{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:365M4QGTA4BQWIHBXN67NXP5QQ","short_pith_number":"pith:365M4QGT","schema_version":"1.0","canonical_sha256":"dfbace40d307030b20e1bb7df6ddfd842fb990a93c7ac6700b0fadb89e4319df","source":{"kind":"arxiv","id":"2108.09910","version":1},"attestation_state":"computed","paper":{"title":"Electromagnetic Field Produced in High Energy Small Collision System within Charge Density Models of Nucleon","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Wei-tian Deng, Xian-Zhuo Cen, Zong-Wei Zhang","submitted_at":"2021-08-23T03:27:51Z","abstract_excerpt":"Recent experiments show that $\\Delta\\gamma$, an observable designed for detecting the chiral magnetic effect (CME), in small collision system $p+A$ is similar with that in heavy ion collision $A+A$. This brings a challenge to the existence of CME because it is believed that there is no azimuthal correlation between the orientation of the magnetic field ($\\Phi_B$) and the participant plane ($\\Phi_2$) in small collision system. In this work, we introduce three charge density models to describe the inner charge distributions of proton and neutron, and calculate the electric and magnetic fields pr"},"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":"2108.09910","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2021-08-23T03:27:51Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"aa701c5922779f30ebbfbc16186ae147946c946a51857ab4c6aff752ff9f78b1","abstract_canon_sha256":"f71559772cf4e7feedf29d4c662d31b7f2593539df179d8ca565c6c2369925d4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:47:08.247406Z","signature_b64":"V96Vv23ScJYWhF4nkBvuoYvE8mMBBbL0D5/lIRGwHPZfE85Yyf1T5CeTJ0Y/I7ntHg0jMi43+TgxGVs698jcBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dfbace40d307030b20e1bb7df6ddfd842fb990a93c7ac6700b0fadb89e4319df","last_reissued_at":"2026-07-05T04:47:08.246918Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:47:08.246918Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electromagnetic Field Produced in High Energy Small Collision System within Charge Density Models of Nucleon","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Wei-tian Deng, Xian-Zhuo Cen, Zong-Wei Zhang","submitted_at":"2021-08-23T03:27:51Z","abstract_excerpt":"Recent experiments show that $\\Delta\\gamma$, an observable designed for detecting the chiral magnetic effect (CME), in small collision system $p+A$ is similar with that in heavy ion collision $A+A$. This brings a challenge to the existence of CME because it is believed that there is no azimuthal correlation between the orientation of the magnetic field ($\\Phi_B$) and the participant plane ($\\Phi_2$) in small collision system. In this work, we introduce three charge density models to describe the inner charge distributions of proton and neutron, and calculate the electric and magnetic fields pr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2108.09910","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/2108.09910/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":"2108.09910","created_at":"2026-07-05T04:47:08.246977+00:00"},{"alias_kind":"arxiv_version","alias_value":"2108.09910v1","created_at":"2026-07-05T04:47:08.246977+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2108.09910","created_at":"2026-07-05T04:47:08.246977+00:00"},{"alias_kind":"pith_short_12","alias_value":"365M4QGTA4BQ","created_at":"2026-07-05T04:47:08.246977+00:00"},{"alias_kind":"pith_short_16","alias_value":"365M4QGTA4BQWIHB","created_at":"2026-07-05T04:47:08.246977+00:00"},{"alias_kind":"pith_short_8","alias_value":"365M4QGT","created_at":"2026-07-05T04:47:08.246977+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2608.10496","citing_title":"Event-by-event analysis of chiral charge separation in $p^{\\uparrow}+$Au collisions within an improved AMPT model","ref_index":27,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/365M4QGTA4BQWIHBXN67NXP5QQ","json":"https://pith.science/pith/365M4QGTA4BQWIHBXN67NXP5QQ.json","graph_json":"https://pith.science/api/pith-number/365M4QGTA4BQWIHBXN67NXP5QQ/graph.json","events_json":"https://pith.science/api/pith-number/365M4QGTA4BQWIHBXN67NXP5QQ/events.json","paper":"https://pith.science/paper/365M4QGT"},"agent_actions":{"view_html":"https://pith.science/pith/365M4QGTA4BQWIHBXN67NXP5QQ","download_json":"https://pith.science/pith/365M4QGTA4BQWIHBXN67NXP5QQ.json","view_paper":"https://pith.science/paper/365M4QGT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2108.09910&json=true","fetch_graph":"https://pith.science/api/pith-number/365M4QGTA4BQWIHBXN67NXP5QQ/graph.json","fetch_events":"https://pith.science/api/pith-number/365M4QGTA4BQWIHBXN67NXP5QQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/365M4QGTA4BQWIHBXN67NXP5QQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/365M4QGTA4BQWIHBXN67NXP5QQ/action/storage_attestation","attest_author":"https://pith.science/pith/365M4QGTA4BQWIHBXN67NXP5QQ/action/author_attestation","sign_citation":"https://pith.science/pith/365M4QGTA4BQWIHBXN67NXP5QQ/action/citation_signature","submit_replication":"https://pith.science/pith/365M4QGTA4BQWIHBXN67NXP5QQ/action/replication_record"}},"created_at":"2026-07-05T04:47:08.246977+00:00","updated_at":"2026-07-05T04:47:08.246977+00:00"}