{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:J3LXJB5BU7QQTVBEC3B7AI2GAR","short_pith_number":"pith:J3LXJB5B","schema_version":"1.0","canonical_sha256":"4ed77487a1a7e109d42416c3f02346046e2e627634065a88fe82748f885ac0bb","source":{"kind":"arxiv","id":"2202.09184","version":2},"attestation_state":"computed","paper":{"title":"Taylor expansions and Pad\\'e approximants for cumulants of conserved charge fluctuations at non-vanishing chemical potentials","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"C. Schmidt, D. Bollweg, F. Karsch, J. Goswami, O. Kaczmarek, P. Petreczky, P. Scior, Swagato Mukherjee","submitted_at":"2022-02-18T13:26:59Z","abstract_excerpt":"Using high statistics datasets generated in (2+1)-flavor QCD calculations at finite temperature we present results for low order cumulants of net baryon-number fluctuations at non-zero values of the baryon chemical potential. We calculate Taylor expansions for the pressure (zeroth order cumulant), net baryon-number density (first order cumulant) and the variance of the distribution on net-baryon number fluctuations (second order cumulant). We obtain series expansions from an eighth order expansion of the pressure and compare these to diagonal Pad\\'e approximants. This allows us to estimate the"},"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":"2202.09184","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-lat","submitted_at":"2022-02-18T13:26:59Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"ecf085c90e0d61639174f2c593163d8c89681dda2ec988eee1cbbdb6c50e6f0b","abstract_canon_sha256":"27bea3eeeedb177311838d0c0b711b0b6aecf2d42bcba48073f2744613f139cb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:19:06.730452Z","signature_b64":"oEZdgl4KUqt1z+iMywYJZuRCaf1m4DAtm0l5xp/R5e7HDtYIrYQfidUFxZ4z4AqxI8rZnRZ2GQsUzaNlzRkIDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4ed77487a1a7e109d42416c3f02346046e2e627634065a88fe82748f885ac0bb","last_reissued_at":"2026-07-05T04:19:06.729947Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:19:06.729947Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Taylor expansions and Pad\\'e approximants for cumulants of conserved charge fluctuations at non-vanishing chemical potentials","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"C. Schmidt, D. Bollweg, F. Karsch, J. Goswami, O. Kaczmarek, P. Petreczky, P. Scior, Swagato Mukherjee","submitted_at":"2022-02-18T13:26:59Z","abstract_excerpt":"Using high statistics datasets generated in (2+1)-flavor QCD calculations at finite temperature we present results for low order cumulants of net baryon-number fluctuations at non-zero values of the baryon chemical potential. We calculate Taylor expansions for the pressure (zeroth order cumulant), net baryon-number density (first order cumulant) and the variance of the distribution on net-baryon number fluctuations (second order cumulant). We obtain series expansions from an eighth order expansion of the pressure and compare these to diagonal Pad\\'e approximants. This allows us to estimate the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2202.09184","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/2202.09184/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":"2202.09184","created_at":"2026-07-05T04:19:06.730006+00:00"},{"alias_kind":"arxiv_version","alias_value":"2202.09184v2","created_at":"2026-07-05T04:19:06.730006+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2202.09184","created_at":"2026-07-05T04:19:06.730006+00:00"},{"alias_kind":"pith_short_12","alias_value":"J3LXJB5BU7QQ","created_at":"2026-07-05T04:19:06.730006+00:00"},{"alias_kind":"pith_short_16","alias_value":"J3LXJB5BU7QQTVBE","created_at":"2026-07-05T04:19:06.730006+00:00"},{"alias_kind":"pith_short_8","alias_value":"J3LXJB5B","created_at":"2026-07-05T04:19:06.730006+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.26326","citing_title":"Studying the QCD Matter produced in Heavy-Ion Collisions using the MUSES Calculation Engine","ref_index":38,"is_internal_anchor":false},{"citing_arxiv_id":"2605.19964","citing_title":"Lee-Yang zeros and edge singularity in a mean-field approach","ref_index":42,"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":20,"is_internal_anchor":false},{"citing_arxiv_id":"2604.19649","citing_title":"Finite-density equation of state of hot QCD using the complex Langevin equation","ref_index":17,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/J3LXJB5BU7QQTVBEC3B7AI2GAR","json":"https://pith.science/pith/J3LXJB5BU7QQTVBEC3B7AI2GAR.json","graph_json":"https://pith.science/api/pith-number/J3LXJB5BU7QQTVBEC3B7AI2GAR/graph.json","events_json":"https://pith.science/api/pith-number/J3LXJB5BU7QQTVBEC3B7AI2GAR/events.json","paper":"https://pith.science/paper/J3LXJB5B"},"agent_actions":{"view_html":"https://pith.science/pith/J3LXJB5BU7QQTVBEC3B7AI2GAR","download_json":"https://pith.science/pith/J3LXJB5BU7QQTVBEC3B7AI2GAR.json","view_paper":"https://pith.science/paper/J3LXJB5B","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2202.09184&json=true","fetch_graph":"https://pith.science/api/pith-number/J3LXJB5BU7QQTVBEC3B7AI2GAR/graph.json","fetch_events":"https://pith.science/api/pith-number/J3LXJB5BU7QQTVBEC3B7AI2GAR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/J3LXJB5BU7QQTVBEC3B7AI2GAR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/J3LXJB5BU7QQTVBEC3B7AI2GAR/action/storage_attestation","attest_author":"https://pith.science/pith/J3LXJB5BU7QQTVBEC3B7AI2GAR/action/author_attestation","sign_citation":"https://pith.science/pith/J3LXJB5BU7QQTVBEC3B7AI2GAR/action/citation_signature","submit_replication":"https://pith.science/pith/J3LXJB5BU7QQTVBEC3B7AI2GAR/action/replication_record"}},"created_at":"2026-07-05T04:19:06.730006+00:00","updated_at":"2026-07-05T04:19:06.730006+00:00"}