{"as_of":"2026-08-11T00:41:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:4a73a5f18bf905d129320520c38c85f54c0e928018d1bea06ef8da5dcb666fa7","coverage":[{"denominator":69,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":69,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-01T07:53:46.492874Z","state":"measured"},{"denominator":69,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":69,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-10T06:31:04.303077+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/2607.21321/citation-record","integrity":"/paper/2607.21321/integrity","json":"/paper/2607.21321/citation-record.json","paper":"/paper/2607.21321"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"2004.00690","last_updated":"2020-04-01T20:12:16Z","snapshot_observed_at":"2026-08-09T18:49:31.997063Z","submitted_at":"2020-04-01T20:12:16Z","title":"Transverse momentum fluctuations and their correlation with elliptic flow in nuclear collision","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2004.00690","snapshot_observed_at":"2026-08-01T07:53:37.308217Z","title":"Schenke, C","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:37.308217Z"},"links":{"cited_paper":"/paper/2004.00690","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:3117aa4a05cda26bff7824b0e798b8bd15c142c9d0125a662c76873cfa376273","observation_id":"f8d6cd78-3780-42cf-94a3-c833f4c3fb2f","resolution":{"observed_at":"2026-08-01T07:53:37.308217Z","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":"2026-08-01T07:53:37.213577Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:37.213577Z"},"links":{"citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:c0b3467ebe105bf6d08fcd50c170578212e300671d9852ee4b72e544bd7c058c","observation_id":"73036ee9-2a21-4780-8f1f-af8ea70ef3fa","resolution":{"observed_at":"2026-08-01T07:53:37.213577Z","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":"2026-08-01T07:53:37.413601Z","title":"Aad et al","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:37.413601Z"},"links":{"citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:76d5c7f63c05b4868714efc2496b8689eb1cd764956f0471b4baab67cad0c5d4","observation_id":"13448225-692e-4a3e-8505-23bc854d7fae","resolution":{"observed_at":"2026-08-01T07:53:37.413601Z","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":"2026-08-01T07:53:37.457716Z","title":"Acharya et al","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:37.457716Z"},"links":{"citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:d7e206b2801e06dc529159175366b68828a88ecb9f829127de0f0a5e5ab923ed","observation_id":"23be74d9-5668-4f14-b00e-6de3ecc93418","resolution":{"observed_at":"2026-08-01T07:53:37.457716Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.17313","last_updated":"2024-08-29T14:33:33Z","snapshot_observed_at":"2026-07-06T18:51:19.677273Z","submitted_at":"2024-07-24T14:31:54Z","title":"Probing collectivity in heavy-ion collisions with fluctuations of the $p_T$ spectrum","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.17313","snapshot_observed_at":"2026-08-01T07:53:37.620636Z","title":"Parida, R","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:37.620636Z"},"links":{"cited_paper":"/paper/2407.17313","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:72d5d9391afab80c06a302e8d1f40ebc063a392df3eab87fdaead461279baa85","observation_id":"e14705eb-e871-48f5-951c-d52a512337f6","resolution":{"observed_at":"2026-08-01T07:53:37.620636Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2506.18690","last_updated":"2025-07-21T16:03:07Z","snapshot_observed_at":"2026-08-10T21:44:38.328071Z","submitted_at":"2025-06-23T14:29:27Z","title":"Correlation between particle spectra and elliptic flow","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2506.18690","snapshot_observed_at":"2026-08-01T07:53:37.781043Z","title":"Parida, R","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:37.781043Z"},"links":{"cited_paper":"/paper/2506.18690","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:0bfdbd7b3fce778c283ba7987046c26c102b14eefced2860e7d8b8d08ab32ec6","observation_id":"e5a1eab4-d576-4d63-9edb-6c78a3e804ee","resolution":{"observed_at":"2026-08-01T07:53:37.781043Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1507.06194","last_updated":"2016-04-09T19:01:49Z","snapshot_observed_at":"2026-08-07T06:19:34.868992Z","submitted_at":"2015-07-22T14:10:36Z","title":"Event shape engineering for inclusive spectra and elliptic flow in Pb-Pb collisions at $\\sqrt{s_\\rm{NN}}=2.76$ TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1507.06194","snapshot_observed_at":"2026-08-01T07:53:37.896843Z","title":"Adam et al","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:37.896843Z"},"links":{"cited_paper":"/paper/1507.06194","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:26a83f1d1afb2e29bbe68e4b3ab3058215e2dac3738b27d758d99f5fe1bc3c2e","observation_id":"5639ef50-677c-4f85-8eb8-f11bc2eeaf8e","resolution":{"observed_at":"2026-08-01T07:53:37.896843Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2604.26731","last_updated":"2026-07-15T08:54:30Z","snapshot_observed_at":"2026-08-02T15:19:09.238158Z","submitted_at":"2026-04-29T14:33:45Z","title":"Thermal and geometric normal modes of spectral fluctuations in heavy-ion collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2604.26731","snapshot_observed_at":"2026-08-01T07:53:38.046927Z","title":"Samanta, Thermal and geometric normal modes of spectral fluctuations in heavy-ion collisions, Phys","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:38.046927Z"},"links":{"cited_paper":"/paper/2604.26731","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:fcf1be893039d86ca309d8b94708d5c342cb43b5e3078fcaa7e13750d05d2871","observation_id":"a404e46d-e24b-4302-a6cd-445da2240bb3","resolution":{"observed_at":"2026-08-01T07:53:38.046927Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/0305084","last_updated":"2003-08-04T15:02:20Z","snapshot_observed_at":"2026-07-07T06:32:53.320484Z","submitted_at":"2003-05-29T18:12:18Z","title":"Hydrodynamic description of ultrarelativistic heavy-ion collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-th/0305084","snapshot_observed_at":"2026-08-01T07:53:38.208819Z","title":null,"venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:38.208819Z"},"links":{"cited_paper":"/paper/nucl-th/0305084","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:4d96cd6fd23d0f0d58960e9a02442c48dc44785cc8bb2ced269e55234b2fb831","observation_id":"9fd075f2-a635-40dd-8386-91cc77faaab8","resolution":{"observed_at":"2026-08-01T07:53:38.208819Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0407264","last_updated":"2013-03-10T16:41:41Z","snapshot_observed_at":"2026-08-03T08:17:31.002337Z","submitted_at":"2004-07-22T04:40:42Z","title":"Topics on Hydrodynamic Model of Nucleus-Nucleus Collisions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0407264","snapshot_observed_at":"2026-08-01T07:53:38.376949Z","title":null,"venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:38.376949Z"},"links":{"cited_paper":"/paper/hep-ph/0407264","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:bce2328e4d9220a80f311bd5c36d53dd7d87871c91f5b7f100b440bd65c57aaf","observation_id":"3a776f8e-8289-403f-9e1d-e328283548c7","resolution":{"observed_at":"2026-08-01T07:53:38.376949Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1007.0368","last_updated":"2011-01-26T17:22:19Z","snapshot_observed_at":"2026-07-06T02:12:33.738387Z","submitted_at":"2010-07-02T14:11:55Z","title":"Event-by-event hydrodynamics and elliptic flow from fluctuating initial state","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1007.0368","snapshot_observed_at":"2026-08-01T07:53:38.536844Z","title":"Holopainen, H","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:38.536844Z"},"links":{"cited_paper":"/paper/1007.0368","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:1e8d4930a1f0e3b44a54fec0337c93b5f52ffaa2ae6f16884b9dd7730f5a1fca","observation_id":"5c558d85-e9b1-4097-8e08-f2c99427f76b","resolution":{"observed_at":"2026-08-01T07:53:38.536844Z","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":"2026-08-01T07:53:38.699708Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:38.699708Z"},"links":{"citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:21075169bdee43e0f60dbad1f60ece3ca3292561442fe1073aa5b75b1c77c8a8","observation_id":"54970e96-c340-423e-b332-908722d1b34c","resolution":{"observed_at":"2026-08-01T07:53:38.699708Z","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":"2026-08-10T00:14:58.825780Z","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":"2026-08-01T07:53:38.865815Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:38.865815Z"},"links":{"cited_paper":"/paper/2010.15130","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:a9c18138fe0e2a9ee60a61edd0c7cb2ac4d06cb7d057beae642a0be637a5cc01","observation_id":"c4f3d8fb-4533-4b35-9cdd-c9bdaad3aed1","resolution":{"observed_at":"2026-08-01T07:53:38.865815Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2010.03928","last_updated":"2020-10-08T12:26:16Z","snapshot_observed_at":"2026-08-07T07:05:50.345576Z","submitted_at":"2020-10-08T12:26:16Z","title":"Phenomenological constraints on the transport properties of QCD matter with data-driven model averaging","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.03928","snapshot_observed_at":"2026-08-01T07:53:38.984216Z","title":"Everett et al","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:38.984216Z"},"links":{"cited_paper":"/paper/2010.03928","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:f1d982e490e669a96c0f8a3fa501d71d4f22601cdd6b786113391d15ce3d7da8","observation_id":"6d6d8316-71c5-4b7d-bd9b-ddd284bbe43d","resolution":{"observed_at":"2026-08-01T07:53:38.984216Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-ex/0009011","last_updated":"2000-09-12T21:03:39Z","snapshot_observed_at":"2026-07-07T06:23:42.852910Z","submitted_at":"2000-09-12T21:03:39Z","title":"Elliptic flow in Au+Au collisions at sqrt(s_NN) = 130 GeV","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-ex/0009011","snapshot_observed_at":"2026-08-01T07:53:39.097767Z","title":null,"venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:39.097767Z"},"links":{"cited_paper":"/paper/nucl-ex/0009011","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:33f02c31a3ea00226940620119de3af486a520471b7edba6e29e446ab40a7046","observation_id":"0e2c11a1-3e61-46a1-80f1-983df4919294","resolution":{"observed_at":"2026-08-01T07:53:39.097767Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0706.1522","last_updated":"2007-10-26T17:04:02Z","snapshot_observed_at":"2026-08-10T11:56:27.186430Z","submitted_at":"2007-06-11T18:19:26Z","title":"Viscosity Information from Relativistic Nuclear Collisions: How Perfect is the Fluid Observed at RHIC?","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0706.1522","snapshot_observed_at":"2026-08-01T07:53:39.209806Z","title":"Romatschke and U","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:39.209806Z"},"links":{"cited_paper":"/paper/0706.1522","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:87e87aee0d75a58f9335859de6d75640cdf23479f10c8aa1862c37fce08293bf","observation_id":"bf747638-91a9-4b11-9622-e63d37611207","resolution":{"observed_at":"2026-08-01T07:53:39.209806Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/0506049","last_updated":"2006-03-08T19:39:53Z","snapshot_observed_at":"2026-07-07T06:35:34.426361Z","submitted_at":"2005-06-15T16:12:01Z","title":"Perfect Fluidity of the Quark Gluon Plasma Core as Seen through its Dissipative Hadronic Corona","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-th/0506049","snapshot_observed_at":"2026-08-01T07:53:39.231799Z","title":"Hirano and M","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:39.231799Z"},"links":{"cited_paper":"/paper/nucl-th/0506049","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:39916fb226fd462509a1afd94f297046913be31f5f5599318834ebe1c05efcb0","observation_id":"f34cfb11-094e-40ad-b710-e9411c2cae49","resolution":{"observed_at":"2026-08-01T07:53:39.231799Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0704.1270","last_updated":"2007-04-10T16:47:11Z","snapshot_observed_at":"2026-07-06T01:25:54.006471Z","submitted_at":"2007-04-10T16:47:11Z","title":"Core-Corona Separation in Ultra-Relativistic Heavy Ion Collisions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0704.1270","snapshot_observed_at":"2026-08-01T07:53:39.253820Z","title":"Werner, Core-corona separation in ultra-relativistic heavy ion