{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:5I3VQ6HKYIPMUNMCB4AYGA3H5V","short_pith_number":"pith:5I3VQ6HK","schema_version":"1.0","canonical_sha256":"ea375878eac21eca35820f01830367ed5bcd4bf278ecb916e0efacedbf3f5dc8","source":{"kind":"arxiv","id":"2503.04660","version":1},"attestation_state":"computed","paper":{"title":"Charge dependent directed flow splitting from baryon inhomogeneity and electromagnetic field","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":["hep-ex","hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"Sandeep Chatterjee, Subhash Singha, Tribhuban Parida","submitted_at":"2025-03-06T17:54:55Z","abstract_excerpt":"This work aims to understand the recent experimental data from the STAR collaboration on the system size dependence of directed flow splitting between oppositely charged hadrons [arXiv:2412.18326]. Previously, we have studied the role of baryon inhomogeneity on charge dependent directed flow. We now incorporate the effects of the electromagnetic (EM) field albeit perturbatively, as implemented in Ref. [arXiv:1806.05288]. This enables us to compare the relative contributions between baryon inhomogeneity and EM field on charge dependent directed flow. Our model calculation describes the experime"},"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":"2503.04660","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"nucl-th","submitted_at":"2025-03-06T17:54:55Z","cross_cats_sorted":["hep-ex","hep-ph","nucl-ex"],"title_canon_sha256":"c27da3f93482db729d51cf53a4803284e8cc87554df25c26f7c235fd986e0242","abstract_canon_sha256":"225ddd9fc66fb17db02d2a21ac4376ea73fd470ef6fc9eb1922c643ab4b23c1e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:25:44.506658Z","signature_b64":"DkThWFFw76ii1KGcx+B4wmJTl/d9Q/cXFSfK5xjMVMQkS90/EWB/iZUSeYiYtaCverD1I1NERKXjaZZ9WhIJBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ea375878eac21eca35820f01830367ed5bcd4bf278ecb916e0efacedbf3f5dc8","last_reissued_at":"2026-07-05T10:25:44.505670Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:25:44.505670Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Charge dependent directed flow splitting from baryon inhomogeneity and electromagnetic field","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":["hep-ex","hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"Sandeep Chatterjee, Subhash Singha, Tribhuban Parida","submitted_at":"2025-03-06T17:54:55Z","abstract_excerpt":"This work aims to understand the recent experimental data from the STAR collaboration on the system size dependence of directed flow splitting between oppositely charged hadrons [arXiv:2412.18326]. Previously, we have studied the role of baryon inhomogeneity on charge dependent directed flow. We now incorporate the effects of the electromagnetic (EM) field albeit perturbatively, as implemented in Ref. [arXiv:1806.05288]. This enables us to compare the relative contributions between baryon inhomogeneity and EM field on charge dependent directed flow. Our model calculation describes the experime"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2503.04660","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/2503.04660/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":"2503.04660","created_at":"2026-07-05T10:25:44.505805+00:00"},{"alias_kind":"arxiv_version","alias_value":"2503.04660v1","created_at":"2026-07-05T10:25:44.505805+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2503.04660","created_at":"2026-07-05T10:25:44.505805+00:00"},{"alias_kind":"pith_short_12","alias_value":"5I3VQ6HKYIPM","created_at":"2026-07-05T10:25:44.505805+00:00"},{"alias_kind":"pith_short_16","alias_value":"5I3VQ6HKYIPMUNMC","created_at":"2026-07-05T10:25:44.505805+00:00"},{"alias_kind":"pith_short_8","alias_value":"5I3VQ6HK","created_at":"2026-07-05T10:25:44.505805+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.01807","citing_title":"Relativistic BDNK MHD Evolution in a Boost-Invariant Medium and Its Impact on Dilepton Production","ref_index":77,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5I3VQ6HKYIPMUNMCB4AYGA3H5V","json":"https://pith.science/pith/5I3VQ6HKYIPMUNMCB4AYGA3H5V.json","graph_json":"https://pith.science/api/pith-number/5I3VQ6HKYIPMUNMCB4AYGA3H5V/graph.json","events_json":"https://pith.science/api/pith-number/5I3VQ6HKYIPMUNMCB4AYGA3H5V/events.json","paper":"https://pith.science/paper/5I3VQ6HK"},"agent_actions":{"view_html":"https://pith.science/pith/5I3VQ6HKYIPMUNMCB4AYGA3H5V","download_json":"https://pith.science/pith/5I3VQ6HKYIPMUNMCB4AYGA3H5V.json","view_paper":"https://pith.science/paper/5I3VQ6HK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2503.04660&json=true","fetch_graph":"https://pith.science/api/pith-number/5I3VQ6HKYIPMUNMCB4AYGA3H5V/graph.json","fetch_events":"https://pith.science/api/pith-number/5I3VQ6HKYIPMUNMCB4AYGA3H5V/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5I3VQ6HKYIPMUNMCB4AYGA3H5V/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5I3VQ6HKYIPMUNMCB4AYGA3H5V/action/storage_attestation","attest_author":"https://pith.science/pith/5I3VQ6HKYIPMUNMCB4AYGA3H5V/action/author_attestation","sign_citation":"https://pith.science/pith/5I3VQ6HKYIPMUNMCB4AYGA3H5V/action/citation_signature","submit_replication":"https://pith.science/pith/5I3VQ6HKYIPMUNMCB4AYGA3H5V/action/replication_record"}},"created_at":"2026-07-05T10:25:44.505805+00:00","updated_at":"2026-07-05T10:25:44.505805+00:00"}