{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:WV7NRPN7WYC7TKBQAKJNWHA4CW","short_pith_number":"pith:WV7NRPN7","schema_version":"1.0","canonical_sha256":"b57ed8bdbfb605f9a8300292db1c1c15b55f86e9c87a78432e3a7e24322e3fed","source":{"kind":"arxiv","id":"2107.04949","version":2},"attestation_state":"computed","paper":{"title":"(3+1)-D viscous hydrodynamics CLVisc at finite net baryon density: identified particle spectra, anisotropic flows and flow fluctuations across BES energies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Guang-You Qin, Long-Gang Pang, Xiang-Yu Wu, Xin-Nian Wang","submitted_at":"2021-07-11T02:50:53Z","abstract_excerpt":"To study the bulk properties of the quark-gluon-plasma (QGP) produced at the beam energy scan (BES) energies at the Relativistic Heavy Ion Collider (RHIC), we extend the (3+1)-dimensional viscous hydrodynamics CLVisc to include net baryon number conservation and Israel-Stewart-like equation for baryon diffusion with the NEOS-BQS equation of state, fluctuating initial conditions from Monte-Carlo Glauber model, and the afterburner SMASH. This integrated framework is shown to provide a good description of identified particle spectra, mean transverse momenta and anisotropic flows for different cen"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2107.04949","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2021-07-11T02:50:53Z","cross_cats_sorted":["nucl-ex","nucl-th"],"title_canon_sha256":"7d688740f6c23eb335eaaf6be5a561727d4191f3b58211dee0b0a64ddc36e6b5","abstract_canon_sha256":"fbd701b5a7d1eb73889347eefe7efd04689b91e1d9b99bfdbe9c1619a068bfb8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:13:31.097572Z","signature_b64":"BvWAwvLQyKPigv6SPSMm74gUs52aS8goqqnxrPkuMQPxSQ+3X18y7o9xQafo1qlwTJg4F4MMV8jD5u5WSUcXAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b57ed8bdbfb605f9a8300292db1c1c15b55f86e9c87a78432e3a7e24322e3fed","last_reissued_at":"2026-07-05T04:13:31.097118Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:13:31.097118Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"(3+1)-D viscous hydrodynamics CLVisc at finite net baryon density: identified particle spectra, anisotropic flows and flow fluctuations across BES energies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Guang-You Qin, Long-Gang Pang, Xiang-Yu Wu, Xin-Nian Wang","submitted_at":"2021-07-11T02:50:53Z","abstract_excerpt":"To study the bulk properties of the quark-gluon-plasma (QGP) produced at the beam energy scan (BES) energies at the Relativistic Heavy Ion Collider (RHIC), we extend the (3+1)-dimensional viscous hydrodynamics CLVisc to include net baryon number conservation and Israel-Stewart-like equation for baryon diffusion with the NEOS-BQS equation of state, fluctuating initial conditions from Monte-Carlo Glauber model, and the afterburner SMASH. This integrated framework is shown to provide a good description of identified particle spectra, mean transverse momenta and anisotropic flows for different cen"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2107.04949","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2107.04949/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2107.04949","created_at":"2026-07-05T04:13:31.097176+00:00"},{"alias_kind":"arxiv_version","alias_value":"2107.04949v2","created_at":"2026-07-05T04:13:31.097176+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2107.04949","created_at":"2026-07-05T04:13:31.097176+00:00"},{"alias_kind":"pith_short_12","alias_value":"WV7NRPN7WYC7","created_at":"2026-07-05T04:13:31.097176+00:00"},{"alias_kind":"pith_short_16","alias_value":"WV7NRPN7WYC7TKBQ","created_at":"2026-07-05T04:13:31.097176+00:00"},{"alias_kind":"pith_short_8","alias_value":"WV7NRPN7","created_at":"2026-07-05T04:13:31.097176+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":12,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2604.19288","citing_title":"Geometric