{"as_of":"2026-08-05T00:26:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:3e860a5faa982e0df991bb52608d86b88959f7314d354c494a0246d1a9df0e14","coverage":[{"denominator":56,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":56,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-04T23:42:41.110678Z","state":"measured"},{"denominator":76,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":76,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-04T06:34:03.388597+00:00","state":"measured"},{"denominator":20,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":20,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-04T19:18:13.636593Z","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":"2026-07-04T09:39:47.075970Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2509.06428","snapshot_observed_at":"2026-08-04T19:18:13.636593Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne−Ne collisions at √sNN = 5.36 TeV,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2509.09376","last_updated":"2026-07-10T13:11:43Z","snapshot_observed_at":"2026-08-04T19:18:10.410284Z","submitted_at":"2025-09-11T11:51:40Z","title":"Scaling approach to rigid and soft nuclear deformation through flow fluctuations in high-energy nuclear collisions","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-04T19:18:13.636593Z"},"links":{"cited_paper":"/paper/2509.06428","citing_paper":"/paper/2509.09376"},"observation_digest":"sha256:3befd32412ab8694ca26467be22b677671c72a197b249b06ea98c3f0ebc9ce97","observation_id":"ce063ab0-727c-4e99-bf8b-3aecd0fd0fec","resolution":{"observed_at":"2026-08-04T19:18:13.636593Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"cited_work":{"arxiv_id":"2509.06428","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2509.06428","snapshot_observed_at":"2026-07-04T09:39:47.075970Z","title":"Acharyaet al.(ALICE Collaboration), (2025), see also related results from ATLAS and CMS Collaborations, arXiv:2509.06428 [nucl-ex]","venue":null,"work_id":"cc0a9a77-b79e-4184-b7d5-2c468070af0e","year":2025},"citing_paper":{"arxiv_id":"2509.09736","last_updated":"2026-04-18T19:49:30Z","snapshot_observed_at":"2026-07-06T22:28:57.048003Z","submitted_at":"2025-09-10T17:02:35Z","title":"Data-driven method to estimate contamination from light ion beam transmutation at colliders","version":3},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-05-18T17:23:49.439017Z"},"links":{"cited_paper":"/paper/2509.06428","citing_paper":"/paper/2509.09736"},"observation_digest":"sha256:c8473ad311d81c9142d1913a14adab2542f501270ea6c2b3d51063e505105ca2","observation_id":"e4553f31-75e4-4594-9137-dce09ac7db24","resolution":{"observed_at":"2026-05-18T17:26:40.575864Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"cited_work":{"arxiv_id":"2509.06428","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2509.06428","snapshot_observed_at":"2026-07-04T09:39:47.075970Z","title":"Acharyaet al.(ALICE Collaboration), (2025), see also related results from ATLAS and CMS Collaborations, arXiv:2509.06428 [nucl-ex]","venue":null,"work_id":"cc0a9a77-b79e-4184-b7d5-2c468070af0e","year":2025},"citing_paper":{"arxiv_id":"2511.04605","last_updated":"2026-04-20T07:45:17Z","snapshot_observed_at":"2026-08-02T05:41:33.918154Z","submitted_at":"2025-11-06T17:58:03Z","title":"The size of the quark-gluon plasma in ultracentral collisions: impact of initial density fluctuations on the average transverse momentum","version":2},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-05-17T23:40:20.719124Z"},"links":{"cited_paper":"/paper/2509.06428","citing_paper":"/paper/2511.04605"},"observation_digest":"sha256:1f2af3339c78fab7aed99f56f88551e40973bd6613f4c2f782582c959fdf08bd","observation_id":"e423cebc-b418-442e-8c05-5f7ffc8ba462","resolution":{"observed_at":"2026-05-17T23:40:31.069378Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"cited_work":{"arxiv_id":"2509.06428","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2509.06428","snapshot_observed_at":"2026-07-04T09:39:47.075970Z","title":"Acharyaet al.(ALICE Collaboration), (2025), see also related results from ATLAS and CMS Collaborations, arXiv:2509.06428 [nucl-ex]","venue":null,"work_id":"cc0a9a77-b79e-4184-b7d5-2c468070af0e","year":2025},"citing_paper":{"arxiv_id":"2512.24079","last_updated":"2026-05-09T15:46:48Z","snapshot_observed_at":"2026-07-06T22:40:23.205898Z","submitted_at":"2025-12-30T08:41:39Z","title":"Initial spin fluctuations as a probe of cluster spin structure in $^{16}\\mathrm{O}$ and $^{20}\\mathrm{Ne}$ nuclei","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-05-16T19:28:57.211973Z"},"links":{"cited_paper":"/paper/2509.06428","citing_paper":"/paper/2512.24079"},"observation_digest":"sha256:d50ac098b7641aea61ddd23c43df03fb05ba23e0b76d909d2493a5f1ebec967f","observation_id":"2272375e-c91d-428b-9b38-c2beb362da31","resolution":{"observed_at":"2026-05-16T19:31:13.206351Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2509.06428","snapshot_observed_at":"2026-08-03T02:42:49.244762Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.09890","last_updated":"2026-03-03T14:37:36Z","snapshot_observed_at":"2026-08-03T02:42:43.924752Z","submitted_at":"2026-02-10T15:28:27Z","title":"Imaging two-body correlations in atomic nuclei via low- and high-energy processes","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-03T02:42:49.244762Z"},"links":{"cited_paper":"/paper/2509.06428","citing_paper":"/paper/2602.09890"},"observation_digest":"sha256:ae57e9ec4547642dcc7b9fa8e6f9d564f81d17d496ae5d92b91c526f0b1e50bb","observation_id":"f23d699e-4342-42be-af6c-30b9604f2bb7","resolution":{"observed_at":"2026-08-03T02:42:49.244762Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"cited_work":{"arxiv_id":"2509.06428","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2509.06428","snapshot_observed_at":"2026-07-04T09:39:47.075970Z","title":"Acharyaet al.(ALICE Collaboration), (2025), see also related results from ATLAS and CMS Collaborations, arXiv:2509.06428 [nucl-ex]","venue":null,"work_id":"cc0a9a77-b79e-4184-b7d5-2c468070af0e","year":2025},"citing_paper":{"arxiv_id":"2604.05307","last_updated":"2026-04-07T01:23:13Z","snapshot_observed_at":"2026-07-06T22:54:04.491386Z","submitted_at":"2026-04-07T01:23:13Z","title":"Equilibrated fraction of QCD matter in high-energy oxygen--oxygen collisions","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-05-10T19:51:54.994133Z"},"links":{"cited_paper":"/paper/2509.06428","citing_paper":"/paper/2604.05307"},"observation_digest":"sha256:460e64500102514faefa0928e0423d116306098a4fec7d34a2c87041e4611bd6","observation_id":"f39e897b-a519-4c5d-8657-ccf7d393247d","resolution":{"observed_at":"2026-05-10T22:25:52.339341Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"cited_work":{"arxiv_id":"2509.06428","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2509.06428","snapshot_observed_at":"2026-07-04T09:39:47.075970Z","title":"Acharyaet al.(ALICE Collaboration), (2025), see also related results from ATLAS and CMS Collaborations, arXiv:2509.06428 [nucl-ex]","venue":null,"work_id":"cc0a9a77-b79e-4184-b7d5-2c468070af0e","year":2025},"citing_paper":{"arxiv_id":"2604.05512","last_updated":"2026-04-07T07:06:50Z","snapshot_observed_at":"2026-07-06T22:54:12.531121Z","submitted_at":"2026-04-07T07:06:50Z","title":"Measurement of charged-particle production in $\\sqrt{s_\\text{NN}}=9.62$ TeV proton-oxygen collisions as a probe of cosmic-ray air showers with the ATLAS detector","version":1},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-05-10T19:20:21.397820Z"},"links":{"cited_paper":"/paper/2509.06428","citing_paper":"/paper/2604.05512"},"observation_digest":"sha256:7fdb020456c8fd23816650dc3126a53fee217bda2751f1010191946a3e6623cd","observation_id":"d46c2545-fa96-452c-9c82-19be0bca19d6","resolution":{"observed_at":"2026-05-10T23:05:50.698306Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"cited_work":{"arxiv_id":"2509.06428","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2509.06428","snapshot_observed_at":"2026-07-04T09:39:47.075970Z","title":"Acharyaet al.