collisions, Phys","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:39.253820Z"},"links":{"cited_paper":"/paper/0704.1270","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:da1c592fb263e1281f813c02044df33f0501cfe5264c176752bd777c7b8d4ce2","observation_id":"9e4a300b-723e-4e2e-89a2-872d7eb3f5f0","resolution":{"observed_at":"2026-08-01T07:53:39.253820Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.07943","last_updated":"2021-08-30T01:35:08Z","snapshot_observed_at":"2026-08-10T22:11:19.070788Z","submitted_at":"2021-08-18T02:25:55Z","title":"Interplay between core and corona components in high-energy nuclear collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.07943","snapshot_observed_at":"2026-08-01T07:53:39.340986Z","title":"Kanakubo, Y","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:39.340986Z"},"links":{"cited_paper":"/paper/2108.07943","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:e134d0708cf5b9b6f24670c7f98cfa4e84106d41e022130192abe310b78427e2","observation_id":"e1e7fab9-4889-401d-beb2-43d47d2ec800","resolution":{"observed_at":"2026-08-01T07:53:39.340986Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2409.00838","last_updated":"2025-02-10T18:27:58Z","snapshot_observed_at":"2026-07-06T19:08:57.415038Z","submitted_at":"2024-09-01T20:55:13Z","title":"Pseudorapidity distributions of charged hadrons in lead-lead collisions at $\\sqrt{s_\\mathrm{NN}}$ = 5.36 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2409.00838","snapshot_observed_at":"2026-08-01T07:53:39.409904Z","title":"Hayrapetyan et al","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:39.409904Z"},"links":{"cited_paper":"/paper/2409.00838","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:1be50cd18c833a0eb3bce10acf71c8e7c8b98de567a6bbac768f9d3c60c12217","observation_id":"da19c9b1-4732-4181-8200-1b7b10b25526","resolution":{"observed_at":"2026-08-01T07:53:39.409904Z","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":"2026-08-01T07:53:39.542189Z","title":"Cooper and G","venue":null,"work_id":null,"year":1974},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:39.542189Z"},"links":{"citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:a421367d97ec9b3ce6a0626b3cbea83f7b3a9f90e0a5c0c56cb1371d82102097","observation_id":"f67bc6f1-6124-44ae-91e5-596bd1f34cfb","resolution":{"observed_at":"2026-08-01T07:53:39.542189Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1710.09425","last_updated":"2018-07-04T19:26:49Z","snapshot_observed_at":"2026-08-10T06:38:42.986903Z","submitted_at":"2017-10-25T19:00:35Z","title":"Decoding the phase structure of QCD via particle production at high energy","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1710.09425","snapshot_observed_at":"2026-08-01T07:53:39.553559Z","title":"Andronic, P","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:39.553559Z"},"links":{"cited_paper":"/paper/1710.09425","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:48951c8804e201afd6a6916eb4b570b40114afc3f4b77afbc3b337d4a6ab8e69","observation_id":"07aa78c1-4aa5-45ff-a856-e54bf9026f53","resolution":{"observed_at":"2026-08-01T07:53:39.553559Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/0301099","last_updated":"2003-06-20T00:46:48Z","snapshot_observed_at":"2026-07-07T06:32:32.817369Z","submitted_at":"2003-01-30T20:51:04Z","title":"The Effect of Shear Viscosity on Spectra, Elliptic Flow, and HBT Radii","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-th/0301099","snapshot_observed_at":"2026-08-01T07:53:39.665183Z","title":"Teaney, The Effects of viscosity on spectra, elliptic flow, and HBT radii, Phys","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:39.665183Z"},"links":{"cited_paper":"/paper/nucl-th/0301099","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:a152c1fbc2485dd77d9e3087b77fa2b7fdfce1fa04d9e6805678f399802ff7c1","observation_id":"9e8ea1f6-f3d1-430b-8b75-e1e6365da84f","resolution":{"observed_at":"2026-08-01T07:53:39.665183Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1109.5181","last_updated":"2012-01-11T17:03:30Z","snapshot_observed_at":"2026-08-10T16:58:39.678410Z","submitted_at":"2011-09-23T20:00:05Z","title":"Bulk viscosity, particle spectra and flow in heavy-ion collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1109.5181","snapshot_observed_at":"2026-08-01T07:53:39.781622Z","title":"Dusling and T","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:39.781622Z"},"links":{"cited_paper":"/paper/1109.5181","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:8da98150d20540d78754f7a2ef93055f109c5ecbc34c37bb9b72a4430a95545a","observation_id":"df90148e-c15f-4522-8576-d68b374e4644","resolution":{"observed_at":"2026-08-01T07:53:39.781622Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1404.7850","last_updated":"2017-02-14T19:33:21Z","snapshot_observed_at":"2026-08-04T10:57:07.576556Z","submitted_at":"2014-04-30T19:53:18Z","title":"Self-consistent conversion of a viscous fluid to particles","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1404.7850","snapshot_observed_at":"2026-08-01T07:53:39.899915Z","title":"Molnar and Z","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:39.899915Z"},"links":{"cited_paper":"/paper/1404.7850","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:23a0800f4fb912de61c73f4dff712a50f0bf598e0222974a76e54e8e4f945551","observation_id":"f2c6a583-ab6b-44a6-8481-446719495b03","resolution":{"observed_at":"2026-08-01T07:53:39.899915Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1502.04066","last_updated":"2015-07-10T14:19:30Z","snapshot_observed_at":"2026-08-02T07:23:20.522589Z","submitted_at":"2015-02-13T17:38:47Z","title":"Viscous corrections to anisotropic flow and transverse momentum spectra from transport theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1502.04066","snapshot_observed_at":"2026-08-01T07:53:40.001640Z","title":"Plumari, G","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:40.001640Z"},"links":{"cited_paper":"/paper/1502.04066","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:67196d7316ed9aa69a9a6a4e33fe33d8995317aa8d9a3a7441f13fee3ea5be03","observation_id":"03bbf7d6-8dd8-43ba-b056-80f1afbad5a0","resolution":{"observed_at":"2026-08-01T07:53:40.001640Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2011.01430","last_updated":"2020-11-06T20:33:35Z","snapshot_observed_at":"2026-07-06T10:11:08.648093Z","submitted_at":"2020-11-03T02:32:56Z","title":"Multi-system