{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:B534ZHDG7A6KTMGSHTU4AKLHNY","short_pith_number":"pith:B534ZHDG","schema_version":"1.0","canonical_sha256":"0f77cc9c66f83ca9b0d23ce9c029676e3f47998487259338b7862ecb4d581501","source":{"kind":"arxiv","id":"1704.04382","version":1},"attestation_state":"computed","paper":{"title":"Chiral magnetic effect in isobaric collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"Gang Wang, Guo-Liang Ma, Wei-tian Deng, Xu-Guang Huang","submitted_at":"2017-04-14T10:18:45Z","abstract_excerpt":"We give a numerical simulation of the generation of the magnetic field and the charge-separation signal due to the chiral magnetic effect (CME) --- the induction of an electric current by the magnetic field in a parity-odd matter --- in the collisions of isobaric nuclei, $^{96}_{44}$Ru + $^{96}_{44}$Ru and $^{96}_{40}$Zr + $^{96}_{40}$Zr, at $\\sqrt{s_{\\rm NN}}=200$ GeV. We show that such collisions provide an ideal tool to disentangle the CME signal from the possible elliptic-flow driven background effects. We also discuss some other effects that can be tested by using the isobaric collisions."},"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":"1704.04382","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-04-14T10:18:45Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"db73c5dedc54600814fe4914891f7432d9b7881c28ca2c0b910d17aecc17bd05","abstract_canon_sha256":"e8d5c1af9b68d535e2afe09624e6beeba670cee501084d84ca2a492add1cd254"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:21:28.443887Z","signature_b64":"8nFMMSiWe9ISkAacV4j71xa5YjPyA69ZrDN0qF7sJ01BxXMXloY50nzIP7iWfBGlQ5MbkaEaKgEQMFz7WlVyDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0f77cc9c66f83ca9b0d23ce9c029676e3f47998487259338b7862ecb4d581501","last_reissued_at":"2026-05-18T00:21:28.443232Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:21:28.443232Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Chiral magnetic effect in isobaric collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"Gang Wang, Guo-Liang Ma, Wei-tian Deng, Xu-Guang Huang","submitted_at":"2017-04-14T10:18:45Z","abstract_excerpt":"We give a numerical simulation of the generation of the magnetic field and the charge-separation signal due to the chiral magnetic effect (CME) --- the induction of an electric current by the magnetic field in a parity-odd matter --- in the collisions of isobaric nuclei, $^{96}_{44}$Ru + $^{96}_{44}$Ru and $^{96}_{40}$Zr + $^{96}_{40}$Zr, at $\\sqrt{s_{\\rm NN}}=200$ GeV. We show that such collisions provide an ideal tool to disentangle the CME signal from the possible elliptic-flow driven background effects. We also discuss some other effects that can be tested by using the isobaric collisions."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.04382","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":""},"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":"1704.04382","created_at":"2026-05-18T00:21:28.443341+00:00"},{"alias_kind":"arxiv_version","alias_value":"1704.04382v1","created_at":"2026-05-18T00:21:28.443341+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.04382","created_at":"2026-05-18T00:21:28.443341+00:00"},{"alias_kind":"pith_short_12","alias_value":"B534ZHDG7A6K","created_at":"2026-05-18T12:31:08.081275+00:00"},{"alias_kind":"pith_short_16","alias_value":"B534ZHDG7A6KTMGS","created_at":"2026-05-18T12:31:08.081275+00:00"},{"alias_kind":"pith_short_8","alias_value":"B534ZHDG","created_at":"2026-05-18T12:31:08.081275+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/B534ZHDG7A6KTMGSHTU4AKLHNY","json":"https://pith.science/pith/B534ZHDG7A6KTMGSHTU4AKLHNY.json","graph_json":"https://pith.science/api/pith-number/B534ZHDG7A6KTMGSHTU4AKLHNY/graph.json","events_json":"https://pith.science/api/pith-number/B534ZHDG7A6KTMGSHTU4AKLHNY/events.json","paper":"https://pith.science/paper/B534ZHDG"},"agent_actions":{"view_html":"https://pith.science/pith/B534ZHDG7A6KTMGSHTU4AKLHNY","download_json":"https://pith.science/pith/B534ZHDG7A6KTMGSHTU4AKLHNY.json","view_paper":"https://pith.science/paper/B534ZHDG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1704.04382&json=true","fetch_graph":"https://pith.science/api/pith-number/B534ZHDG7A6KTMGSHTU4AKLHNY/graph.json","fetch_events":"https://pith.science/api/pith-number/B534ZHDG7A6KTMGSHTU4AKLHNY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/B534ZHDG7A6KTMGSHTU4AKLHNY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/B534ZHDG7A6KTMGSHTU4AKLHNY/action/storage_attestation","attest_author":"https://pith.science/pith/B534ZHDG7A6KTMGSHTU4AKLHNY/action/author_attestation","sign_citation":"https://pith.science/pith/B534ZHDG7A6KTMGSHTU4AKLHNY/action/citation_signature","submit_replication":"https://pith.science/pith/B534ZHDG7A6KTMGSHTU4AKLHNY/action/replication_record"}},"created_at":"2026-05-18T00:21:28.443341+00:00","updated_at":"2026-05-18T00:21:28.443341+00:00"}