(ALICE Collaboration), (2025), see also related results from ATLAS and CMS Collaborations, arXiv:2509.06428 [nucl-ex]","venue":null,"work_id":"cc0a9a77-b79e-4184-b7d5-2c468070af0e","year":2025},"citing_paper":{"arxiv_id":"2604.07184","last_updated":"2026-04-08T15:12:28Z","snapshot_observed_at":"2026-08-01T22:49:21.877202Z","submitted_at":"2026-04-08T15:12:28Z","title":"Recent ALICE results from light-ion collision systems","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-05-10T17:48:55.977207Z"},"links":{"cited_paper":"/paper/2509.06428","citing_paper":"/paper/2604.07184"},"observation_digest":"sha256:18ecb105098f821c9a45ad06a82c6029ce4a60be1608c314020dfd5861fca594","observation_id":"8e529ebf-39a4-4631-9ede-03f911856908","resolution":{"observed_at":"2026-05-11T06:05:57.082454Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"cited_work":{"arxiv_id":"2509.06428","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2509.06428","snapshot_observed_at":"2026-07-04T09:39:47.075970Z","title":"Acharyaet al.(ALICE Collaboration), (2025), see also related results from ATLAS and CMS Collaborations, arXiv:2509.06428 [nucl-ex]","venue":null,"work_id":"cc0a9a77-b79e-4184-b7d5-2c468070af0e","year":2025},"citing_paper":{"arxiv_id":"2604.18010","last_updated":"2026-04-20T09:31:59Z","snapshot_observed_at":"2026-07-06T23:04:59.629739Z","submitted_at":"2026-04-20T09:31:59Z","title":"Jet Quenching in the Smallest Hadronic Collision Systems","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-05-10T04:38:11.257460Z"},"links":{"cited_paper":"/paper/2509.06428","citing_paper":"/paper/2604.18010"},"observation_digest":"sha256:f57cbe03fcaf3c42b17af4edcc9b3115f059ae3f77e8f2a7bc2d8c7c0a2284c8","observation_id":"8766c5b7-8bf1-4153-8287-84cc903e21bb","resolution":{"observed_at":"2026-05-10T12:10:22.789898Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"cited_work":{"arxiv_id":"2509.06428","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2509.06428","snapshot_observed_at":"2026-07-04T09:39:47.075970Z","title":"Acharyaet al.(ALICE Collaboration), (2025), see also related results from ATLAS and CMS Collaborations, arXiv:2509.06428 [nucl-ex]","venue":null,"work_id":"cc0a9a77-b79e-4184-b7d5-2c468070af0e","year":2025},"citing_paper":{"arxiv_id":"2605.00866","last_updated":"2026-04-22T12:15:36Z","snapshot_observed_at":"2026-08-02T08:00:31.902739Z","submitted_at":"2026-04-22T12:15:36Z","title":"Nuclear geometry driven symmetry plane correlations in OO and Ne--Ne collisions at the Large Hadron Collider","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-05-10T00:18:36.123166Z"},"links":{"cited_paper":"/paper/2509.06428","citing_paper":"/paper/2605.00866"},"observation_digest":"sha256:daf25849b7e3dc6a46ebb48922279c86b43a79602b65d6172742ad8eeae12eaf","observation_id":"6f127fb5-e3db-4c7f-bd37-4389656627b1","resolution":{"observed_at":"2026-05-10T00:19:46.683572Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"cited_work":{"arxiv_id":"2509.06428","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2509.06428","snapshot_observed_at":"2026-07-04T09:39:47.075970Z","title":"Acharyaet al.(ALICE Collaboration), (2025), see also related results from ATLAS and CMS Collaborations, arXiv:2509.06428 [nucl-ex]","venue":null,"work_id":"cc0a9a77-b79e-4184-b7d5-2c468070af0e","year":2025},"citing_paper":{"arxiv_id":"2606.02285","last_updated":"2026-06-01T14:07:59Z","snapshot_observed_at":"2026-07-06T23:42:44.661608Z","submitted_at":"2026-06-01T14:07:59Z","title":"Centrality dependence of charged-hadron pseudorapidity distributions in oxygen-oxygen collisions at $\\sqrt{s_\\mathrm{NN}}$ = 5.36 TeV","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-06-28T11:47:34.735266Z"},"links":{"cited_paper":"/paper/2509.06428","citing_paper":"/paper/2606.02285"},"observation_digest":"sha256:e9f11eb710de7f6a4d6a76b405e951d6abe3dbf7903c796f4b3b82627ee06109","observation_id":"0041bdea-e786-4be5-b960-23c4955728b7","resolution":{"observed_at":"2026-07-02T01:36:25.344948Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"cited_work":{"arxiv_id":"2509.06428","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2509.06428","snapshot_observed_at":"2026-07-04T09:39:47.075970Z","title":"Acharyaet al.(ALICE Collaboration), (2025), see also related results from ATLAS and CMS Collaborations, arXiv:2509.06428 [nucl-ex]","venue":null,"work_id":"cc0a9a77-b79e-4184-b7d5-2c468070af0e","year":2025},"citing_paper":{"arxiv_id":"2606.03993","last_updated":"2026-06-02T17:59:59Z","snapshot_observed_at":"2026-07-06T23:44:09.692359Z","submitted_at":"2026-06-02T17:59:59Z","title":"Yoctosecond imaging of the ground state of $^{129}$Xe at the Large Hadron Collider","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-06-28T07:49:11.283514Z"},"links":{"cited_paper":"/paper/2509.06428","citing_paper":"/paper/2606.03993"},"observation_digest":"sha256:16e0063c23d9e311076875e296e62f197d60c0c501791ff3f0023ff9df1ef1af","observation_id":"ce49ff15-f4e6-4e30-9ec5-13f6deff35d3","resolution":{"observed_at":"2026-07-02T05:56:41.009029Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"cited_work":{"arxiv_id":"2509.06428","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2509.06428","snapshot_observed_at":"2026-07-04T09:39:47.075970Z","title":"Acharyaet al.(ALICE Collaboration), (2025), see also related results from ATLAS and CMS Collaborations, arXiv:2509.06428 [nucl-ex]","venue":null,"work_id":"cc0a9a77-b79e-4184-b7d5-2c468070af0e","year":2025},"citing_paper":{"arxiv_id":"2606.10258","last_updated":"2026-06-08T23:57:35Z","snapshot_observed_at":"2026-08-02T09:34:04.270644Z","submitted_at":"2026-06-08T23:57:35Z","title":"Nonflow Subtraction Beyond Two-Particle Correlations","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-06-27T14:22:32.690392Z"},"links":{"cited_paper":"/paper/2509.06428","citing_paper":"/paper/2606.10258"},"observation_digest":"sha256:704313ac696a3567b6b12d78e326957f93343a4ce72ad9c738447d6ae5ae1521","observation_id":"0ddeb2bb-27c8-4ef6-ab19-98bd91ad0a4a","resolution":{"observed_at":"2026-07-03T03:57:38.459304Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"cited_work":{"arxiv_id":"2509.06428","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2509.06428","snapshot_observed_at":"2026-07-04T09:39:47.075970Z","title":"Acharyaet al.(ALICE Collaboration), (2025), see also related results from ATLAS and CMS Collaborations, arXiv:2509.06428 [nucl-ex]","venue":null,"work_id":"cc0a9a77-b79e-4184-b7d5-2c468070af0e","year":2025},"citing_paper":{"arxiv_id":"2606.20257","last_updated":"2026-06-18T14:06:08Z","snapshot_observed_at":"2026-07-06T23:55:25.144457Z","submitted_at":"2026-06-18T14:06:08Z","title":"Measurements of charged-particle pseudorapidity and transverse momentum distributions in O+O and Ne+Ne collisions at $\\sqrt{s_{_\\text{NN}}} = 5.36$ TeV with the ATLAS detector","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-06-26T14:50:25.803149Z"},"links":{"cited_paper":"/paper/2509.06428","citing_paper":"/paper/2606.20257"},"observation_digest":"sha256:1d58e0b9d68a1a1254e3b23628e57ad459988d6e0552f37f938c89b92c9fe1c6","observation_id":"e22646da-d558-4f3e-90d6-29e5e89abf82","resolution":{"observed_at":"2026-07-04T06:09:37.060150Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"cited_work":{"arxiv_id":"2509.06428","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2509.06428","snapshot_observed_at":"2026-07-04T09:39:47.075970Z","title":"Acharyaet al.(ALICE Collaboration), (2025), see also related results from ATLAS and CMS Collaborations, arXiv:2509.06428 [nucl-ex]","venue":null,"work_id":"cc0a9a77-b79e-4184-b7d5-2c468070af0e","year":2025},"citing_paper":{"arxiv_id":"2606.20463","last_updated":"2026-06-18T16:45:40Z","snapshot_observed_at":"2026-07-06T23:55:38.979306Z","submitted_at":"2026-06-18T16:45:40Z","title":"Observation of centrality-dependent dijet transverse momentum imbalance in O+O and Ne+Ne collisions at $\\sqrt{s_{NN}}$ = 5.36 TeV with the ATLAS detector","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-06-26T14:36:12.131066Z"},"links":{"cited_paper":"/paper/2509.06428","citing_paper":"/paper/2606.20463"},"observation_digest":"sha256:fe0000596c794a4c211cd5df3c466aa9e79c60cf4d32aa7035c71f40db35a2b0","observation_id":"9296597a-f1ae-42eb-92ad-6385711f12e2","resolution":{"observed_at":"2026-07-04T06:19:38.358119Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"cited_work":{"arxiv_id":"2509.06428","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2509.06428","snapshot_observed_at":"2026-07-04T09:39:47.075970Z","title":"Acharyaet al.