Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2308.10953","last_updated":"2023-08-21T18:00:13Z","snapshot_observed_at":"2026-08-10T10:55:49.801570Z","submitted_at":"2023-08-21T18:00:13Z","title":"Generalized analysis of a dust collapse in effective loop quantum gravity: fate of shocks and covariance","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2308.10953","snapshot_observed_at":"2026-08-09T10:26:39.398332Z","title":"Generalized analysis of a dust collapse in eﬀective loop quantum grav- ity: fate of shocks and covariance,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.398332Z"},"links":{"cited_paper":"/paper/2308.10953","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:8c0d6784c2d9e237b73dd4bd91e838a59a33952594f4fe83f439c7461d58b4fd","observation_id":"94820c86-38de-4769-84a8-3f254b86ba71","resolution":{"observed_at":"2026-08-09T10:26:39.398332Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2210.02253","last_updated":"2023-02-28T16:55:27Z","snapshot_observed_at":"2026-08-09T11:25:50.463466Z","submitted_at":"2022-10-05T13:31:50Z","title":"Quantum Oppenheimer-Snyder and Swiss Cheese models","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2210.02253","snapshot_observed_at":"2026-08-09T10:26:39.403842Z","title":"Quan- tum Oppenheimer-Snyder and Swiss Cheese Models,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.403842Z"},"links":{"cited_paper":"/paper/2210.02253","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:b0843b86acba9e4766d00e4dbb80f044727d81b94787dc4bd86339d3bbe38ce7","observation_id":"b8690319-57ee-4c07-bb34-fb7f7ca0e1ce","resolution":{"observed_at":"2026-08-09T10:26:39.403842Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2307.07797","last_updated":"2023-08-03T08:08:33Z","snapshot_observed_at":"2026-08-10T14:10:14.634407Z","submitted_at":"2023-07-15T13:06:06Z","title":"Painlev\\'e-Gullstrand coordinates discontinuity in the quantum Oppenheimer-Snyder model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2307.07797","snapshot_observed_at":"2026-08-09T10:26:39.414636Z","title":"Painlev´ e- Gullstrand coordinates discontinuity in the quantum Oppenheimer-Snyder model,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.414636Z"},"links":{"cited_paper":"/paper/2307.07797","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:c3731bdc445b093a7d0098b44d8754bad3e722590c4eceadaa7b9fe7ad3c0c34","observation_id":"3559826a-1303-46c1-b7b6-2cceddeb853e","resolution":{"observed_at":"2026-08-09T10:26:39.414636Z","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":"2026-08-09T10:26:40.924118Z","title":"(25) In order to write the denominator explicitly, we need to distinguish between odd and even n","venue":null,"work_id":"e10d784d-856b-43bd-9dfc-2112c61575da","year":null},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.349552Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:01f060b4bae93df26898a5712f521dfcca3b9dcb0a11b24a1397e62192248bef","observation_id":"aac8d414-9492-46f6-9d12-8e044ea5289c","resolution":{"observed_at":"2026-08-09T10:26:40.930622Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2203.04238","last_updated":"2022-06-13T20:29:17Z","snapshot_observed_at":"2026-08-10T13:06:27.623994Z","submitted_at":"2022-03-08T17:54:26Z","title":"On the fate of quantum black holes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2203.04238","snapshot_observed_at":"2026-08-09T10:26:39.421134Z","title":"Fate of quantum black holes,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.421134Z"},"links":{"cited_paper":"/paper/2203.04238","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:1df5dc66a734d200a17fdd872ab6ec025a2a002625f7880f5b95954c9828bbd2","observation_id":"a8ab544e-9efb-46ca-8d15-c62ab745a310","resolution":{"observed_at":"2026-08-09T10:26:39.421134Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2006.09325","last_updated":"2022-06-13T20:31:59Z","snapshot_observed_at":"2026-08-06T23:02:37.285141Z","submitted_at":"2020-06-16T17:06:39Z","title":"Black hole collapse and bounce in effective loop quantum gravity","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.09325","snapshot_observed_at":"2026-08-09T10:26:39.426782Z","title":"Black hole collapse and bounce in eﬀective loop quan- tum