{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:AD25QAJTJCNHJW5KEGYBYMR7HA","short_pith_number":"pith:AD25QAJT","schema_version":"1.0","canonical_sha256":"00f5d80133489a74dbaa21b01c323f38243d9e4c14b9289e59427ac24adebd5f","source":{"kind":"arxiv","id":"2312.12376","version":1},"attestation_state":"computed","paper":{"title":"Tracing baryon and electric charge transport in isobar collisions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Akihiko Monnai, Bj\\\"orn Schenke, Chun Shen, Gregoire Pihan","submitted_at":"2023-12-19T18:09:05Z","abstract_excerpt":"It is of fundamental interest to understand the carrier of conserved quantum charges within protons and nuclei at high energy. Preliminary data from isobar collisions at RHIC reveal a scaled net-baryon to net-electric charge ratio ($B/\\Delta Q \\times \\Delta Z/A$) at mid-rapidity between 1.2 and 2, consistent with string junction model predictions. Here, we compute the initial stage scaled net-baryon to net-electric charge ratio for isobar collisions. Our model incorporates a realization of the string junction model and models the nuclear structure. Our predictions identify the baseline expecta"},"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":"2312.12376","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2023-12-19T18:09:05Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"9897c875c4c5d3dcceeb90538de4327676e8259cd61b4e492440efbe5a922c44","abstract_canon_sha256":"7bb80711574fe6585341cc1f2aaec1062ada18b6a6807b11438d74adb706f2e9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:26:02.622838Z","signature_b64":"R/r/AwzZPUOegg/rzoIMt9rZ+878GoijMt0KmPMZ/sbNinB/0kixPRChxz7brpV5MmCemkVTZfudUg61c4zqAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"00f5d80133489a74dbaa21b01c323f38243d9e4c14b9289e59427ac24adebd5f","last_reissued_at":"2026-07-05T07:26:02.622353Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:26:02.622353Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Tracing baryon and electric charge transport in isobar collisions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Akihiko Monnai, Bj\\\"orn Schenke, Chun Shen, Gregoire Pihan","submitted_at":"2023-12-19T18:09:05Z","abstract_excerpt":"It is of fundamental interest to understand the carrier of conserved quantum charges within protons and nuclei at high energy. Preliminary data from isobar collisions at RHIC reveal a scaled net-baryon to net-electric charge ratio ($B/\\Delta Q \\times \\Delta Z/A$) at mid-rapidity between 1.2 and 2, consistent with string junction model predictions. Here, we compute the initial stage scaled net-baryon to net-electric charge ratio for isobar collisions. Our model incorporates a realization of the string junction model and models the nuclear structure. Our predictions identify the baseline expecta"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2312.12376","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/2312.12376/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":"2312.12376","created_at":"2026-07-05T07:26:02.622413+00:00"},{"alias_kind":"arxiv_version","alias_value":"2312.12376v1","created_at":"2026-07-05T07:26:02.622413+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2312.12376","created_at":"2026-07-05T07:26:02.622413+00:00"},{"alias_kind":"pith_short_12","alias_value":"AD25QAJTJCNH","created_at":"2026-07-05T07:26:02.622413+00:00"},{"alias_kind":"pith_short_16","alias_value":"AD25QAJTJCNHJW5K","created_at":"2026-07-05T07:26:02.622413+00:00"},{"alias_kind":"pith_short_8","alias_value":"AD25QAJT","created_at":"2026-07-05T07:26:02.622413+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.30164","citing_title":"Isospin-Driven Splitting of Chemical Potentials in Isobar Collisions from Lattice QCD","ref_index":58,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/AD25QAJTJCNHJW5KEGYBYMR7HA","json":"https://pith.science/pith/AD25QAJTJCNHJW5KEGYBYMR7HA.json","graph_json":"https://pith.science/api/pith-number/AD25QAJTJCNHJW5KEGYBYMR7HA/graph.json","events_json":"https://pith.science/api/pith-number/AD25QAJTJCNHJW5KEGYBYMR7HA/events.json","paper":"https://pith.science/paper/AD25QAJT"},"agent_actions":{"view_html":"https://pith.science/pith/AD25QAJTJCNHJW5KEGYBYMR7HA","download_json":"https://pith.science/pith/AD25QAJTJCNHJW5KEGYBYMR7HA.json","view_paper":"https://pith.science/paper/AD25QAJT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2312.12376&json=true","fetch_graph":"https://pith.science/api/pith-number/AD25QAJTJCNHJW5KEGYBYMR7HA/graph.json","fetch_events":"https://pith.science/api/pith-number/AD25QAJTJCNHJW5KEGYBYMR7HA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AD25QAJTJCNHJW5KEGYBYMR7HA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AD25QAJTJCNHJW5KEGYBYMR7HA/action/storage_attestation","attest_author":"https://pith.science/pith/AD25QAJTJCNHJW5KEGYBYMR7HA/action/author_attestation","sign_citation":"https://pith.science/pith/AD25QAJTJCNHJW5KEGYBYMR7HA/action/citation_signature","submit_replication":"https://pith.science/pith/AD25QAJTJCNHJW5KEGYBYMR7HA/action/replication_record"}},"created_at":"2026-07-05T07:26:02.622413+00:00","updated_at":"2026-07-05T07:26:02.622413+00:00"}