(ALICE Collaboration), (2025), see also related results from ATLAS and CMS Collaborations, arXiv:2509.06428 [nucl-ex]","venue":null,"work_id":"cc0a9a77-b79e-4184-b7d5-2c468070af0e","year":2025},"citing_paper":{"arxiv_id":"2606.21094","last_updated":"2026-06-19T04:49:36Z","snapshot_observed_at":"2026-08-02T07:43:24.661176Z","submitted_at":"2026-06-19T04:49:36Z","title":"Analysis note: Long-range near-side correlation in $e^+e^-$ with $W$-boson-pair events at 183-209 GeV with ALEPH archived data","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-06-26T13:07:43.600064Z"},"links":{"cited_paper":"/paper/2509.06428","citing_paper":"/paper/2606.21094"},"observation_digest":"sha256:d9247d071192c4dddbcec2407c8c5fe4230179b56a3e1abaa1136978cedff233","observation_id":"838b0565-352f-404e-8b41-f258a71e8b86","resolution":{"observed_at":"2026-07-04T07:39:39.226921Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"cited_work":{"arxiv_id":"2509.06428","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2509.06428","snapshot_observed_at":"2026-07-04T09:39:47.075970Z","title":"Acharyaet al.(ALICE Collaboration), (2025), see also related results from ATLAS and CMS Collaborations, arXiv:2509.06428 [nucl-ex]","venue":null,"work_id":"cc0a9a77-b79e-4184-b7d5-2c468070af0e","year":2025},"citing_paper":{"arxiv_id":"2606.22558","last_updated":"2026-06-21T15:33:04Z","snapshot_observed_at":"2026-07-06T23:57:23.574340Z","submitted_at":"2026-06-21T15:33:04Z","title":"Event-by-event fluctuations of elliptic flow in ultrarelativistic O+O collisions","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-06-26T09:38:37.556805Z"},"links":{"cited_paper":"/paper/2509.06428","citing_paper":"/paper/2606.22558"},"observation_digest":"sha256:ade20a1cafa8da63d337bb235cce6e31cb288c8d4f548d99c02c862cf5c9c3ce","observation_id":"754855c8-47a0-4e85-a1be-fa1cf7ddde24","resolution":{"observed_at":"2026-07-04T09:39:47.077438Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2509.06428","snapshot_observed_at":"2026-08-02T03:53:07.290070Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and NeNe collisions at √sNN =5.36 TeV","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.13758","last_updated":"2026-07-15T12:20:12Z","snapshot_observed_at":"2026-08-02T20:05:30.138864Z","submitted_at":"2026-07-15T12:20:12Z","title":"Evidence for sequential $\\Upsilon$(nS) suppression in light ion collisions","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-02T03:53:07.290070Z"},"links":{"cited_paper":"/paper/2509.06428","citing_paper":"/paper/2607.13758"},"observation_digest":"sha256:277b114a5c73d7efb20d7da49b7dd8d0b271e071a5072c6b77f83cfdba1ad4e3","observation_id":"6f59c7ef-499e-4e0c-a262-0abf37ebeabc","resolution":{"observed_at":"2026-08-02T03:53:07.290070Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2509.06428","snapshot_observed_at":"2026-08-01T20:55:37.582724Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.16485","last_updated":"2026-07-17T20:20:13Z","snapshot_observed_at":"2026-08-03T12:28:59.600302Z","submitted_at":"2026-07-17T20:20:13Z","title":"Wounded parton scaling of multiplicities in ultra-relativistic light- and heavy-ion collisions","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-01T20:55:37.582724Z"},"links":{"cited_paper":"/paper/2509.06428","citing_paper":"/paper/2607.16485"},"observation_digest":"sha256:5575a278436fc2a7578627c756e7a934c1c85b28e93fd9e4b1abed35d0e2256b","observation_id":"7d7ccd33-609d-4233-b3bf-9c5dc8ced6fe","resolution":{"observed_at":"2026-08-01T20:55:37.582724Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2509.06428","snapshot_observed_at":"2026-07-30T21:59:25.592670Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.26758","last_updated":"2026-07-29T10:56:38Z","snapshot_observed_at":"2026-08-02T17:41:12.202563Z","submitted_at":"2026-07-29T10:56:38Z","title":"Constraining $\\alpha$-cluster compactness in $^{16}\\rm O$ and $^{20}\\rm Ne$ at TeV energies using azimuthal anisotropy","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-07-30T21:59:25.592670Z"},"links":{"cited_paper":"/paper/2509.06428","citing_paper":"/paper/2607.26758"},"observation_digest":"sha256:ef3e8f02782163de4e0839520cba42aa5225826d42aae41235495a6848da3a2e","observation_id":"b0a6997b-2cf4-4553-8225-ad5ee7ad9860","resolution":{"observed_at":"2026-07-30T21:59:25.592670Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2509.06428/citation-record","integrity":"/paper/2509.06428/integrity","json":"/paper/2509.06428/citation-record.json","paper":"/paper/2509.06428"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"1105.3865","last_updated":"2017-09-28T06:53:23Z","snapshot_observed_at":"2026-07-06T02:27:59.654777Z","submitted_at":"2011-05-19T13:28:11Z","title":"Higher harmonic anisotropic flow measurements of charged particles in Pb-Pb collisions at 2.76 TeV","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1105.3865","snapshot_observed_at":"2026-08-04T23:42:36.668404Z","title":"Anisotropy as a signature of transverse collective flow","venue":null,"work_id":null,"year":1992},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:36.668404Z"},"links":{"cited_paper":"/paper/1105.3865","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:504e6605c34147f43e9649139312017c2501786dd4da97762249b99421835a5f","observation_id":"02fb595f-9867-4619-b9dc-066ea5f8c169","resolution":{"observed_at":"2026-08-04T23:42:36.668404Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1301.2826","last_updated":"2013-01-13T21:37:02Z","snapshot_observed_at":"2026-08-04T03:17:21.674143Z","submitted_at":"2013-01-13T21:37:02Z","title":"Collective flow and viscosity in relativistic heavy-ion collisions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1301.2826","snapshot_observed_at":"2026-08-04T23:42:36.740184Z","title":"Collective flow and viscosity in relativistic heavy-ion collisions","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:36.740184Z"},"links":{"cited_paper":"/paper/1301.2826","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:83414ae14045f42dd7d7034521669d9432abf6e0a2498c1badd0473e9b302c22","observation_id":"6ca94e47-7211-4396-8bfd-698063bf616e","resolution":{"observed_at":"2026-08-04T23:42:36.740184Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1605.03954","last_updated":"2016-08-19T17:41:49Z","snapshot_observed_at":"2026-08-03T18:29:21.691415Z","submitted_at":"2016-05-12T19:55:33Z","title":"Applying Bayesian parameter estimation to relativistic heavy-ion collisions: simultaneous characterization of the initial state and quark-gluon plasma medium","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1605.03954","snapshot_observed_at":"2026-08-04T23:42:36.815010Z","title":"Applying Bayesian parameter estimation to relativistic heavy-ion collisions: simultaneous characterization of the initial state and quark-gluon plasma medium","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:36.815010Z"},"links":{"cited_paper":"/paper/1605.03954","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:d26087d3e555866cef89458e291899c9186c409cca5ffce15a371111266e4a3a","observation_id":"3584335c-8755-496f-ab8d-7e28852e98ce","resolution":{"observed_at":"2026-08-04T23:42:36.815010Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2010.15130","last_updated":"2021-04-30T08:53:13Z","snapshot_observed_at":"2026-07-06T10:09:30.922063Z","submitted_at":"2020-10-28T18:00:02Z","title":"A transverse momentum differential global analysis of Heavy Ion Collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.15130","snapshot_observed_at":"2026-08-04T23:42:36.903713Z","title":"Transverse Momentum Differential Global Analysis of Heavy-Ion Collisions","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:36.903713Z"},"links":{"cited_paper":"/paper/2010.15130","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:992681488ab0e24c464747251055be6c2967b39e89749415dd85f4b220d8d0f8","observation_id":"314047be-5ed0-4541-8ee0-fe0f88a20377","resolution":{"observed_at":"2026-08-04T23:42:36.903713Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0405231","last_updated":"2005-03-17T01:44:41Z","snapshot_observed_at":"2026-08-04T23:17:46.226034Z","submitted_at":"2004-05-26T02:04:08Z","title":"Viscosity in Strongly Interacting Quantum Field Theories from Black Hole Physics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0405231","snapshot_observed_at":"2026-08-04T23:42:37.006515Z","title":"Viscosity in strongly interacting quantum field theories from black hole physics","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:37.006515Z"},"links":{"cited_paper":"/paper/hep-th/0405231","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:9f3888b4cd86ec59e879ba1c746b8d4affbe956ff54899acf5d920745d65928a","observation_id":"fd73658f-c6ec-4a35-b52f-a47b8d06204f","resolution":{"observed_at":"2026-08-04T23:42:37.006515Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1812.06772","last_updated":"2019-02-25T14:30:16Z","snapshot_observed_at":"2026-07-06T07:21:37.707171Z","submitted_at":"2018-12-17T14:01:17Z","title":"Future