gravity,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.426782Z"},"links":{"cited_paper":"/paper/2006.09325","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:031dc4a68475679988f0592129df56a550cbb40cae3d219f8eef4fc673d55b6e","observation_id":"c9cc769c-ae98-47ea-8593-c6c97673a148","resolution":{"observed_at":"2026-08-09T10:26:39.426782Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2004.12977","last_updated":"2020-07-21T08:12:48Z","snapshot_observed_at":"2026-08-08T04:47:27.442152Z","submitted_at":"2020-04-27T17:45:14Z","title":"Towards consistent black-to-white hole bounces from matter collapse","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2004.12977","snapshot_observed_at":"2026-08-09T10:26:39.432365Z","title":"Towards consistent black-to-white hole bounces from matter collapse,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.432365Z"},"links":{"cited_paper":"/paper/2004.12977","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:1b8f9bf6b2850be201056065e9cf1e60e11eca6b1a66c2f1f644e50ba7e9fca3","observation_id":"fb634d13-60a8-404b-afec-a069bd4564a7","resolution":{"observed_at":"2026-08-09T10:26:39.432365Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1707.07333","last_updated":"2017-09-20T12:43:59Z","snapshot_observed_at":"2026-07-06T05:52:19.613514Z","submitted_at":"2017-07-23T19:13:25Z","title":"From black holes to white holes: a quantum gravitational, symmetric bounce","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1707.07333","snapshot_observed_at":"2026-08-09T10:26:39.443829Z","title":"From black holes to white holes: a quantum gravitational, symmet- ric bounce,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.443829Z"},"links":{"cited_paper":"/paper/1707.07333","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:bbf1f6c59aeff1d1729e67887d10bb49091c081a1e5cbf1c01a34bf9851e9d6b","observation_id":"f19de82b-1def-4515-b347-17b5ba654d2c","resolution":{"observed_at":"2026-08-09T10:26:39.443829Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1802.04264","last_updated":"2018-03-17T16:53:19Z","snapshot_observed_at":"2026-08-06T15:43:14.586881Z","submitted_at":"2018-02-12T17:24:41Z","title":"White Holes as Remnants: A Surprising Scenario for the End of a Black Hole","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1802.04264","snapshot_observed_at":"2026-08-09T10:26:39.449061Z","title":"White Holes as Remnants: A Surprising Scenario for the End of a Black Hole,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.449061Z"},"links":{"cited_paper":"/paper/1802.04264","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:e06f0abc29fc17fd89319134f0b6633609dd30eedb065fb5023b19fd5b6bd447","observation_id":"6b126228-5610-4ebd-bef6-f400f8ffaa7f","resolution":{"observed_at":"2026-08-09T10:26:39.449061Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1605.05268","last_updated":"2016-09-14T11:42:48Z","snapshot_observed_at":"2026-07-06T04:56:36.516881Z","submitted_at":"2016-05-17T17:59:54Z","title":"Realistic Observable in Background-Free Quantum Gravity: the Planck-Star Tunnelling-Time","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1605.05268","snapshot_observed_at":"2026-08-09T10:26:39.454257Z","title":"Planck star tunneling time: An astrophysically rele- vant observable from background-free quantum gravity,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.454257Z"},"links":{"cited_paper":"/paper/1605.05268","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:9b8beefb8ea382b60d6589c6585c31767360d72594589c476d919419af9f5fd8","observation_id":"6fd184e0-bc1c-4343-87b3-eb8ee2871ec1","resolution":{"observed_at":"2026-08-09T10:26:39.454257Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2010.13480","last_updated":"2021-08-16T11:35:32Z","snapshot_observed_at":"2026-08-10T12:18:14.372434Z","submitted_at":"2020-10-26T10:57:18Z","title":"Effective Quantum Dust Collapse via Surface Matching","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.13480","snapshot_observed_at":"2026-08-09T10:26:39.459368Z","title":"Eﬀective quantum dust collapse via sur- face matching,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.459368Z"},"links":{"cited_paper":"/paper/2010.13480","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:9adf4c919881178795921d57ebe091c77eecf3de19b344a939409373b00bde79","observation_id":"e0f7a86e-bb77-48a4-bafb-0ced947899d6","resolution":{"observed_at":"2026-08-09T10:26:39.459368Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2001.06153","last_updated":"2020-12-02T17:24:14Z","snapshot_observed_at":"2026-08-08T14:41:46.875470Z","submitted_at":"2020-01-17T04:11:14Z","title":"Bouncing compact objects. Part II: Effective theory of a pulsating Planck