Bayesian constraints on the transport coefficients of QCD matter","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2011.01430","snapshot_observed_at":"2026-08-01T07:53:40.163676Z","title":"Everett et al","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:40.163676Z"},"links":{"cited_paper":"/paper/2011.01430","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:8ee8f77aa1a2f829d1d568e0f7fe53bd3350562b1026a2806233fac7e908f41a","observation_id":"782f0381-1f8f-4fea-9c53-35407b19424e","resolution":{"observed_at":"2026-08-01T07:53:40.163676Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.15658","last_updated":"2025-09-10T14:10:51Z","snapshot_observed_at":"2026-08-06T12:18:02.862881Z","submitted_at":"2024-12-20T08:17:31Z","title":"Azimuthal anisotropies of charged particles with high transverse momentum in Pb+Pb collisions at $\\sqrt{s_{_\\text{NN}}} = 5.02$ TeV with the ATLAS detector","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.15658","snapshot_observed_at":"2026-08-01T07:53:40.332428Z","title":"Aad et al","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:40.332428Z"},"links":{"cited_paper":"/paper/2412.15658","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:78ae97ee20718ec489667fb0b9d82227e194a8a20d84ab63b281bc39a5668c1f","observation_id":"123c7cc6-f941-4809-988d-f6fe997e52d3","resolution":{"observed_at":"2026-08-01T07:53:40.332428Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2206.04587","last_updated":"2023-06-15T10:32:59Z","snapshot_observed_at":"2026-08-10T14:02:01.764070Z","submitted_at":"2022-06-09T16:09:04Z","title":"Anisotropic flow and flow fluctuations of identified hadrons in Pb$-$Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}$ = 5.02 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2206.04587","snapshot_observed_at":"2026-08-01T07:53:40.485256Z","title":"Acharya et al","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:40.485256Z"},"links":{"cited_paper":"/paper/2206.04587","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:1a36f70018e18e54914864b53555b875140e66b27b03e5aa24c9569ec34d8bf3","observation_id":"a5d4a8d2-0e07-461b-8adb-ffdb9586c0df","resolution":{"observed_at":"2026-08-01T07:53:40.485256Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1201.3158","last_updated":"2013-01-22T12:44:25Z","snapshot_observed_at":"2026-08-04T11:00:00.925071Z","submitted_at":"2012-01-16T04:46:19Z","title":"Centrality dependence of dihadron correlations and azimuthal anisotropy harmonics in PbPb collisions at sqrt(s[NN]) = 2.76 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1201.3158","snapshot_observed_at":"2026-08-01T07:53:40.624360Z","title":"Chatrchyan et al","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:40.624360Z"},"links":{"cited_paper":"/paper/1201.3158","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:3a5ca585fb149a59b5d66781325c32228d936f97205f9abeb58bc9f3441c3c3e","observation_id":"8ecc5953-1d51-4f5f-9369-4dcdd3e11c9d","resolution":{"observed_at":"2026-08-01T07:53:40.624360Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1203.3087","last_updated":"2012-07-24T22:49:57Z","snapshot_observed_at":"2026-08-10T08:50:06.072386Z","submitted_at":"2012-03-14T14:01:19Z","title":"Measurement of the azimuthal anisotropy for charged particle production in sqrt(s_NN) = 2.76 TeV lead-lead collisions with the ATLAS detector","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1203.3087","snapshot_observed_at":"2026-08-01T07:53:40.801902Z","title":"Aad et al","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:40.801902Z"},"links":{"cited_paper":"/paper/1203.3087","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:e307c87f121fdbf5bdea594c216b399ed986471d6af4ca961d1aba1042806903","observation_id":"f154007c-b5cc-4adb-b5e8-90b8f3b3ecd9","resolution":{"observed_at":"2026-08-01T07:53:40.801902Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.03951","last_updated":"2018-12-18T07:53:45Z","snapshot_observed_at":"2026-07-06T06:55:14.364480Z","submitted_at":"2018-08-12T14:37:16Z","title":"Measurement of the azimuthal anisotropy of charged particles produced in $\\sqrt{s_\\mathrm{NN}} = 5.02$ TeV Pb+Pb collisions with the ATLAS detector","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.03951","snapshot_observed_at":"2026-08-01T07:53:40.949385Z","title":"Aaboud et al","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:40.949385Z"},"links":{"cited_paper":"/paper/1808.03951","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:d1e994a4e959dfcbed514b477640b3fd21d9dd380070d9ce0aac9f24cebeeae0","observation_id":"0df9fb9c-39ca-4269-a15d-5166cde2adff","resolution":{"observed_at":"2026-08-01T07:53:40.949385Z","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":"2026-08-01T07:53:41.159145Z","title":"Adams et al","venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:41.159145Z"},"links":{"citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:25c22ef6dab1213307915816fc49dda50cef5f8d16d21b894b1029c96e17fa55","observation_id":"10b1d144-5ee8-45c6-8d23-cedfcbdcc419","resolution":{"observed_at":"2026-08-01T07:53:41.159145Z","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":"2026-08-01T07:53:41.341749Z","title":null,"venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:41.341749Z"},"links":{"citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:4a8199b0b747d164963c6b127c7b364d148715611cd5eb9885e179ddbf429959","observation_id":"8f816485-a385-4156-ae4f-43ee8b00d874","resolution":{"observed_at":"2026-08-01T07:53:41.341749Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1307.3237","last_updated":"2014-09-15T06:29:28Z","snapshot_observed_at":"2026-08-10T17:11:34.176152Z","submitted_at":"2013-07-11T19:53:50Z","title":"Long-range angular correlations of $\\rm \\pi$, K and p in p-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1307.3237","snapshot_observed_at":"2026-08-01T07:53:41.466206Z","title":null,"venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:41.466206Z"},"links":{"cited_paper":"/paper/1307.3237","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:6e63a7f1f343806916b249aab4b61d51204986bf1b35058858bc74b44e2676c3","observation_id":"ecb600a1-f81c-46e3-9768-fca1ac9aec10","resolution":{"observed_at":"2026-08-01T07:53:41.466206Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1405.4632","last_updated":"2015-07-14T15:23:53Z","snapshot_observed_at":"2026-08-02T06:32:25.808809Z","submitted_at":"2014-05-19T08:10:04Z","title":"Elliptic