physics opportunities for high-density QCD at the LHC with heavy-ion and proton beams","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1812.06772","snapshot_observed_at":"2026-08-04T23:42:37.105027Z","title":"Report from Working Group 5: Future physics opportunities for high-density QCD at the LHC with heavy-ion and proton beams","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:37.105027Z"},"links":{"cited_paper":"/paper/1812.06772","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:cb26f7e6af3358eade562d173d215b0235d5d8611c5a0d9b01d154366cf9d75b","observation_id":"143771da-bc3f-44d8-97c6-4c43b2db3943","resolution":{"observed_at":"2026-08-04T23:42:37.105027Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.00670","last_updated":"2017-03-02T08:56:53Z","snapshot_observed_at":"2026-07-06T05:32:01.622092Z","submitted_at":"2017-03-02T08:56:53Z","title":"Collective flow and hydrodynamics in large and small systems at the LHC","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.00670","snapshot_observed_at":"2026-08-04T23:42:37.178539Z","title":"Collective flow and hydrodynamics in large and small systems at the LHC","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:37.178539Z"},"links":{"cited_paper":"/paper/1703.00670","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:112c96f7040a2a4c08f90da45278db8ab86278b46c84062f7525664dc11d7af5","observation_id":"32950832-ce07-4141-a586-f907ddf241a6","resolution":{"observed_at":"2026-08-04T23:42:37.178539Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1801.03477","last_updated":"2018-05-10T15:35:58Z","snapshot_observed_at":"2026-07-06T06:18:04.975530Z","submitted_at":"2018-01-10T17:49:51Z","title":"Small System Collectivity in Relativistic Hadron and Nuclear Collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1801.03477","snapshot_observed_at":"2026-08-04T23:42:37.250136Z","title":"Small System Collectivity in Relativistic Hadronic and Nuclear Collisions","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:37.250136Z"},"links":{"cited_paper":"/paper/1801.03477","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:7f38bf2154d14f9f3c3faa409216e429aa987a6cd9735defcf0f5886ddb0f136","observation_id":"8db6b6ff-bbb7-4c56-953e-5f29e3d58674","resolution":{"observed_at":"2026-08-04T23:42:37.250136Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.02672","last_updated":"2024-12-03T18:45:35Z","snapshot_observed_at":"2026-07-06T20:01:05.921085Z","submitted_at":"2024-12-03T18:45:35Z","title":"Soft QCD Physics at the LHC: highlights and opportunities","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.02672","snapshot_observed_at":"2026-08-04T23:42:37.354331Z","title":"Soft qcd physics at the lhc: Highlights and opportunities","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:37.354331Z"},"links":{"cited_paper":"/paper/2412.02672","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:2245b9b42644ffaccf3d920fae798f94421589b5c527e8fb1a95e61c03394249","observation_id":"72058b0d-14dd-49ca-8f42-a6a117ccaa82","resolution":{"observed_at":"2026-08-04T23:42:37.354331Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.07484","last_updated":"2024-07-10T09:15:37Z","snapshot_observed_at":"2026-07-06T18:44:07.924943Z","submitted_at":"2024-07-10T09:15:37Z","title":"A Decade of Collectivity in Small Systems","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.07484","snapshot_observed_at":"2026-08-04T23:42:37.428075Z","title":"A Decade of Collectivity in Small Systems","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:37.428075Z"},"links":{"cited_paper":"/paper/2407.07484","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:ca7af50f8aebf7f3a5038fb6b85922cce8b52dc00f426bb746ee3c021e0aaf33","observation_id":"83c4b9d5-8284-490f-978d-c299d19a0b9f","resolution":{"observed_at":"2026-08-04T23:42:37.428075Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1911.00826","last_updated":"2020-09-21T03:39:25Z","snapshot_observed_at":"2026-07-06T08:34:18.782838Z","submitted_at":"2019-11-03T04:21:13Z","title":"Probing the partonic degrees of freedom in high multiplicity p-Pb collisions at $\\sqrt{s_{NN}}=$ 5.02 TeV","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1911.00826","snapshot_observed_at":"2026-08-04T23:42:37.500695Z","title":"Probing the Partonic Degrees of Freedom in High-Multiplicity p–Pb collisions at √sNN = 5.02 TeV","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:37.500695Z"},"links":{"cited_paper":"/paper/1911.00826","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:09433fe30b14c77b26d122cbbfb6ff32d58cceb493e045832585874a70b65219","observation_id":"b6456a38-c4f1-4859-8523-3efdfb2d5961","resolution":{"observed_at":"2026-08-04T23:42:37.500695Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1112.0915","last_updated":"2012-01-28T16:33:10Z","snapshot_observed_at":"2026-07-06T02:38:48.305771Z","submitted_at":"2011-12-05T13:05:04Z","title":"Collective flow in p-Pb and d-Pb collisions at TeV energies","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1112.0915","snapshot_observed_at":"2026-08-04T23:42:37.565461Z","title":"Collective flow in p-Pb and d-Pb collisions at TeV energies","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:37.565461Z"},"links":{"cited_paper":"/paper/1112.0915","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:4090c6c0d9d73285eecd9cbd50d4d9d9deccbc0694a7b63ca06e9760885aa121","observation_id":"84892830-4b83-4996-b094-88bd4e685da5","resolution":{"observed_at":"2026-08-04T23:42:37.565461Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1705.03177","last_updated":"2017-05-09T05:02:41Z","snapshot_observed_at":"2026-07-06T05:41:50.872484Z","submitted_at":"2017-05-09T05:02:41Z","title":"Imprints of fluctuating proton shapes on flow in proton-lead collisions at the LHC","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1705.03177","snapshot_observed_at":"2026-08-04T23:42:37.634115Z","title":"Imprints of fluctuating proton shapes on flow in proton-lead collisions at the LHC","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:37.634115Z"},"links":{"cited_paper":"/paper/1705.03177","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:a8a2be62d60aa989b261af259c270f988337ce383d7d9f3c9cb4905610d54b0b","observation_id":"fa4cb2f8-d881-453a-83c1-154ea215c5d1","resolution":{"observed_at":"2026-08-04T23:42:37.634115Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1701.07145","last_updated":"2017-01-25T02:33:28Z","snapshot_observed_at":"2026-08-03T16:05:39.266513Z","submitted_at":"2017-01-25T02:33:28Z","title":"One fluid to rule them all: viscous hydrodynamic description of event-by-event central p+p, p+Pb and Pb+Pb collisions at $\\sqrt{s}=5.02$ TeV","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1701.07145","snapshot_observed_at":"2026-08-04T23:42:37.699298Z","title":"One fluid to rule them all: viscous hydrodynamic description of event-by-event central p+p, p+Pb and Pb+Pb collisions at √s=5.02 TeV","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:37.699298Z"},"links":{"cited_paper":"/paper/1701.07145","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:36f5dcc1a7d9f34e2696202614c0de62dcaca550bda5665cfae7f640902436d8","observation_id":"2a98cb71-1203-40ec-8e3c-786c7aff4e7c","resolution":{"observed_at":"2026-08-04T23:42:37.699298Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1801.00271","last_updated":"2018-04-21T09:24:33Z","snapshot_observed_at":"2026-07-06T06:16:43.550293Z","submitted_at":"2017-12-31T11:57:20Z","title":"Hydrodynamic Collectivity in Proton--Proton Collisions at 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1801.00271","snapshot_observed_at":"2026-08-04T23:42:37.772646Z","title":"Hydrodynamic collectivity in proton–proton collisions at 13 TeV","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:37.772646Z"},"links":{"cited_paper":"/paper/1801.00271","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:416e5cd5b8025f07c3b10e0ec1c24207a20310ba68ceaf5f673b31898ed57a06","observation_id":"4ade5a40-161e-440b-8d2c-acb6afabd55b","resolution":{"observed_at":"2026-08-04T23:42:37.772646Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2001.06742","last_updated":"2020-01-19T00:19:55Z","snapshot_observed_at":"2026-08-01T16:31:30.883531Z","submitted_at":"2020-01-19T00:19:55Z","title":"Searching for small droplets of hydrodynamic fluid in proton--proton collisions at the