star","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2001.06153","snapshot_observed_at":"2026-08-09T10:26:39.464374Z","title":"Bouncing compact ob- jects. II. Eﬀective theory of a pulsating Planck star,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.464374Z"},"links":{"cited_paper":"/paper/2001.06153","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:c63b35d36cf8bce76a616754a4a19634d84a1a7430766776f974a7a18ce4e62a","observation_id":"5de3f8ad-44a6-4e1d-945c-d06b8b1a9b24","resolution":{"observed_at":"2026-08-09T10:26:39.464374Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.12708","last_updated":"2023-03-22T16:47:33Z","snapshot_observed_at":"2026-08-10T08:44:19.460644Z","submitted_at":"2023-03-22T16:47:33Z","title":"Rainbow Oppenheimer-Snyder collapse and the entanglement entropy production","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.12708","snapshot_observed_at":"2026-08-09T10:26:39.469166Z","title":"Rainbow Oppenheimer- Snyder collapse and the entanglement entropy production,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.469166Z"},"links":{"cited_paper":"/paper/2303.12708","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:bfa0cd5988359650898674f2524bb33d85fb0e7ac1625c2bcb3c4cde065b3f72","observation_id":"508d70ea-fff6-4b28-8b20-286b33899cc4","resolution":{"observed_at":"2026-08-09T10:26:39.469166Z","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":"2026-08-09T10:26:39.474236Z","title":"Status of Birkhoﬀ’s the- orem in the polymerized semiclassical regime of loop quantum gravity,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.474236Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:f68876633476403aae6e1c7f06763e14641a4406ea7a49440de43385aa1d05f6","observation_id":"4157314f-fb6b-435c-a4a7-5a4bf4a9bc08","resolution":{"observed_at":"2026-08-09T10:26:39.474236Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.15505","last_updated":"2024-03-06T16:48:22Z","snapshot_observed_at":"2026-08-10T10:55:33.370307Z","submitted_at":"2023-12-24T15:14:01Z","title":"Nonsingular collapse of a spherical dust cloud","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.15505","snapshot_observed_at":"2026-08-09T10:26:39.479121Z","title":"Nonsingular col- lapse of a spherical dust cloud,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.479121Z"},"links":{"cited_paper":"/paper/2312.15505","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:2927623101dd06d3a4cbac99164b131530b767a2ef6ffc259b6fdda621a25f37","observation_id":"3ec98d53-a87c-47fa-b8cc-03c7e4b22f6e","resolution":{"observed_at":"2026-08-09T10:26:39.479121Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2308.10890","last_updated":"2026-05-04T20:40:29Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2023-08-21T17:44:26Z","title":"Dust collapse in asymptotic safety: a path to regular black holes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2308.10890","snapshot_observed_at":"2026-08-09T10:26:39.484461Z","title":"Dust Collapse in Asymptotic Safety: A Path to Regular Black Holes,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.484461Z"},"links":{"cited_paper":"/paper/2308.10890","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:8d276d565d2f0d2f3ab1257d60c5cfc50bb5846b5ee5aa088ba05dbab99ee6b4","observation_id":"aa1c385d-90fd-42b0-86d1-be201eaecb6c","resolution":{"observed_at":"2026-08-09T10:26:39.484461Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2001.06148","last_updated":"2020-04-27T14:21:57Z","snapshot_observed_at":"2026-08-08T14:57:09.174513Z","submitted_at":"2020-01-17T03:45:37Z","title":"Bouncing compact objects I: Quantum extension of the Oppenheimer-Snyder collapse","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2001.06148","snapshot_observed_at":"2026-08-09T10:26:39.489755Z","title":"Bounc- ing compact objects. Part I. Quantum extension of the Oppenheimer-Snyder collapse,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.489755Z"},"links":{"cited_paper":"/paper/2001.06148","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:4c4f99b773f820c70abc475a5f85b94d0a5b827951375b157c9f9b4955d5e9e0","observation_id":"158002fb-f837-44fe-909e-5f4a4e03ea06","resolution":{"observed_at":"2026-08-09T10:26:39.489755Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1405.7249","last_updated":"2014-08-17T16:19:27Z","snapshot_observed_at":"2026-07-06T03:44:53.228869Z","submitted_at":"2014-05-28T14:14:51Z","title":"Singularity avoidance in quantum-inspired inhomogeneous dust