{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:2Z4GDB426L3OFHNZGI3J5TZB7Y","short_pith_number":"pith:2Z4GDB42","schema_version":"1.0","canonical_sha256":"d67861879af2f6e29db932369ecf21fe30ad26ba67fe058e2839cf8ed0120ebe","source":{"kind":"arxiv","id":"1911.08547","version":1},"attestation_state":"computed","paper":{"title":"Transport coefficients for the hot quark-gluon plasma at finite chemical potential $\\mu_B$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Elena Bratkovskaya, Olga Soloveva, Pierre Moreau","submitted_at":"2019-11-17T22:49:02Z","abstract_excerpt":"We calculate transport coefficients of the quark-gluon plasma (QGP) within the dynamical quasiparticle model (DQPM) by explicitly computing the parton interaction rates as a function of temperature $T$ and baryon chemical potential $\\mu_B$ on the basis of the DQPM couplings and partonic propagators. The latter are extracted from lattice QCD by matching the equation of state, entropy density and energy density at $\\mu_B$= 0. For baryon chemical potentials $0 \\leq \\mu_B \\leq 500 MeV$ we employ a scaling Ansatz for the effective coupling which was shown before to lead to thermodynamic consistent "},"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":"1911.08547","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-11-17T22:49:02Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"319f5120065233e426c84e93f1297903d5b9430b21570666aadcb5d1f9d97866","abstract_canon_sha256":"3a3cc22d65d97c7cd2870b183b283f77923879fe4b82825dd94951ebf5b37f9e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:57:12.914034Z","signature_b64":"r2MWMlfdwiqA5Nqr6azj7dbsGORwJlBr1ZqIm+nBEVQSMCyjQIlD0Z8hcruwWfUx/xkmYQJXQpmJKrNH32fgDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d67861879af2f6e29db932369ecf21fe30ad26ba67fe058e2839cf8ed0120ebe","last_reissued_at":"2026-07-05T00:57:12.913555Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:57:12.913555Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Transport coefficients for the hot quark-gluon plasma at finite chemical potential $\\mu_B$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Elena Bratkovskaya, Olga Soloveva, Pierre Moreau","submitted_at":"2019-11-17T22:49:02Z","abstract_excerpt":"We calculate transport coefficients of the quark-gluon plasma (QGP) within the dynamical quasiparticle model (DQPM) by explicitly computing the parton interaction rates as a function of temperature $T$ and baryon chemical potential $\\mu_B$ on the basis of the DQPM couplings and partonic propagators. The latter are extracted from lattice QCD by matching the equation of state, entropy density and energy density at $\\mu_B$= 0. For baryon chemical potentials $0 \\leq \\mu_B \\leq 500 MeV$ we employ a scaling Ansatz for the effective coupling which was shown before to lead to thermodynamic consistent "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1911.08547","kind":"arxiv","version":1},"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/1911.08547/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":"1911.08547","created_at":"2026-07-05T00:57:12.913615+00:00"},{"alias_kind":"arxiv_version","alias_value":"1911.08547v1","created_at":"2026-07-05T00:57:12.913615+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1911.08547","created_at":"2026-07-05T00:57:12.913615+00:00"},{"alias_kind":"pith_short_12","alias_value":"2Z4GDB426L3O","created_at":"2026-07-05T00:57:12.913615+00:00"},{"alias_kind":"pith_short_16","alias_value":"2Z4GDB426L3OFHNZ","created_at":"2026-07-05T00:57:12.913615+00:00"},{"alias_kind":"pith_short_8","alias_value":"2Z4GDB42","created_at":"2026-07-05T00:57:12.913615+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.13363","citing_title":"Transport coefficients of strongly interacting quark-gluon plasma including elastic and inelastic scattering within the dynamical quasiparticle model","ref_index":25,"is_internal_anchor":false},{"citing_arxiv_id":"2605.29479","citing_title":"Charmonium production at SPS and FAIR energies","ref_index":41,"is_internal_anchor":false},{"citing_arxiv_id":"2404.09767","citing_title":"Electrical conductivity of QGP with quasiparticle quarks and Gribov gluon","ref_index":58,"is_internal_anchor":false},{"citing_arxiv_id":"2605.04743","citing_title":"Chiral Magnetic Effect and Negative Magnetoresistance across the phase diagram of finite-density SU(2) gauge theory","ref_index":78,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2Z4GDB426L3OFHNZGI3J5TZB7Y","json":"https://pith.science/pith/2Z4GDB426L3OFHNZGI3J5TZB7Y.json","graph_json":"https://pith.science/api/pith-number/2Z4GDB426L3OFHNZGI3J5TZB7Y/graph.json","events_json":"https://pith.science/api/pith-number/2Z4GDB426L3OFHNZGI3J5TZB7Y/events.json","paper":"https://pith.science/paper/2Z4GDB42"},"agent_actions":{"view_html":"https://pith.science/pith/2Z4GDB426L3OFHNZGI3J5TZB7Y","download_json":"https://pith.science/pith/2Z4GDB426L3OFHNZGI3J5TZB7Y.json","view_paper":"https://pith.science/paper/2Z4GDB42","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1911.08547&json=true","fetch_graph":"https://pith.science/api/pith-number/2Z4GDB426L3OFHNZGI3J5TZB7Y/graph.json","fetch_events":"https://pith.science/api/pith-number/2Z4GDB426L3OFHNZGI3J5TZB7Y/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2Z4GDB426L3OFHNZGI3J5TZB7Y/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2Z4GDB426L3OFHNZGI3J5TZB7Y/action/storage_attestation","attest_author":"https://pith.science/pith/2Z4GDB426L3OFHNZGI3J5TZB7Y/action/author_attestation","sign_citation":"https://pith.science/pith/2Z4GDB426L3OFHNZGI3J5TZB7Y/action/citation_signature","submit_replication":"https://pith.science/pith/2Z4GDB426L3OFHNZGI3J5TZB7Y/action/replication_record"}},"created_at":"2026-07-05T00:57:12.913615+00:00","updated_at":"2026-07-05T00:57:12.913615+00:00"}