LHC","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2001.06742","snapshot_observed_at":"2026-08-04T23:42:37.837051Z","title":"Searching for small droplets of hydrodynamic fluid in proton–proton collisions at the LHC","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:37.837051Z"},"links":{"cited_paper":"/paper/2001.06742","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:f31600733ca2c3776014db4b0c3e6c52c18dbef339cba439c53321ec937638bc","observation_id":"95f5ec5f-a5da-4cf5-9f5c-64512515fa9d","resolution":{"observed_at":"2026-08-04T23:42:37.837051Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1502.05572","last_updated":"2016-01-07T00:00:56Z","snapshot_observed_at":"2026-07-06T04:09:40.816055Z","submitted_at":"2015-02-19T13:52:24Z","title":"Anisotropic parton escape is the dominant source of azimuthal anisotropy in transport models","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1502.05572","snapshot_observed_at":"2026-08-04T23:42:37.906788Z","title":"Anisotropic parton escape is the dominant source of azimuthal anisotropy in transport models","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:37.906788Z"},"links":{"cited_paper":"/paper/1502.05572","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:380b8e1080b3a64d24f895a6c05d1fcefb4e153f8f9fbbdd65ad343e4977b22c","observation_id":"00f613f7-dc76-4fce-be84-8f861e593c5e","resolution":{"observed_at":"2026-08-04T23:42:37.906788Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.02072","last_updated":"2018-07-06T12:09:27Z","snapshot_observed_at":"2026-07-06T06:26:49.130171Z","submitted_at":"2018-03-06T09:33:14Z","title":"Nearly isentropic flow at sizeable $\\eta/s$","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.02072","snapshot_observed_at":"2026-08-04T23:42:37.965969Z","title":"Nearly isentropic flow at sizeableη/s","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:37.965969Z"},"links":{"cited_paper":"/paper/1803.02072","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:e4c9e22fe56d3475fc6d261c3663ea5396abb70d7aa180f644ce7042893989b6","observation_id":"5cafa55f-5d0c-4ae4-b7de-3e3a9f03dc4a","resolution":{"observed_at":"2026-08-04T23:42:37.965969Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2401.00913","last_updated":"2024-01-01T04:30:52Z","snapshot_observed_at":"2026-07-06T17:10:36.020497Z","submitted_at":"2024-01-01T04:30:52Z","title":"Exploring the partonic collectivity in small systems at the LHC","version":1},"cited_work":{"arxiv_id":"2401.00913","doi":null,"metadata_source":"pith","pith_arxiv_id":"2401.00913","snapshot_observed_at":"2026-08-04T23:42:42.814515Z","title":"Exploring the partonic collectivity in small systems at the LHC","venue":"nucl-th","work_id":"76fad7ef-87bb-40e8-9e88-54d78fcf0e4d","year":2024},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:38.100492Z"},"links":{"cited_paper":"/paper/2401.00913","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:f83f09318ea015a89daf34d8e9d6985a67dec55bd2cfc92c9ba1487fd07607d6","observation_id":"839b2960-7876-44f2-bb8e-496628625b4e","resolution":{"observed_at":"2026-08-04T23:42:42.817850Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2005.14682","last_updated":"2020-05-29T17:17:24Z","snapshot_observed_at":"2026-07-06T09:24:27.338337Z","submitted_at":"2020-05-29T17:17:24Z","title":"Running the gamut of high energy nuclear collisions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2005.14682","snapshot_observed_at":"2026-08-04T23:42:38.168388Z","title":"Running the gamut of high energy nuclear collisions","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:38.168388Z"},"links":{"cited_paper":"/paper/2005.14682","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:0d1eea75ccc442d5c80861c366139d8d6041091b7f9853fcdd4cc17b6fa68e59","observation_id":"041f56bd-e8a6-49be-be81-118ecd566de2","resolution":{"observed_at":"2026-08-04T23:42:38.168388Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2202.01998","last_updated":"2022-02-04T07:00:56Z","snapshot_observed_at":"2026-08-04T20:30:28.929846Z","submitted_at":"2022-02-04T07:00:56Z","title":"Bayesian inference of the fluctuating proton shape","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2202.01998","snapshot_observed_at":"2026-08-04T23:42:38.228465Z","title":"Bayesian inference of the fluctuating proton shape","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:38.228465Z"},"links":{"cited_paper":"/paper/2202.01998","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:7d184f3cfaec4519182240c2e7b83e89e27216ad0c2dc7993726069c27bb1f83","observation_id":"3a84ccf8-0a70-44fb-84cc-0959bfdbdea8","resolution":{"observed_at":"2026-08-04T23:42:38.228465Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1702.02507","last_updated":"2017-05-02T05:24:23Z","snapshot_observed_at":"2026-07-06T05:29:18.341886Z","submitted_at":"2017-02-08T16:42:41Z","title":"Nuclear cluster structure effect on elliptic and triangular flows in heavy-ion collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1702.02507","snapshot_observed_at":"2026-08-04T23:42:38.340924Z","title":"Nuclear cluster structure effect on elliptic and triangular flows in heavy-ion collisions","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:38.340924Z"},"links":{"cited_paper":"/paper/1702.02507","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:d28f305c980becb2683b98a0e84768924cb9284a0a36918de9abb39e87cdfb4b","observation_id":"a1437cc1-38f6-484f-b9dc-46bb74ae5a13","resolution":{"observed_at":"2026-08-04T23:42:38.340924Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.05995","last_updated":"2024-02-08T19:00:00Z","snapshot_observed_at":"2026-07-06T17:27:41.385431Z","submitted_at":"2024-02-08T19:00:00Z","title":"The unexpected uses of a bowling pin: exploiting $^{20}$Ne isotopes for precision characterizations of collectivity in small systems","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.05995","snapshot_observed_at":"2026-08-04T23:42:38.409825Z","title":"Exploiting 20Ne Isotopes for Precision Characterizations of Collectivity in Small Systems","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:38.409825Z"},"links":{"cited_paper":"/paper/2402.05995","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:26b02c4793b1a7238cbd5c7ed871d7a30a42c6f979f38eb7253c762c5fe4c5a1","observation_id":"977fc8d0-3dc0-4ebf-b88a-22d99182d961","resolution":{"observed_at":"2026-08-04T23:42:38.409825Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2010.10003","last_updated":"2020-10-20T04:30:03Z","snapshot_observed_at":"2026-07-06T10:06:02.860601Z","submitted_at":"2020-10-20T04:30:03Z","title":"Signatures of $\\alpha$ clustering in $^{16}$O by using a multiphase transport model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.10003","snapshot_observed_at":"2026-08-04T23:42:38.480862Z","title":"Signatures ofα-clustering in16O by using a multiphase transport model","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:38.480862Z"},"links":{"cited_paper":"/paper/2010.10003","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:00df9c90f8445d09e1921377603724b8463788d5b08625d7bfa916f5b9993057","observation_id":"1138a90e-e0ba-433d-8589-4dcb1b5bc9bf","resolution":{"observed_at":"2026-08-04T23:42:38.480862Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2401.15723","last_updated":"2024-05-07T17:07:07Z","snapshot_observed_at":"2026-07-06T17:21:30.030202Z","submitted_at":"2024-01-28T18:14:23Z","title":"Exploring the compactness of $\\alpha$ cluster in $^{16}$O nuclei with relativistic $^{16}$O+$^{16}$O collisions","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.15723","snapshot_observed_at":"2026-08-04T23:42:38.544794Z","title":"Exploring the compactness ofαclusters in O16 nuclei with relativistic O16+O16 collisions","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:38.544794Z"},"links":{"cited_paper":"/paper/2401.15723","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:5a1102bcab613b4b11851a8f4963fc1abcd97a79da6bedd9b0aed3fa3876a2f2","observation_id":"20af73d0-f422-41d2-842e-ccb0342d356a","resolution":{"observed_at":"2026-08-04T23:42:38.544794Z","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":"2404.09780","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T23:42:42.561906Z","title":"Nuclear cluster structure effect in 16O+16O collisions at the top RHIC