collapse","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1405.7249","snapshot_observed_at":"2026-08-09T10:26:39.494690Z","title":"Singularity avoidance in quantum-inspired inhomoge- neous dust collapse,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.494690Z"},"links":{"cited_paper":"/paper/1405.7249","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:6dda52c4201b1bee478d033656511af18a229856da65bd517cb563f201c1f125","observation_id":"28e060e2-189c-45f5-8cef-b692df30ec6d","resolution":{"observed_at":"2026-08-09T10:26:39.494690Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1305.4790","last_updated":"2013-08-06T07:10:09Z","snapshot_observed_at":"2026-07-06T03:13:51.698831Z","submitted_at":"2013-05-21T11:54:15Z","title":"Non-singular quantum-inspired gravitational collapse","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1305.4790","snapshot_observed_at":"2026-08-09T10:26:39.500472Z","title":"Non-singular quantum-inspired gravitational collapse,","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.500472Z"},"links":{"cited_paper":"/paper/1305.4790","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:d987ea731805e88c7da4d45b46a5919adba31ac36408b9d616a71a4cf5b77f1c","observation_id":"f7710646-c466-4289-bb63-fdde8fb3f581","resolution":{"observed_at":"2026-08-09T10:26:39.500472Z","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":"2026-08-09T10:26:39.506289Z","title":"Stellar collapse with pressure in eﬀective loop quantum gravity,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.506289Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:8ba774b001c10b88501fb15508f790722bb8572964d36d37886ea82eeeaf087f","observation_id":"0e2ca7a3-5abd-4ec3-bafd-22fddf9ca20f","resolution":{"observed_at":"2026-08-09T10:26:39.506289Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/0612070","last_updated":"2007-02-07T14:23:38Z","snapshot_observed_at":"2026-08-05T09:58:56.525184Z","submitted_at":"2006-12-12T14:28:20Z","title":"Loop quantum cosmology and the k = - 1 RW model","version":2},"cited_work":{"arxiv_id":"gr-qc/0612070","doi":null,"metadata_source":"pith","pith_arxiv_id":"gr-qc/0612070","snapshot_observed_at":"2026-08-09T10:26:39.929300Z","title":"Loop quantum cosmology and the k = - 1 RW model","venue":"gr-qc","work_id":"457efff6-b10f-47d2-b507-3ff6ae45909f","year":2006},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.511708Z"},"links":{"cited_paper":"/paper/gr-qc/0612070","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:91a25e6c5f43961b88de9219b4b37325730ef410f47218762d61c8ef8a4b1fc5","observation_id":"c1b97737-4612-4166-88d8-c555a83ed35a","resolution":{"observed_at":"2026-08-09T10:26:39.934616Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1310.6728","last_updated":"2014-01-22T15:31:52Z","snapshot_observed_at":"2026-07-06T03:26:28.991211Z","submitted_at":"2013-10-24T19:49:08Z","title":"Quantization ambiguities and bounds on geometric scalars in anisotropic loop quantum cosmology","version":2},"cited_work":{"arxiv_id":"1310.6728","doi":null,"metadata_source":"pith","pith_arxiv_id":"1310.6728","snapshot_observed_at":"2026-08-09T10:26:39.904524Z","title":"Quantization ambiguities and bounds on geometric scalars in anisotropic loop quantum cosmology","venue":"gr-qc","work_id":"0dd87ab6-2f97-4f74-a911-46e683fa173b","year":2013},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.517073Z"},"links":{"cited_paper":"/paper/1310.6728","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:f5dc0176dc38862095f9eedbc6c6703579d486dac11dd7eb56794f1ca4165b54","observation_id":"910e7311-afe3-4106-9983-49a4b2ad616f","resolution":{"observed_at":"2026-08-09T10:26:39.910337Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/0607039","last_updated":"2006-08-30T19:04:05Z","snapshot_observed_at":"2026-07-07T03:22:44.516364Z","submitted_at":"2006-07-10T17:20:55Z","title":"Quantum Nature of the Big Bang: Improved dynamics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/0607039","snapshot_observed_at":"2026-08-09T10:26:39.522451Z","title":"Quantum Na- ture of the Big Bang: Improved dynamics,","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.522451Z"},"links":{"cited_paper":"/paper/gr-qc/0607039","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:755439861d83f553f85a83693e066ed3d54c270850a2aded6851c63c3c99e58c","observation_id":"18ad3d20-bfaa-4d3c-99aa-17505d547ff5","resolution":{"observed_at":"2026-08-09T10:26:39.522451Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0709.2129","last_updated":"2007-10-08T10:07:45Z","snapshot_observed_at":"2026-07-06T01:33:48.430163Z","submitted_at":"2007-09-13T17:10:18Z","title":"Loop