flow of identified hadrons in Pb-Pb collisions at $\\sqrt{s_{\\rm{NN}}}$ = 2.76 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1405.4632","snapshot_observed_at":"2026-08-01T07:53:41.585552Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:41.585552Z"},"links":{"cited_paper":"/paper/1405.4632","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:396817697471d9dfe042c5ecf3242d74a6e0ee8b95f276e65951caee61d161f4","observation_id":"d0f368b9-91bb-4dac-8424-74fc444681b4","resolution":{"observed_at":"2026-08-01T07:53:41.585552Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2107.10592","last_updated":"2022-01-13T13:57:55Z","snapshot_observed_at":"2026-08-02T20:11:46.000155Z","submitted_at":"2021-07-22T11:45:21Z","title":"Anisotropic flow of identified hadrons in Xe-Xe collisions at $\\sqrt{s_{\\rm NN}}$ = 5.44TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2107.10592","snapshot_observed_at":"2026-08-01T07:53:41.723503Z","title":"Acharya et al","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:41.723503Z"},"links":{"cited_paper":"/paper/2107.10592","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:c25f2e4146368e6d8018884281bb8552fe3e63bb5d5d4bd1738ad5869bf00274","observation_id":"c201fc12-f449-426b-a575-63bc71074812","resolution":{"observed_at":"2026-08-01T07:53:41.723503Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/0105040","last_updated":"2001-09-25T06:24:30Z","snapshot_observed_at":"2026-08-09T13:18:56.697452Z","submitted_at":"2001-05-17T15:51:55Z","title":"Flow analysis from multiparticle azimuthal correlations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-th/0105040","snapshot_observed_at":"2026-08-01T07:53:41.865826Z","title":"Borghini, P","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:41.865826Z"},"links":{"cited_paper":"/paper/nucl-th/0105040","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:b41e92ee78d37ad58ce230ae4fee4c720c52babdf5d6bd2348feeb8eb62d9785","observation_id":"36ce9fc8-94e0-488f-b2a5-1d5076669fe0","resolution":{"observed_at":"2026-08-01T07:53:41.865826Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1505.02677","last_updated":"2015-05-11T15:52:23Z","snapshot_observed_at":"2026-07-06T04:17:30.616743Z","submitted_at":"2015-05-11T15:52:23Z","title":"Event-by-event fluctuations in perturbative QCD + saturation + hydro model: pinning down QCD matter shear viscosity in ultrarelativistic heavy-ion collisions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1505.02677","snapshot_observed_at":"2026-08-01T07:53:41.983283Z","title":"Niemi, K","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:41.983283Z"},"links":{"cited_paper":"/paper/1505.02677","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:c110ad8b180fe0a2dfeebd58b72600bcd31bb53da28aab892dd9374623e718cd","observation_id":"f5f56054-b5ff-4aaa-9649-bde5a18baace","resolution":{"observed_at":"2026-08-01T07:53:41.983283Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/0506045","last_updated":"2006-07-28T14:09:26Z","snapshot_observed_at":"2026-07-07T06:35:34.426361Z","submitted_at":"2005-06-14T14:10:54Z","title":"Momentum spectra, anisotropic flow, and ideal fluids","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-th/0506045","snapshot_observed_at":"2026-08-01T07:53:42.105683Z","title":"Borghini and J.-Y","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:42.105683Z"},"links":{"cited_paper":"/paper/nucl-th/0506045","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:1c52020170c0050d6d4d291d27559ec8d59d99b032a0e8d14dfb7d8351bd1686","observation_id":"eb8cef44-ab2b-46f5-89e3-74e04c98624d","resolution":{"observed_at":"2026-08-01T07:53:42.105683Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0805.0018","last_updated":"2008-04-30T22:31:24Z","snapshot_observed_at":"2026-07-06T01:38:46.068255Z","submitted_at":"2008-04-30T22:31:24Z","title":"Importance of Granular Structure in the Initial Conditions for the Elliptic Flow","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0805.0018","snapshot_observed_at":"2026-08-01T07:53:42.246571Z","title":null,"venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:42.246571Z"},"links":{"cited_paper":"/paper/0805.0018","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:814d32cc54a138154f50545d8b7b9c9964292e93ae2f2b0ff7cff9005dc12392","observation_id":"0757fcce-0e66-4455-a54b-547c9267e9c8","resolution":{"observed_at":"2026-08-01T07:53:42.246571Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1209.6330","last_updated":"2012-09-27T18:58:31Z","snapshot_observed_at":"2026-08-06T03:22:27.348050Z","submitted_at":"2012-09-27T18:58:31Z","title":"Event-by-event anisotropic flow in heavy-ion collisions from combined Yang-Mills and viscous fluid dynamics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1209.6330","snapshot_observed_at":"2026-08-01T07:53:42.331365Z","title":null,"venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:42.331365Z"},"links":{"cited_paper":"/paper/1209.6330","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:f769eae7f1043277537b798acde686427652b6f06099147f5d03190be7b1697b","observation_id":"42982313-b5f9-427b-a6c7-6cdd49d84d11","resolution":{"observed_at":"2026-08-01T07:53:42.331365Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2010.11919","last_updated":"2021-04-15T12:09:41Z","snapshot_observed_at":"2026-07-06T10:07:22.052360Z","submitted_at":"2020-10-22T17:50:56Z","title":"Effective shear and bulk viscosities for anisotropic flow","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.11919","snapshot_observed_at":"2026-08-01T07:53:42.414064Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:42.414064Z"},"links":{"cited_paper":"/paper/2010.11919","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:77fbdcaaa023745aef549a57b56f74c8648f05d2a8f531572c22a219271be99a","observation_id":"8a4432fd-0323-441a-b106-88fe74096f73","resolution":{"observed_at":"2026-08-01T07:53:42.414064Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.08692","last_updated":"2022-07-18T15:43:18Z","snapshot_observed_at":"2026-08-05T22:17:34.587065Z","submitted_at":"2022-07-18T15:43:18Z","title":"Effective