energy","venue":null,"work_id":"f0e5d5e2-ed97-4590-a406-6e4dde16b8e5","year":null},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:38.644640Z"},"links":{"citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:5ef54d7cef47eabebf5f42a0b7722eeafda1ca0d2318816521192f84c78a20de","observation_id":"b64d66a9-176e-451b-991d-bb2d9872b616","resolution":{"observed_at":"2026-08-04T23:42:42.657780Z","resolver_source":"raw_fallback","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1812.08096","last_updated":"2019-04-06T00:07:20Z","snapshot_observed_at":"2026-08-03T02:37:16.756297Z","submitted_at":"2018-12-19T17:16:54Z","title":"Exploring New Small System Geometries in Heavy Ion Collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1812.08096","snapshot_observed_at":"2026-08-04T23:42:38.714338Z","title":"Exploring New Small System Geometries in Heavy Ion Collisions","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:38.714338Z"},"links":{"cited_paper":"/paper/1812.08096","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:deea1cc998dea5400565a9137f15e4808b92ab111953831bdeb3194874756679","observation_id":"941f4f76-47dc-445e-b080-225ec1c5d2b5","resolution":{"observed_at":"2026-08-04T23:42:38.714338Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2103.03345","last_updated":"2021-03-04T21:47:36Z","snapshot_observed_at":"2026-07-06T10:47:00.751179Z","submitted_at":"2021-03-04T21:47:36Z","title":"$^{16}\\mathrm{O}^{16}\\mathrm{O}$ at RHIC and the LHC comparing $\\alpha$ clustering vs substructure","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2103.03345","snapshot_observed_at":"2026-08-04T23:42:38.780212Z","title":"16O 16O collisions at energies available at the BNL Relativistic Heavy Ion Collider and at the CERN Large Hadron Collider comparingαclustering versus substructure","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:38.780212Z"},"links":{"cited_paper":"/paper/2103.03345","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:a2ff09d844d8b47a2d5c9b5885b9d58f1fce08d53187e57a46bf24ed52eeba9f","observation_id":"f4aa5e63-05b2-4129-9df0-d834a46ba2c1","resolution":{"observed_at":"2026-08-04T23:42:38.780212Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2304.10879","last_updated":"2023-09-15T06:09:22Z","snapshot_observed_at":"2026-07-06T15:18:18.845864Z","submitted_at":"2023-04-21T10:46:17Z","title":"Effects of clustered nuclear geometry on the anisotropic flow in O-O collisions at the LHC within a multiphase transport model framework","version":2},"cited_work":{"arxiv_id":"2304.10879","doi":null,"metadata_source":"pith","pith_arxiv_id":"2304.10879","snapshot_observed_at":"2026-08-04T23:42:42.264199Z","title":"Effects of clustered nuclear geometry on the anisotropic flow in O-O collisions at the LHC within a multiphase transport model framework","venue":"hep-ph","work_id":"d4f82ef6-4343-4faa-8bf8-35313f0dd329","year":2023},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:38.908990Z"},"links":{"cited_paper":"/paper/2304.10879","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:01ccff089284fcd6f3d58b2284f41ad24e5f1f0ea4bcae730321e04b52e1108e","observation_id":"9aa42323-027e-454b-8810-8e2068f697ff","resolution":{"observed_at":"2026-08-04T23:42:42.364573Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2209.11042","last_updated":"2024-12-13T13:28:29Z","snapshot_observed_at":"2026-07-06T13:55:12.797796Z","submitted_at":"2022-09-22T14:37:51Z","title":"Imaging the initial condition of heavy-ion collisions and nuclear structure across the nuclide chart","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2209.11042","snapshot_observed_at":"2026-08-04T23:42:39.006729Z","title":"Imaging the initial condition of heavy-ion collisions and nuclear structure across the nuclide chart","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:39.006729Z"},"links":{"cited_paper":"/paper/2209.11042","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:b711ed0cc75a2af2f8b392c6b912fad4adba1e318e279671abe5dda773f11c99","observation_id":"14b08127-0c2f-4606-ab49-62c5135da0dc","resolution":{"observed_at":"2026-08-04T23:42:39.006729Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.01454","last_updated":"2025-07-02T08:13:02Z","snapshot_observed_at":"2026-07-06T21:50:55.182461Z","submitted_at":"2025-07-02T08:13:02Z","title":"Nuclear Physics Confronts Relativistic Collisions Of Isobars","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.01454","snapshot_observed_at":"2026-08-04T23:42:39.098471Z","title":"Nuclear Physics Confronts Relativistic Collisions Of Isobars","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:39.098471Z"},"links":{"cited_paper":"/paper/2507.01454","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:7d702eb806d53558abfc5a259414c9e21df5e6ca8cf066d6c3f17762948623d1","observation_id":"bf25a700-05ad-4c45-a5a5-620d315d00f1","resolution":{"observed_at":"2026-08-04T23:42:39.098471Z","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":"2026-08-04T23:42:43.031348Z","title":"Ring and P","venue":null,"work_id":"2e6535c9-21cf-4009-9f08-5e084bcb5e22","year":1980},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:39.175981Z"},"links":{"citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:b36ee7e5759d9bfa076c61001fcd065323f2382c92c3e9d022717a88b1b79c36","observation_id":"f3742862-485d-41c3-9441-a3eca018ec7d","resolution":{"observed_at":"2026-08-04T23:42:43.034804Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+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":"2026-08-04T23:42:39.236324Z","title":"Lattice Effective Field Theory Simulations of Nuclei","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:39.236324Z"},"links":{"citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:1c36728a346d15ff7102ac51f73dd9009f653b8270449e76dcf5743337aa96cf","observation_id":"3ba1ae53-34b2-4e25-9a47-6738d28ff301","resolution":{"observed_at":"2026-08-04T23:42:39.236324Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2110.15737","last_updated":"2022-01-27T17:15:55Z","snapshot_observed_at":"2026-07-06T12:03:28.439864Z","submitted_at":"2021-10-29T12:21:04Z","title":"Multi-reference many-body perturbation theory for nuclei I -- Novel PGCM-PT formalism","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2110.15737","snapshot_observed_at":"2026-08-04T23:42:39.329023Z","title":"Multi-reference many-body perturbation theory for nuclei: I. Novel PGCM-PT formalism","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:39.329023Z"},"links":{"cited_paper":"/paper/2110.15737","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:7cac8158eec1c0c6e62977c21608a5f7a08e9b21a0129e1bfacbd5a24f1aca5a","observation_id":"ff0e3e61-ff22-4cd5-9bd5-c38d1e5d7dc6","resolution":{"observed_at":"2026-08-04T23:42:39.329023Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2111.00797","last_updated":"2022-01-27T17:18:18Z","snapshot_observed_at":"2026-07-06T12:04:06.076820Z","submitted_at":"2021-11-01T09:49:17Z","title":"Multi-reference many-body perturbation theory for nuclei II -- Ab initio study of neon isotopes via PGCM and IM-NCSM calculations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2111.00797","snapshot_observed_at":"2026-08-04T23:42:39.424456Z","title":"Multi-reference many-body perturbation theory for nuclei: II. Ab initio study of neon isotopes via PGCM and IM-NCSM calculations","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:39.424456Z"},"links":{"cited_paper":"/paper/2111.00797","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:fcffed943d60fb2eea856e558b5eb10d3b4b4b1187830ef84d29efc3fc57911f","observation_id":"083cc934-7ae8-4b71-9602-0d585f0ccd37","resolution":{"observed_at":"2026-08-04T23:42:39.424456Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1606.04717","last_updated":"2016-06-15T10:46:23Z","snapshot_observed_at":"2026-07-06T05:00:01.744710Z","submitted_at":"2016-06-15T10:46:23Z","title":"Time-dependent density-functional description of nuclear dynamics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1606.04717","snapshot_observed_at":"2026-08-04T23:42:39.496990Z","title":"Time-dependent density-functional description of nuclear dynamics","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:39.496990Z"},"links":{"cited_paper":"/paper/1606.04717","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:28bae77106bc446aa1099df86f41f82d18fd2d7d03b32ea4da656b24e359a064","observation_id":"b7f66d26-74e1-4ad9-a103-4b662493ca0d","resolution":{"observed_at":"2026-08-04T23:42:39.496990Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1505.07812","last_updated":"2015-11-07T23:35:26Z","snapshot_observed_at":"2026-07-06T04:19:15.167225Z","submitted_at":"2015-05-28T19:24:22Z","title":"Azimuthal anisotropy in U+U