Quantum Dynamics of the Schwarzschild Interior","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0709.2129","snapshot_observed_at":"2026-08-09T10:26:39.528621Z","title":"Loop Quantum Dy- namics of the Schwarzschild Interior,","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.528621Z"},"links":{"cited_paper":"/paper/0709.2129","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:0f732971e4e888d25c472734673638d9860be552d171fef46d49315052756d07","observation_id":"51de280a-766e-43e5-bac1-9f48ae624851","resolution":{"observed_at":"2026-08-09T10:26:39.528621Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2012.14212","last_updated":"2021-06-15T12:21:49Z","snapshot_observed_at":"2026-08-10T01:37:44.578302Z","submitted_at":"2020-12-28T12:28:02Z","title":"Loop quantum black hole extensions within the improved dynamics","version":2},"cited_work":{"arxiv_id":"2012.14212","doi":null,"metadata_source":"pith","pith_arxiv_id":"2012.14212","snapshot_observed_at":"2026-08-09T10:26:39.843748Z","title":"Loop quantum black hole extensions within the improved dynamics","venue":"gr-qc","work_id":"9151a22d-8369-4795-93ea-ea3fa22ef4e9","year":2020},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.534827Z"},"links":{"cited_paper":"/paper/2012.14212","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:87ad454d5f34ed5b234b024228d69d926249123997481dc7075ea4c2ce8487da","observation_id":"98921d8a-0d0c-461c-81da-2dfd4d2d1ba4","resolution":{"observed_at":"2026-08-09T10:26:39.849383Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2006.09302","last_updated":"2022-06-13T20:35:29Z","snapshot_observed_at":"2026-08-04T03:14:14.024230Z","submitted_at":"2020-06-16T16:46:03Z","title":"Effective loop quantum gravity framework for vacuum spherically symmetric space-times","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.09302","snapshot_observed_at":"2026-08-09T10:26:39.540794Z","title":"Eﬀec- tive loop quantum gravity framework for vacuum spher- ically symmetric spacetimes,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.540794Z"},"links":{"cited_paper":"/paper/2006.09302","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:c08bb5dc00b065eba86f3cffbb798d4e366ca9c088e1cf5dfd7c6c1d709f8a1e","observation_id":"e5104562-a2c8-46c2-a674-adb15f51e9ed","resolution":{"observed_at":"2026-08-09T10:26:39.540794Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2308.10949","last_updated":"2023-08-21T18:00:10Z","snapshot_observed_at":"2026-07-06T16:08:41.390521Z","submitted_at":"2023-08-21T18:00:10Z","title":"Embedding generalized LTB models in polymerized spherically symmetric spacetimes","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2308.10949","snapshot_observed_at":"2026-08-09T10:26:39.546360Z","title":"Embedding generalized LTB models in polymerized spherically symmetric spacetimes,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.546360Z"},"links":{"cited_paper":"/paper/2308.10949","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:578b392e9e711884fc66a234e007456f7c99aad6c64e174cb856300fbcdcb4d6","observation_id":"d6e9e291-fb73-4384-a61e-9111c5b7d4b5","resolution":{"observed_at":"2026-08-09T10:26:39.546360Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.02032","last_updated":"2024-04-09T18:34:24Z","snapshot_observed_at":"2026-08-10T10:54:29.866983Z","submitted_at":"2023-12-04T16:52:15Z","title":"Shell-crossings and shock formation during gravitational collapse in effective loop quantum gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.02032","snapshot_observed_at":"2026-08-09T10:26:39.551605Z","title":"Shell- crossings and shock formation during gravitational col- lapse in eﬀective loop quantum gravity,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.551605Z"},"links":{"cited_paper":"/paper/2312.02032","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:f010d039712700a87eb8543f032ee751baaf07edc004be060de26c6260757d1d","observation_id":"1b55fcc0-6b82-4ea7-9d35-f8316f286a0a","resolution":{"observed_at":"2026-08-09T10:26:39.551605Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2404.04192","last_updated":"2024-09-05T15:51:12Z","snapshot_observed_at":"2026-08-06T07:28:25.984518Z","submitted_at":"2024-04-05T16:04:23Z","title":"Gravitational collapse in effective loop quantum gravity: beyond marginally bound configurations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2404.04192","snapshot_observed_at":"2026-08-09T10:26:39.556891Z","title":"Gravita- tional