{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:ZI2WBIAWY6KYM3DB57HNQ2VMXI","short_pith_number":"pith:ZI2WBIAW","schema_version":"1.0","canonical_sha256":"ca3560a016c795866c61efced86aacba1fc5ca28c051513519d144813cf37655","source":{"kind":"arxiv","id":"1708.08901","version":2},"attestation_state":"computed","paper":{"title":"Probing the chiral magnetic wave in pPb and PbPb collisions at $ \\sqrt{\\smash[b]{s_{_{\\mathrm{NN}}}}} = $ 5.02 TeV using charge-dependent azimuthal anisotropies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"CMS Collaboration","submitted_at":"2017-08-29T17:39:16Z","abstract_excerpt":"Charge-dependent anisotropy Fourier coefficients ($v_n$) of particle azimuthal distributions are measured in pPb and PbPb collisions at $ \\sqrt{\\smash[b]{s_{_{\\mathrm{NN}}}}} = $ 5.02 TeV with the CMS detector at the LHC. The normalized difference in the second-order anisotropy coefficients ($v_2$) between positively and negatively charged particles is found to depend linearly on the observed event charge asymmetry with comparable slopes for both pPb and PbPb collisions over a wide range of charged particle multiplicity. In PbPb, the third-order anisotropy coefficient, $v_3$, shows a similar l"},"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":"1708.08901","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2017-08-29T17:39:16Z","cross_cats_sorted":[],"title_canon_sha256":"f0f18dc03789ac0b3c69adb7755b7c8760fae5fc086a017c16a49b214ec313d1","abstract_canon_sha256":"804fcbd7db2ee4f9779095a2c9caabd7302df79d05d475d6d0b90ddcd82a1b58"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:28:05.782630Z","signature_b64":"B79fDA79ducHj2p92DTmEfqZH0d1/nAtUZDFuKqJjiA+IV09g0XbMUF/5rTHFd6FNCpg+3f3outxLv1We2KQAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ca3560a016c795866c61efced86aacba1fc5ca28c051513519d144813cf37655","last_reissued_at":"2026-07-05T00:28:05.782254Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:28:05.782254Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Probing the chiral magnetic wave in pPb and PbPb collisions at $ \\sqrt{\\smash[b]{s_{_{\\mathrm{NN}}}}} = $ 5.02 TeV using charge-dependent azimuthal anisotropies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"CMS Collaboration","submitted_at":"2017-08-29T17:39:16Z","abstract_excerpt":"Charge-dependent anisotropy Fourier coefficients ($v_n$) of particle azimuthal distributions are measured in pPb and PbPb collisions at $ \\sqrt{\\smash[b]{s_{_{\\mathrm{NN}}}}} = $ 5.02 TeV with the CMS detector at the LHC. The normalized difference in the second-order anisotropy coefficients ($v_2$) between positively and negatively charged particles is found to depend linearly on the observed event charge asymmetry with comparable slopes for both pPb and PbPb collisions over a wide range of charged particle multiplicity. In PbPb, the third-order anisotropy coefficient, $v_3$, shows a similar l"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.08901","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/1708.08901/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":"1708.08901","created_at":"2026-07-05T00:28:05.782311+00:00"},{"alias_kind":"arxiv_version","alias_value":"1708.08901v2","created_at":"2026-07-05T00:28:05.782311+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.08901","created_at":"2026-07-05T00:28:05.782311+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZI2WBIAWY6KY","created_at":"2026-07-05T00:28:05.782311+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZI2WBIAWY6KYM3DB","created_at":"2026-07-05T00:28:05.782311+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZI2WBIAW","created_at":"2026-07-05T00:28:05.782311+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.25487","citing_title":"A higher-harmonic observable for the chiral magnetic effect in heavy-ion collisions","ref_index":48,"is_internal_anchor":false},{"citing_arxiv_id":"1906.11413","citing_title":"Experimental searches for the chiral magnetic effect in heavy-ion collisions","ref_index":143,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZI2WBIAWY6KYM3DB57HNQ2VMXI","json":"https://pith.science/pith/ZI2WBIAWY6KYM3DB57HNQ2VMXI.json","graph_json":"https://pith.science/api/pith-number/ZI2WBIAWY6KYM3DB57HNQ2VMXI/graph.json","events_json":"https://pith.science/api/pith-number/ZI2WBIAWY6KYM3DB57HNQ2VMXI/events.json","paper":"https://pith.science/paper/ZI2WBIAW"},"agent_actions":{"view_html":"https://pith.science/pith/ZI2WBIAWY6KYM3DB57HNQ2VMXI","download_json":"https://pith.science/pith/ZI2WBIAWY6KYM3DB57HNQ2VMXI.json","view_paper":"https://pith.science/paper/ZI2WBIAW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1708.08901&json=true","fetch_graph":"https://pith.science/api/pith-number/ZI2WBIAWY6KYM3DB57HNQ2VMXI/graph.json","fetch_events":"https://pith.science/api/pith-number/ZI2WBIAWY6KYM3DB57HNQ2VMXI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZI2WBIAWY6KYM3DB57HNQ2VMXI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZI2WBIAWY6KYM3DB57HNQ2VMXI/action/storage_attestation","attest_author":"https://pith.science/pith/ZI2WBIAWY6KYM3DB57HNQ2VMXI/action/author_attestation","sign_citation":"https://pith.science/pith/ZI2WBIAWY6KYM3DB57HNQ2VMXI/action/citation_signature","submit_replication":"https://pith.science/pith/ZI2WBIAWY6KYM3DB57HNQ2VMXI/action/replication_record"}},"created_at":"2026-07-05T00:28:05.782311+00:00","updated_at":"2026-07-05T00:28:05.782311+00:00"}