and Au+Au collisions at RHIC","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1505.07812","snapshot_observed_at":"2026-08-04T23:42:39.573599Z","title":"Azimuthal anisotropy in U+U and Au+Au collisions at RHIC","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:39.573599Z"},"links":{"cited_paper":"/paper/1505.07812","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:ea6b4e94ad58cefa291a7222be08d55da58a48f58cb27605e455ea7e68aaf799","observation_id":"faa38c93-afa6-4c83-b696-a321a3fc7d09","resolution":{"observed_at":"2026-08-04T23:42:39.573599Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2003.06747","last_updated":"2020-03-15T03:40:18Z","snapshot_observed_at":"2026-07-06T09:04:46.527250Z","submitted_at":"2020-03-15T03:40:18Z","title":"Collision system size scan of collective flows in relativistic heavy-ion collisions","version":1},"cited_work":{"arxiv_id":"2003.06747","doi":null,"metadata_source":"pith","pith_arxiv_id":"2003.06747","snapshot_observed_at":"2026-08-04T23:42:41.858331Z","title":"Collision system size scan of collective flows in relativistic heavy-ion collisions","venue":"nucl-th","work_id":"40b4667a-ca15-49fc-b3b6-ea8dfcb38540","year":2020},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:39.648114Z"},"links":{"cited_paper":"/paper/2003.06747","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:d52e3b1dc8b4ab5c93ac57d0cd17c09101eda38647873b7f9017d34d12ba8ee7","observation_id":"53f9acde-9f5d-4f27-a089-76b0a4addf33","resolution":{"observed_at":"2026-08-04T23:42:41.925297Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1312.3572","last_updated":"2013-12-20T12:52:41Z","snapshot_observed_at":"2026-07-06T03:30:43.486957Z","submitted_at":"2013-12-12T18:04:34Z","title":"Generic framework for anisotropic flow analyses with multi-particle azimuthal correlations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1312.3572","snapshot_observed_at":"2026-08-04T23:42:39.805567Z","title":"Generic framework for anisotropic flow analyses with multiparticle azimuthal correlations","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:39.805567Z"},"links":{"cited_paper":"/paper/1312.3572","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:db1a78603c5cd70d43e7306e855c93b7f4a657f767aca41e9f39797723c47480","observation_id":"f7deda96-1757-4e00-9a31-72666fa4d150","resolution":{"observed_at":"2026-08-04T23:42:39.805567Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2005.07974","last_updated":"2020-05-16T12:40:30Z","snapshot_observed_at":"2026-07-06T09:20:52.610549Z","submitted_at":"2020-05-16T12:40:30Z","title":"Generic algorithm for multi-particle cumulants of azimuthal correlations in high energy nucleus collisions","version":1},"cited_work":{"arxiv_id":"2005.07974","doi":null,"metadata_source":"pith","pith_arxiv_id":"2005.07974","snapshot_observed_at":"2026-08-04T23:42:41.736773Z","title":"Generic algorithm for multi-particle cumulants of azimuthal correlations in high energy nucleus collisions","venue":"nucl-th","work_id":"2ed16aa7-502f-482b-8244-f8b1b8ad1dd9","year":2020},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:39.867118Z"},"links":{"cited_paper":"/paper/2005.07974","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:263933f93a098c67c6ced90e129f5a56afae343e1219dc6512d59dfc90835a08","observation_id":"620ae360-1398-430e-9d86-3764de3584e2","resolution":{"observed_at":"2026-08-04T23:42:41.806078Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1503.06986","last_updated":"2015-03-24T11:12:31Z","snapshot_observed_at":"2026-07-06T04:12:55.794960Z","submitted_at":"2015-03-24T11:12:31Z","title":"Hadronic \"flow\" in p--Pb collisions at the Large Hadron Collider?","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1503.06986","snapshot_observed_at":"2026-08-04T23:42:39.942772Z","title":"Investigation of possible hadronic flow in√sNN =5.02 TeV p–Pb collisions","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:39.942772Z"},"links":{"cited_paper":"/paper/1503.06986","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:a983e75de3105462f0c96b0bde4b26e26c2cc1b71b597ae06dc4e732690467c7","observation_id":"84df40d0-152a-41da-be3a-cf8df41a6144","resolution":{"observed_at":"2026-08-04T23:42:39.942772Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1710.07567","last_updated":"2017-12-31T02:02:52Z","snapshot_observed_at":"2026-07-06T06:05:13.673003Z","submitted_at":"2017-10-20T15:14:00Z","title":"Importance of non-flow in mixed-harmonic multi-particle correlations in small collision systems","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1710.07567","snapshot_observed_at":"2026-08-04T23:42:40.027561Z","title":"Importance of non-flow in mixed-harmonic multi-particle correlations in small collision systems","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:40.027561Z"},"links":{"cited_paper":"/paper/1710.07567","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:0617f17843e203e8990c460e27f7025a868ccf3507dbfbc8ee182cedd48cd353","observation_id":"1d5a07c2-95b3-413b-b93c-be4acf6cf5ea","resolution":{"observed_at":"2026-08-04T23:42:40.027561Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ex/0207026","last_updated":"2002-07-06T15:30:28Z","snapshot_observed_at":"2026-07-07T03:34:45.507395Z","submitted_at":"2002-07-06T15:30:28Z","title":"Systematic Errors: facts and fictions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ex/0207026","snapshot_observed_at":"2026-08-04T23:42:40.108030Z","title":"Systematic errors: Facts and fictions","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:40.108030Z"},"links":{"cited_paper":"/paper/hep-ex/0207026","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:7b868084e196e2cc74c5a6841e94629c6159856e03389962f06d1cb0f88cf63b","observation_id":"32e96638-5092-421e-b69c-bad67dd21467","resolution":{"observed_at":"2026-08-04T23:42:40.108030Z","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":"2026-08-04T23:42:40.224448Z","title":"Glauber predictions for oxygen and neon collisions at LHC","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:40.224448Z"},"links":{"citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:30d6c1122da47a23eb210440755b8545e91c5cc6b0049e774bf91d4a9b135d19","observation_id":"2660166e-792b-4086-b60a-db3bb7fe37eb","resolution":{"observed_at":"2026-08-04T23:42:40.224448Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2110.13153","last_updated":"2021-10-25T18:00:00Z","snapshot_observed_at":"2026-07-06T12:01:32.397293Z","submitted_at":"2021-10-25T18:00:00Z","title":"Predictions and postdictions for relativistic lead and oxygen collisions with Trajectum","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2110.13153","snapshot_observed_at":"2026-08-04T23:42:40.297472Z","title":"Predictions and postdictions for relativistic lead and oxygen collisions with the computational simulation code Trajectum","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:40.297472Z"},"links":{"cited_paper":"/paper/2110.13153","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:12ff32f5d0f68dd85d14b0f713289ede64a087f3c05dc59f46c14ef247050681","observation_id":"4e904621-ef4c-4156-93c3-ee9355a6df17","resolution":{"observed_at":"2026-08-04T23:42:40.297472Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2010.15134","last_updated":"2021-04-29T18:29:32Z","snapshot_observed_at":"2026-07-06T10:09:30.922063Z","submitted_at":"2020-10-28T18:00:03Z","title":"Bayesian analysis of heavy ion collisions with the heavy ion computational framework Trajectum","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.15134","snapshot_observed_at":"2026-08-04T23:42:40.359617Z","title":"Bayesian analysis of heavy ion collisions with the heavy ion computational framework Trajectum","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:40.359617Z"},"links":{"cited_paper":"/paper/2010.15134","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:c14cc2e8abefeec95612885ab373d2e595b855263c77cf7721180e933c81100a","observation_id":"b21111dd-e439-4034-8e4a-8ef6db3b9265","resolution":{"observed_at":"2026-08-04T23:42:40.359617Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2502.05138","last_updated":"2025-02-07T18:14:24Z","snapshot_observed_at":"2026-07-06T20:33:01.960703Z","submitted_at":"2025-02-07T18:14:24Z","title":"Collision energy dependence in heavy ion collisions from nonlinear QCD evolution","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2502.05138","snapshot_observed_at":"2026-08-04T23:42:40.421354Z","title":"Collision-Energy Dependence in Heavy-Ion Collisions from Nonlinear