collapse in eﬀective loop quantum gravity: Be- yond marginally bound conﬁgurations,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.556891Z"},"links":{"cited_paper":"/paper/2404.04192","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:73761c9bceddc129c7dc342e7db06a24c80334cd9c5a46141ec36a6b1e255abd","observation_id":"55085937-24eb-4b61-8b28-ec00739d8630","resolution":{"observed_at":"2026-08-09T10:26:39.556891Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2103.17112","last_updated":"2021-08-26T10:53:12Z","snapshot_observed_at":"2026-08-10T14:34:53.361097Z","submitted_at":"2021-03-31T14:30:31Z","title":"Causal Structure of a recent Loop Quantum Gravity Black Hole Collapse Model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2103.17112","snapshot_observed_at":"2026-08-09T10:26:39.561912Z","title":"Causal structure of a recent loop quantum gravity black hole collapse model,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.561912Z"},"links":{"cited_paper":"/paper/2103.17112","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:746f5aa42c53561ac7c8d90ab3050690e20c1bc29db4ddf882a857c01934e245","observation_id":"39939073-c5b2-4cfe-b735-5b53c8f51339","resolution":{"observed_at":"2026-08-09T10:26:39.561912Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.16533","last_updated":"2025-03-03T14:33:35Z","snapshot_observed_at":"2026-08-07T05:48:54.252525Z","submitted_at":"2024-08-29T13:43:51Z","title":"Static Planck stars from effective loop quantum gravity","version":2},"cited_work":{"arxiv_id":"2408.16533","doi":null,"metadata_source":"pith","pith_arxiv_id":"2408.16533","snapshot_observed_at":"2026-08-09T10:26:39.732559Z","title":"Static Planck stars from effective loop quantum gravity","venue":"gr-qc","work_id":"3da61996-3773-490b-b533-55ccc08bc27f","year":2024},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.567284Z"},"links":{"cited_paper":"/paper/2408.16533","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:4c18b285267f3c3d370a5f9bff97ef6cfbbb9530b8a544e46206a378530ca39c","observation_id":"d630c373-fe03-4fda-a42d-737fd792a571","resolution":{"observed_at":"2026-08-09T10:26:39.740096Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-09T10:26:40.819291Z","title":"Shell crossings and the Tolman model,","venue":null,"work_id":"b95b29fe-4045-4621-9eef-84c5c9f397af","year":1985},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.574914Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:9670d892137dc96113b1eaa235ae2068f7312617a23ce6f637ba885e99265f2f","observation_id":"72671a37-7eb2-48e5-9826-f8d61772fdf2","resolution":{"observed_at":"2026-08-09T10:26:40.825749Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-09T10:26:40.800757Z","title":"What is a shell crossing singu- larity?,","venue":null,"work_id":"5fac3e07-35d6-4944-a97e-9a0b763a4abd","year":1999},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.580595Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:022e3ddc807e88f6442268843588fa231a9baee2b9d14ef3c03eede4c2c42bd9","observation_id":"310b8843-d781-4ead-9cbc-ebbc1c88ce0c","resolution":{"observed_at":"2026-08-09T10:26:40.806204Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/0301028","last_updated":"2003-01-08T18:02:22Z","snapshot_observed_at":"2026-07-07T03:17:11.181957Z","submitted_at":"2003-01-08T18:02:22Z","title":"Dynamical extensions for shell-crossing singularities","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/0301028","snapshot_observed_at":"2026-08-09T10:26:39.585748Z","title":"Dynamical extensions for shell crossing singularities,","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.585748Z"},"links":{"cited_paper":"/paper/gr-qc/0301028","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:c424e842883b0634b481830869fbcbd07b9cb8eeb8c3fc0e5e8eb79b3146fbc6","observation_id":"0a2f9f33-9b71-446e-bcfe-6ae7ca136cc8","resolution":{"observed_at":"2026-08-09T10:26:39.585748Z","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":"2026-08-09T10:26:40.783457Z","title":null,"venue":null,"work_id":"ac4aadb0-1682-4c70-9c64-48b707860a07","year":2002},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.591338Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:09a336aef36b23fe8f4472b805372c66396834049eb068acb1a7e90fd0ffd6c8","observation_id":"9162d35b-4d00-45dd-a7a8-9e756b4de2fa","resolution":{"observed_at":"2026-08-09T10:26:40.788702Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-09T10:26:40.766285Z","title":"Linear