shear and bulk viscosities of the quark-gluon plasma: QCD versus heavy-ion data","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.08692","snapshot_observed_at":"2026-08-01T07:53:42.494616Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:42.494616Z"},"links":{"cited_paper":"/paper/2207.08692","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:633329098d9eed92defad3cfaab90c44f4d9eeeb3e7d7171e103cb0c2e86ae8e","observation_id":"5a84c7b6-b9c3-4850-bb46-451962d2b369","resolution":{"observed_at":"2026-08-01T07:53:42.494616Z","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":"2026-08-01T07:53:42.603096Z","title":"Huovinen, P","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:42.603096Z"},"links":{"citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:595ba6d47ee3031b78ae8decaa0848106fada3035b0ebe707d3c1269cccff94f","observation_id":"dc9cd26e-b52a-42c8-88da-fd73f50e19ee","resolution":{"observed_at":"2026-08-01T07:53:42.603096Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/0301087","last_updated":"2003-05-19T19:35:12Z","snapshot_observed_at":"2026-07-07T06:32:32.817369Z","submitted_at":"2003-01-27T16:56:55Z","title":"Hadronization in heavy ion collisions: Recombination and fragmentation of partons","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-th/0301087","snapshot_observed_at":"2026-08-01T07:53:42.742644Z","title":null,"venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:42.742644Z"},"links":{"cited_paper":"/paper/nucl-th/0301087","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:4937cabc5d5955472735b800e45b20389e5d3b133858bc8103bb93f3d9aca20e","observation_id":"740588ec-cd25-45c1-b4f3-fbdd967fd7c1","resolution":{"observed_at":"2026-08-01T07:53:42.742644Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/0302014","last_updated":"2003-09-02T18:29:05Z","snapshot_observed_at":"2026-07-07T06:32:32.817369Z","submitted_at":"2003-02-05T20:42:10Z","title":"Elliptic flow at large transverse momenta from quark coalescence","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-th/0302014","snapshot_observed_at":"2026-08-01T07:53:42.886746Z","title":"Molnar and S","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:42.886746Z"},"links":{"cited_paper":"/paper/nucl-th/0302014","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:b7833a70157da4ac51a13d13795a26f52f8c2ccd62f441b5703826afa6e9f22d","observation_id":"68b01007-ab99-4e05-b6f3-0f43c3dfdd50","resolution":{"observed_at":"2026-08-01T07:53:42.886746Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/0306027","last_updated":"2003-06-12T21:48:47Z","snapshot_observed_at":"2026-07-07T06:33:01.225231Z","submitted_at":"2003-06-05T16:46:51Z","title":"Hadron production in heavy ion collisions: Fragmentation and recombination from a dense parton phase","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-th/0306027","snapshot_observed_at":"2026-08-01T07:53:43.027893Z","title":null,"venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:43.027893Z"},"links":{"cited_paper":"/paper/nucl-th/0306027","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:1a2b1d6518887e92c0d5ebead18e46646ddc3be3870210dfaa51f63ee7551209","observation_id":"b258c3fa-979c-4f94-9f85-3324a4b59062","resolution":{"observed_at":"2026-08-01T07:53:43.027893Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/0305024","last_updated":"2003-05-10T00:05:01Z","snapshot_observed_at":"2026-07-07T06:32:53.320484Z","submitted_at":"2003-05-10T00:05:01Z","title":"Parton coalescence at RHIC","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-th/0305024","snapshot_observed_at":"2026-08-01T07:53:43.164817Z","title":"Greco, C","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:43.164817Z"},"links":{"cited_paper":"/paper/nucl-th/0305024","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:721591c1ffdac1b449371716f80ad5a28a941712fc6595e8af47205f777705e6","observation_id":"7e5691f0-1d24-4e46-a77a-0a05c96f980c","resolution":{"observed_at":"2026-08-01T07:53:43.164817Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2012.07898","last_updated":"2021-06-17T11:19:40Z","snapshot_observed_at":"2026-08-05T03:35:04.830760Z","submitted_at":"2020-12-14T19:25:27Z","title":"Fluid velocity from transverse momentum spectra","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2012.07898","snapshot_observed_at":"2026-08-01T07:53:43.306005Z","title":"Guillen and J.-Y","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:43.306005Z"},"links":{"cited_paper":"/paper/2012.07898","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:7e8c4a4de7d2fc1638302ca03d35a9e64c45d8bd702fb70fe4418a59eee5ba5f","observation_id":"e68d2f00-7053-4dd4-bb2b-da5b85a629ba","resolution":{"observed_at":"2026-08-01T07:53:43.306005Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2101.10847","last_updated":"2021-01-26T15:11:28Z","snapshot_observed_at":"2026-08-04T12:48:44.950769Z","submitted_at":"2021-01-26T15:11:28Z","title":"Soft pions and transport near the chiral critical point","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2101.10847","snapshot_observed_at":"2026-08-01T07:53:43.424239Z","title":"Grossi, A","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:43.424239Z"},"links":{"cited_paper":"/paper/2101.10847","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:f460c3fac3ac3789f8195d229a672031dbfc0857241cc3d827be21268e542fef","observation_id":"d1b8dd10-506e-4240-9d96-11195a9e8ced","resolution":{"observed_at":"2026-08-01T07:53:43.424239Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2111.03640","last_updated":"2021-11-22T23:09:04Z","snapshot_observed_at":"2026-08-08T01:07:04.404861Z","submitted_at":"2021-11-05T17:45:42Z","title":"Dynamics of the $O(4)$ critical point in QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2111.03640","snapshot_observed_at":"2026-08-01T07:53:43.535449Z","title":"Florio, E","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:43.535449Z"},"links":{"cited_paper":"/paper/2111.03640","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:0754623808304e8a7298bb37fbd0db27cde5995e6ae2d90090d227e3a36504e7","observation_id":"e9631d08-4bdb-4195-89ab-9bd174d81b67","resolution":{"observed_at":"2026-08-01T07:53:43.535449Z","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":"2026-08-01T07:53:43.662363Z","title":"Bruschke, A","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:43.662363Z"},"links":{"citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:0093744ec79c3e22c6d2e58a3db5dee4bbc04007d12fd29c5fe6ca7751570f29","observation_id":"0b51af33-53c4-4b12-a085-724e64499c9b","resolution":{"observed_at":"2026-08-01T07:53:43.662363Z","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":"2026-08-01T07:53:43.788218Z","title":"Du, Characterizing radial flow fluctuations in rela- tivistic heavy-ion collisions at top RHIC and LHC ener- gies, Phys","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:43.788218Z"},"links":{"citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:96492830b4df615c26922a2125ee0542d0a511234754d5dc03d94b4bab53e203","observation_id":"1a854e08-51a3-4f05-8722-9ba59b0321d8","resolution":{"observed_at":"2026-08-01T07:53:43.788218Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2505.19697","last_updated":"2025-05-26T08:52:05Z","snapshot_observed_at":"2026-08-10T02:28:16.946300Z","submitted_at":"2025-05-26T08:52:05Z","title":"Study of $p_\\mathrm{T}$-differential radial flow in blast-wave model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2505.19697","snapshot_observed_at":"2026-08-01T07:53:43.942971Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:43.942971Z"},"links":{"cited_paper":"/paper/2505.19697","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:f723c2c9abc793784c9794097db0883b7a8073628d7fd0d418fa8b0a2e268185","observation_id":"ff0940e4-8864-426c-85fa-e1712ad77852","resolution":{"observed_at":"2026-08-01T07:53:43.942971Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2401.06625","last_updated":"2024-11-06T22:48:52Z","snapshot_observed_at":"2026-07-06T17:14:49.296971Z","submitted_at":"2024-01-12T15:17:59Z","title":"Imaging Shapes of Atomic Nuclei in High-Energy Nuclear Collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.06625","snapshot_observed_at":"2026-08-01T07:53:44.156563Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:44.156563Z"},"links":{"cited_paper":"/paper/2401.06625","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:724747cee45f154bfbd1d3ee33e7406960c4e044b12f16a2edadc97ff92ccc03","observation_id":"85fc343c-c892-41a4-b620-7decfccb67c0","resolution":{"observed_at":"2026-08-01T07:53:44.156563Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1601.04513","last_updated":"2016-03-17T12:23:21Z","snapshot_observed_at":"2026-08-08T04:01:31.226421Z","submitted_at":"2016-01-18T13:48:45Z","title":"Transverse momentum-flow correlations in relativistic heavy-ion collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1601.04513","snapshot_observed_at":"2026-08-01T07:53:44.349805Z","title":"Bozek, Transverse-momentum–flow correlations in rel- ativistic heavy-ion collisions, Phys","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:44.349805Z"},"links":{"cited_paper":"/paper/1601.04513","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:37c792a0c30e8797f6a91afff6bd5a785893b5f75a531925f26d7256bc645a4e","observation_id":"d4e8d774-0562-4ae7-802b-a2773d9aa13e","resolution":{"observed_at":"2026-08-01T07:53:44.349805Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1702.01730","last_updated":"2017-05-24T14:43:09Z","snapshot_observed_at":"2026-08-10T07:30:43.266657Z","submitted_at":"2017-02-06T18:14:34Z","title":"Relative flow fluctuations as a probe of initial state fluctuations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1702.01730","snapshot_observed_at":"2026-08-01T07:53:44.486883Z","title":"Giacalone, J","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:44.486883Z"},"links":{"cited_paper":"/paper/1702.01730","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:a08379a933c1b9d5814344cf3b7aa108184320968c68d6b42da684bf6ecc64cf","observation_id":"0d5c26bb-c2a3-4a1d-954d-134f043c524c","resolution":{"observed_at":"2026-08-01T07:53:44.486883Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2004.01765","last_updated":"2021-02-22T15:46:43Z","snapshot_observed_at":"2026-08-08T23:33:55.349898Z","submitted_at":"2020-04-03T20:41:20Z","title":"Correlation between mean transverse momentum and anisotropic flow in heavy-ion collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2004.01765","snapshot_observed_at":"2026-08-01T07:53:44.679875Z","title":"Giacalone, F","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:44.679875Z"},"links":{"cited_paper":"/paper/2004.01765","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:4d521c0f783a908b650a454dd8f7864ddef305409a376a6c16f5851dbc293c5a","observation_id":"ef99b030-5396-4ebf-b80d-392abbe8f183","resolution":{"observed_at":"2026-08-01T07:53:44.679875Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2205.00039","last_updated":"2023-10-23T13:57:45Z","snapshot_observed_at":"2026-07-06T13:05:16.090823Z","submitted_at":"2022-04-29T18:48:13Z","title":"Correlations between flow and transverse momentum in Xe+Xe and Pb+Pb collisions at the LHC with the ATLAS detector: a probe of the heavy-ion initial state and nuclear deformation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2205.00039","snapshot_observed_at":"2026-08-01T07:53:44.846946Z","title":"Aad et al","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:44.846946Z"},"links":{"cited_paper":"/paper/2205.00039","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:468b763866fd4fce5e56e2854b3be2fc168784bccf1a6b943391d178f8326af7","observation_id":"55c274fd-b4bf-4030-a3c1-1aaf539d92dc","resolution":{"observed_at":"2026-08-01T07:53:44.846946Z","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":"2026-08-01T07:53:45.033831Z","title":null,"venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:45.033831Z"},"links":{"citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:d24351e05054619b5f6023449e7fd09a294869a71b48a1022cb7fc2b72b9883d","observation_id":"9b9f6cab-26b7-409f-a7d3-ecdd4d18c4a7","resolution":{"observed_at":"2026-08-01T07:53:45.033831Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1206.1905","last_updated":"2012-08-22T20:10:23Z","snapshot_observed_at":"2026-08-05T19:22:30.059697Z","submitted_at":"2012-06-09T04:44:41Z","title":"Non