Bias and Centrality Dependence of Jet Quenching in High-Energy Nuclear Collisions","ref_index":72,"is_internal_anchor":true},{"citing_arxiv_id":"2606.10341","citing_title":"Global polarization of $\\Lambda$, $\\Xi^{-}$, and $\\Omega^{-}$ hyperons in Au+Au collisions at RHIC BES-II energies","ref_index":96,"is_internal_anchor":false},{"citing_arxiv_id":"2606.03552","citing_title":"$D^0$-$D_s^+$ Elliptic-Flow Splitting under Event-Shape Engineering: A Probe of Sequential Charm Hadronization","ref_index":24,"is_internal_anchor":false},{"citing_arxiv_id":"2605.21222","citing_title":"System-size dependence of the $D^0$--$D_s^+$ flow splitting from early $D_s^+$ formation at $\\sqrt{s_{NN}} = 5.36$~TeV","ref_index":35,"is_internal_anchor":false},{"citing_arxiv_id":"2605.28788","citing_title":"Energy-energy correlators inside single inclusive jets in heavy-ion collisions with CoLBT-hydro model","ref_index":78,"is_internal_anchor":false},{"citing_arxiv_id":"2512.08007","citing_title":"(3+1)D event-by-event pre-equilibrium dynamics in heavy-ion collisions","ref_index":58,"is_internal_anchor":false},{"citing_arxiv_id":"2605.21222","citing_title":"System-size dependence of the $D^0$--$D_s^+$ flow splitting from early $D_s^+$ formation at $\\sqrt{s_{NN}} = 5.36$~TeV","ref_index":35,"is_internal_anchor":false},{"citing_arxiv_id":"2605.17511","citing_title":"Study of jet-induced hydro response in high-energy heavy-ion collisions with a flow-matching generative model","ref_index":68,"is_internal_anchor":false},{"citing_arxiv_id":"2510.25837","citing_title":"Deriving a parton shower for jet thermalization in QCD plasmas","ref_index":25,"is_internal_anchor":false},{"citing_arxiv_id":"2512.07169","citing_title":"Bayesian Inference of Heavy-Quark Dissipation and Jet Transport Parameters from D-Meson observables in heavy-ion collisions at the LHC energies","ref_index":87,"is_internal_anchor":false},{"citing_arxiv_id":"2604.22352","citing_title":"Four-dimensional QCD equation of state from a quasi-parton model with physics-informed neural networks","ref_index":15,"is_internal_anchor":false},{"citing_arxiv_id":"2604.19288","citing_title":"Geometric Bias and Centrality Dependence of Jet Quenching in High-Energy Nuclear Collisions","ref_index":72,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WV7NRPN7WYC7TKBQAKJNWHA4CW","json":"https://pith.science/pith/WV7NRPN7WYC7TKBQAKJNWHA4CW.json","graph_json":"https://pith.science/api/pith-number/WV7NRPN7WYC7TKBQAKJNWHA4CW/graph.json","events_json":"https://pith.science/api/pith-number/WV7NRPN7WYC7TKBQAKJNWHA4CW/events.json","paper":"https://pith.science/paper/WV7NRPN7"},"agent_actions":{"view_html":"https://pith.science/pith/WV7NRPN7WYC7TKBQAKJNWHA4CW","download_json":"https://pith.science/pith/WV7NRPN7WYC7TKBQAKJNWHA4CW.json","view_paper":"https://pith.science/paper/WV7NRPN7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2107.04949&json=true","fetch_graph":"https://pith.science/api/pith-number/WV7NRPN7WYC7TKBQAKJNWHA4CW/graph.json","fetch_events":"https://pith.science/api/pith-number/WV7NRPN7WYC7TKBQAKJNWHA4CW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WV7NRPN7WYC7TKBQAKJNWHA4CW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WV7NRPN7WYC7TKBQAKJNWHA4CW/action/storage_attestation","attest_author":"https://pith.science/pith/WV7NRPN7WYC7TKBQAKJNWHA4CW/action/author_attestation","sign_citation":"https://pith.science/pith/WV7NRPN7WYC7TKBQAKJNWHA4CW/action/citation_signature","submit_replication":"https://pith.science/pith/WV7NRPN7WYC7TKBQAKJNWHA4CW/action/replication_record"}},"created_at":"2026-07-05T04:13:31.097176+00:00","updated_at":"2026-07-05T04:13:31.097176+00:00"}