and nonlinear waves,","venue":null,"work_id":"7a02a066-d414-4059-ad57-817233da4610","year":2009},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.596054Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:895b560a80d619142a220c1d1811e17496435f3fa8cc9f59420c8ac3a51912ed","observation_id":"f027e10c-297a-4abb-8bff-e1e2ea9147d6","resolution":{"observed_at":"2026-08-09T10:26:40.771498Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-09T10:26:40.749740Z","title":null,"venue":null,"work_id":"c2112192-065f-465a-b1b4-0af3ebb0df6b","year":2000},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.600813Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:e17de916d66675b352b8df5b496e9da9dfb2495035ab665fb7813944dbd58bf8","observation_id":"903d9b12-1304-4f2d-89a5-8e2bb6998ed8","resolution":{"observed_at":"2026-08-09T10:26:40.755096Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+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":"2026-08-09T10:26:40.732018Z","title":"Dispersive and clas- sical shock waves in Bose-Einstein condensates and gas dynamics,","venue":null,"work_id":"caf466bb-c887-4287-8364-103eebd021f1","year":2006},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.605854Z"},"links":{"citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:292099798e46b691eba8a81969f6ec135b6667875817ee8772773a0dc938890b","observation_id":"4e7d82f5-d3ba-49ce-91e0-52a7ff608fe4","resolution":{"observed_at":"2026-08-09T10:26:40.737877Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1909.05101","last_updated":"2019-09-08T16:27:57Z","snapshot_observed_at":"2026-07-06T08:20:55.549794Z","submitted_at":"2019-09-08T16:27:57Z","title":"Implosion-explosion in supernovae","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1909.05101","snapshot_observed_at":"2026-08-09T10:26:39.611075Z","title":"Implosion-explosion in supernovae,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.611075Z"},"links":{"cited_paper":"/paper/1909.05101","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:6aae53e2ab216f5552f5c748581bca211d97cb35c5914493d7be3e04747ff98d","observation_id":"cfb8d246-0287-421c-8c1d-60ca9ff3812e","resolution":{"observed_at":"2026-08-09T10:26:39.611075Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2301.01309","last_updated":"2023-01-03T19:01:05Z","snapshot_observed_at":"2026-08-10T04:08:15.990258Z","submitted_at":"2023-01-03T19:01:05Z","title":"Regular black holes from Loop Quantum Gravity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2301.01309","snapshot_observed_at":"2026-08-09T10:26:39.616573Z","title":"Regular black holes from Loop Quantum Gravity,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.616573Z"},"links":{"cited_paper":"/paper/2301.01309","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:5d0596dd53e4d7efeaf2f61c959d23868e47dd23684146d120a08a2a5dd941e0","observation_id":"63efb440-3b78-450e-b16d-dc8b78782795","resolution":{"observed_at":"2026-08-09T10:26:39.616573Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1408.7112","last_updated":"2014-08-29T19:38:44Z","snapshot_observed_at":"2026-08-02T17:41:14.458781Z","submitted_at":"2014-08-29T19:38:44Z","title":"Group Field Theory and Loop Quantum Gravity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1408.7112","snapshot_observed_at":"2026-08-09T10:26:39.622401Z","title":"Group Field Theory and Loop Quantum Grav- ity,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-09T10:26:39.622401Z"},"links":{"cited_paper":"/paper/1408.7112","citing_paper":"/paper/2502.03003"},"observation_digest":"sha256:902ec5031195141d233bfe05375fe7c6b3f40a819fe4afb61ff526070baba858","observation_id":"07aaffbb-25ae-411d-bf92-4612c2602ccf","resolution":{"observed_at":"2026-08-09T10:26:39.622401Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2502.03003","last_updated":"2025-02-05T08:55:40Z","latest_version":1,"primary_category":"gr-qc","snapshot_observed_at":"2026-08-09T10:28:45.562363Z","submitted_at":"2025-02-05T08:55:40Z","title":"Non-uniqueness of the shockwave dynamics in effective loop quantum gravity"},"reference_resolution":{"displayed":59,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":40,"verified_exact":4,"verified_fuzzy":15},"total_outbound_references":59},"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":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"thesis":"As of 10 August 2026, this Paper Citation Record lists 59 of 59 outbound references and 2 inbound Pith citation observations for arXiv:2502.03003."}