linearities in the harmonic spectrum of heavy ion collisions with ideal and viscous hydrodynamics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1206.1905","snapshot_observed_at":"2026-08-01T07:53:45.204427Z","title":"Teaney and L","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:45.204427Z"},"links":{"cited_paper":"/paper/1206.1905","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:b885863e25a7b8aed3ad24f45f9b54a383f85eb9c8bde2dd2ba22bcdcb18e645","observation_id":"070c2e6e-9c21-4ca2-92f2-c662461521a1","resolution":{"observed_at":"2026-08-01T07:53:45.204427Z","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":"2026-08-01T07:53:45.416527Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:45.416527Z"},"links":{"citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:93e14fe7762efb7c15b8ac09ca5449660dc48b7988c9e3dd8ca7e1d09c67d5da","observation_id":"c6f8da67-3341-43f7-a042-6a074ad7a1f2","resolution":{"observed_at":"2026-08-01T07:53:45.416527Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1412.4708","last_updated":"2015-06-07T23:21:15Z","snapshot_observed_at":"2026-07-06T04:03:39.564117Z","submitted_at":"2014-12-15T18:22:12Z","title":"Alternative ansatz to wounded nucleon and binary collision scaling in high-energy nuclear collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1412.4708","snapshot_observed_at":"2026-08-01T07:53:45.587042Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:45.587042Z"},"links":{"cited_paper":"/paper/1412.4708","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:e230953ceeca0b869223b59ab40521b4e20de73d0093d878efb92ab0a0a77e88","observation_id":"4a530e5b-d3ed-4009-a66d-ffb7d6d8bfad","resolution":{"observed_at":"2026-08-01T07:53:45.587042Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1512.06104","last_updated":"2016-05-30T10:19:38Z","snapshot_observed_at":"2026-07-06T04:40:25.365167Z","submitted_at":"2015-12-18T20:32:27Z","title":"Centrality dependence of the charged-particle multiplicity density at mid-rapidity in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1512.06104","snapshot_observed_at":"2026-08-01T07:53:45.857735Z","title":"Adam et al","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:45.857735Z"},"links":{"cited_paper":"/paper/1512.06104","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:d4c0bfc26041e20302665094834cf2a4381d0380a81814de0f03bf809e8e0093","observation_id":"73a7b855-34af-4992-972a-215bf49c06a7","resolution":{"observed_at":"2026-08-01T07:53:45.857735Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1004.1408","last_updated":"2010-07-20T15:59:44Z","snapshot_observed_at":"2026-07-06T02:05:50.908404Z","submitted_at":"2010-04-08T19:54:32Z","title":"3+1D hydrodynamic simulation of relativistic heavy-ion collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1004.1408","snapshot_observed_at":"2026-08-01T07:53:45.979909Z","title":"Schenke, S","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:45.979909Z"},"links":{"cited_paper":"/paper/1004.1408","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:c740299a1996831fd288f7812bdeb705526e9bb5feac8b25c6d0f32309a56318","observation_id":"39b28844-14cf-4084-a6d2-552040d4590d","resolution":{"observed_at":"2026-08-01T07:53:45.979909Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1009.3244","last_updated":"2010-10-01T19:04:52Z","snapshot_observed_at":"2026-08-05T11:36:48.705922Z","submitted_at":"2010-09-16T18:58:22Z","title":"Elliptic and triangular flow in event-by-event (3+1)D viscous hydrodynamics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1009.3244","snapshot_observed_at":"2026-08-01T07:53:46.162323Z","title":"Schenke, S","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:46.162323Z"},"links":{"cited_paper":"/paper/1009.3244","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:b95356ca2317ca25ff750dcc2525afd50ffb870ee2899b7c4f60b9b793c09dc1","observation_id":"81b9b1c3-1a3c-42a5-afa6-6fbb917fb981","resolution":{"observed_at":"2026-08-01T07:53:46.162323Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1509.06738","last_updated":"2016-04-13T12:41:57Z","snapshot_observed_at":"2026-07-06T04:30:44.067910Z","submitted_at":"2015-09-22T19:27:18Z","title":"The production of photons in relativistic heavy-ion collisions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1509.06738","snapshot_observed_at":"2026-08-01T07:53:46.337375Z","title":"Paquet, C","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:46.337375Z"},"links":{"cited_paper":"/paper/1509.06738","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:207af049a8c9f6dd0334f5c9bc25833f37128a51a7028b3901356b662953baf4","observation_id":"ddb11cc7-dde3-4db9-ac35-89dbb11c08eb","resolution":{"observed_at":"2026-08-01T07:53:46.337375Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1512.02189","last_updated":"2016-01-22T18:26:15Z","snapshot_observed_at":"2026-07-06T04:39:03.563746Z","submitted_at":"2015-12-07T19:49:33Z","title":"Hydrodynamic simulations of relativistic heavy-ion collisions with different lattice QCD calculations of the equation of state","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1512.02189","snapshot_observed_at":"2026-08-01T07:53:46.492874Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$","version":1},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-01T07:53:46.492874Z"},"links":{"cited_paper":"/paper/1512.02189","citing_paper":"/paper/2607.21321"},"observation_digest":"sha256:926572207217245d1162221670a858999e6a187cf0979dcb8fa501fdd16e5393","observation_id":"e49eacf4-c308-435d-acd6-ee50aab939db","resolution":{"observed_at":"2026-08-01T07:53:46.492874Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2607.21321","last_updated":"2026-07-23T13:46:49Z","latest_version":1,"primary_category":"nucl-th","snapshot_observed_at":"2026-08-10T03:33:59.105881Z","submitted_at":"2026-07-23T13:46:49Z","title":"Enhanced hydrodynamic predictions for $v_{02}(p_T)$"},"reference_resolution":{"displayed":69,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":69,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":69},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"thesis":"As of 11 August 2026, this Paper Citation Record lists 69 of 69 outbound references and 0 inbound Pith citation observations for arXiv:2607.21321."}