QCD Evolution","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:40.421354Z"},"links":{"cited_paper":"/paper/2502.05138","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:28d956604dd500eec0d2465e417619c8c9b7f2150e768089aeb2a560f04db351","observation_id":"4bb55d01-a330-4567-a46b-5c7596519234","resolution":{"observed_at":"2026-08-04T23:42:40.421354Z","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":"2026-08-04T23:42:40.496401Z","title":"Bayesian analysis of (3+1)D relativistic nuclear dynamics with the RHIC beam energy scan data","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:40.496401Z"},"links":{"citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:0efc74db65267c3b8c3af03fc5229435b64cdccd2e4988530cbe16c388d40683","observation_id":"dc485911-c6a2-42cb-889b-61709f720a40","resolution":{"observed_at":"2026-08-04T23:42:40.496401Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2102.08158","last_updated":"2021-02-16T13:58:16Z","snapshot_observed_at":"2026-07-06T10:41:50.330204Z","submitted_at":"2021-02-16T13:58:16Z","title":"Accessing the shape of atomic nuclei with relativistic collisions of isobars","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2102.08158","snapshot_observed_at":"2026-08-04T23:42:40.606581Z","title":"Accessing the shape of atomic nuclei with relativistic collisions of isobars","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:40.606581Z"},"links":{"cited_paper":"/paper/2102.08158","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:01e36d1b64b9bd9124a46c9fc302e5d09bce3aef9094d5d8f17a756cdd357a82","observation_id":"38d70e70-28b8-4d0d-90e0-86c0f996ad1d","resolution":{"observed_at":"2026-08-04T23:42:40.606581Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1603.04349","last_updated":"2016-07-18T14:27:32Z","snapshot_observed_at":"2026-07-06T04:49:25.894963Z","submitted_at":"2016-03-14T17:11:33Z","title":"Evidence of strong proton shape fluctuations from incoherent diffraction","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1603.04349","snapshot_observed_at":"2026-08-04T23:42:40.708627Z","title":"Evidence of strong proton shape fluctuations from incoherent diffraction","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:40.708627Z"},"links":{"cited_paper":"/paper/1603.04349","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:de7d84e14ae5aedc8e8c58a88497b055ceb7be1802fca759e153727ed8932137","observation_id":"ba810657-15d4-4585-9ad8-6ae6112e665a","resolution":{"observed_at":"2026-08-04T23:42:40.708627Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1607.01711","last_updated":"2016-08-30T18:16:25Z","snapshot_observed_at":"2026-07-06T05:02:37.459715Z","submitted_at":"2016-07-06T17:21:05Z","title":"Revealing proton shape fluctuations with incoherent diffraction at high energy","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1607.01711","snapshot_observed_at":"2026-08-04T23:42:40.772662Z","title":"Revealing proton shape fluctuations with incoherent diffraction at high energy","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:40.772662Z"},"links":{"cited_paper":"/paper/1607.01711","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:8d5764ce7541320ed9878fde7a45a0095ba65325938b1403b0c0d1b8cbe96709","observation_id":"9dfda158-4d45-47df-a452-00d439c9ce26","resolution":{"observed_at":"2026-08-04T23:42:40.772662Z","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":"2026-08-04T23:42:43.020287Z","title":"Investigating the gluonic structure of nuclei via J/ψscattering","venue":null,"work_id":"b6e12ed2-5e49-4ff8-986d-9328b6505bb3","year":2010},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:40.854377Z"},"links":{"citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:029ff7d990e9cf09d85e9b8e209fba6336db065d4b3765de68c51c64297ccd48","observation_id":"e62e7e87-d3a5-41d1-8ddb-3158f84ce711","resolution":{"observed_at":"2026-08-04T23:42:43.023919Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1206.6805","last_updated":"2012-06-28T19:36:54Z","snapshot_observed_at":"2026-07-06T02:50:53.242072Z","submitted_at":"2012-06-28T19:36:54Z","title":"Event-by-event gluon multiplicity, energy density and eccentricities at RHIC and LHC","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1206.6805","snapshot_observed_at":"2026-08-04T23:42:40.893493Z","title":"Event-by-event gluon multiplicity, energy density, and eccentricities in ultrarelativistic heavy-ion collisions","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:40.893493Z"},"links":{"cited_paper":"/paper/1206.6805","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:43cff263f0dd10e5e0bd4fd2796011d45054dbfce1e382ba1aa02ea1565a4d63","observation_id":"dbb74236-71d0-49fa-8b98-3d1ae142f1f2","resolution":{"observed_at":"2026-08-04T23:42:40.893493Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2111.02908","last_updated":"2021-11-04T14:30:29Z","snapshot_observed_at":"2026-07-31T09:50:25.380878Z","submitted_at":"2021-11-04T14:30:29Z","title":"Constraining the nucleon size with relativistic nuclear collisions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2111.02908","snapshot_observed_at":"2026-08-04T23:42:40.997453Z","title":"Constraining the Nucleon Size with Relativistic Nuclear Collisions","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:40.997453Z"},"links":{"cited_paper":"/paper/2111.02908","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:84a9e09f1f0640dd41380288a085ec402a690df1f5f9e33ceba46a336370d04b","observation_id":"a7c4cc95-5aa7-493c-8df8-c04858a8421b","resolution":{"observed_at":"2026-08-04T23:42:40.997453Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.02348","last_updated":"2024-07-08T09:04:17Z","snapshot_observed_at":"2026-07-06T17:24:57.402088Z","submitted_at":"2024-02-04T05:08:25Z","title":"System size and shape dependences of collective flow fluctuations in relativistic nuclear collisions","version":2},"cited_work":{"arxiv_id":"2402.02348","doi":null,"metadata_source":"pith","pith_arxiv_id":"2402.02348","snapshot_observed_at":"2026-08-04T23:42:41.234307Z","title":"System size and shape dependences of collective flow fluctuations in relativistic nuclear collisions","venue":"nucl-th","work_id":"7c0ecf45-4804-4214-bb82-24e480cbba39","year":2024},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:41.070256Z"},"links":{"cited_paper":"/paper/2402.02348","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:6b9553afc50d582171bbed594716a7e7153ce77d74c1505a8408e3b410c6783c","observation_id":"4dd16d74-6625-4056-8728-28aefccb9561","resolution":{"observed_at":"2026-08-04T23:42:41.279920Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-04T06:34:03.388597+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2404.08385","last_updated":"2025-02-14T06:06:59Z","snapshot_observed_at":"2026-07-06T17:59:17.149142Z","submitted_at":"2024-04-12T10:41:23Z","title":"$Ab$-$initio$ nucleon-nucleon correlations and their impact on high energy $^{16}$O+$^{16}$O collisions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2404.08385","snapshot_observed_at":"2026-08-04T23:42:41.110678Z","title":"Ab-initio nucleon-nucleon correlations and their impact on high energy 16O+16O collisions","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV","version":1},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-04T23:42:41.110678Z"},"links":{"cited_paper":"/paper/2404.08385","citing_paper":"/paper/2509.06428"},"observation_digest":"sha256:a880cb74cf835bb27b89892a1d87b0d2065e4b3e9d9da7814fa3786582fe2bb8","observation_id":"b4e15e48-a160-4372-81d4-825d2a08164b","resolution":{"observed_at":"2026-08-04T23:42:41.110678Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2509.06428","last_updated":"2025-09-08T08:23:43Z","latest_version":1,"primary_category":"nucl-ex","snapshot_observed_at":"2026-08-04T23:42:34.418489Z","submitted_at":"2025-09-08T08:23:43Z","title":"Evidence of nuclear geometry-driven anisotropic flow in OO and Ne$-$Ne collisions at $\\mathbf{\\sqrt{{\\textit s}_{\\rm\\mathbf {NN}}}}$ = 5.36 TeV"},"reference_resolution":{"displayed":56,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":48,"verified_exact":6,"verified_fuzzy":2},"total_outbound_references":56},"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":"2026-08-04T06:34:03.388597+00:00","source":"crossref"},{"observed_at":"2026-08-04T06:33:57.428241+00:00","source":"retraction_watch"}],"thesis":"As of 5 August 2026, this Paper Citation Record lists 56 of 56 outbound references and 20 inbound Pith citation observations for arXiv:2509.06428."}