{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:L6RBTTBIMASJXK2ZODMHQO5KC4","short_pith_number":"pith:L6RBTTBI","schema_version":"1.0","canonical_sha256":"5fa219cc2860249bab5970d8783baa1701c0e2a0a974327400afb22192b67c82","source":{"kind":"arxiv","id":"1807.11908","version":2},"attestation_state":"computed","paper":{"title":"Gradient resummation for nonlinear chiral transport: an insight from holography","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-th","authors_text":"Michael Lublinsky, Tuna Demircik, Yanyan Bu","submitted_at":"2018-07-30T14:21:13Z","abstract_excerpt":"Nonlinear transport phenomena induced by chiral anomaly are explored within a 4D field theory defined holographically as $U(1)_V\\times U(1)_A$ Maxwell-Chern-Simons theory in Schwarzschild-$AdS_5$. In presence of weak constant background electromagnetic fields, the constitutive relations for vector and axial currents, resummed to all orders in the gradients of charge densities, are encoded in nine momenta-dependent transport coefficient functions (TCFs). These TCFs are first calculated analytically up to third order in gradient expansion, and then evaluated numerically beyond the hydrodynamic 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":"1807.11908","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2018-07-30T14:21:13Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"3a7935fb1d896c4bf03b9012389f01d387815dc65fb8023eb234c4ce4e8a48e1","abstract_canon_sha256":"569dc202f19ad8d10ccea241d77e8672e66d3aa3a3d37138b0a559b70aa319c9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:50:59.542922Z","signature_b64":"RDF0vj+kKqpPnu9KOKa0bAnx3ydvgA1UtgJv8gdcoho0wk+w8RTMgdHgdRwk/8KU5Yr+Drf2Mg2UvoJ/GvJpCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5fa219cc2860249bab5970d8783baa1701c0e2a0a974327400afb22192b67c82","last_reissued_at":"2026-05-17T23:50:59.542219Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:50:59.542219Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gradient resummation for nonlinear chiral transport: an insight from holography","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-th","authors_text":"Michael Lublinsky, Tuna Demircik, Yanyan Bu","submitted_at":"2018-07-30T14:21:13Z","abstract_excerpt":"Nonlinear transport phenomena induced by chiral anomaly are explored within a 4D field theory defined holographically as $U(1)_V\\times U(1)_A$ Maxwell-Chern-Simons theory in Schwarzschild-$AdS_5$. In presence of weak constant background electromagnetic fields, the constitutive relations for vector and axial currents, resummed to all orders in the gradients of charge densities, are encoded in nine momenta-dependent transport coefficient functions (TCFs). These TCFs are first calculated analytically up to third order in gradient expansion, and then evaluated numerically beyond the hydrodynamic l"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.11908","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":""},"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":"1807.11908","created_at":"2026-05-17T23:50:59.542330+00:00"},{"alias_kind":"arxiv_version","alias_value":"1807.11908v2","created_at":"2026-05-17T23:50:59.542330+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.11908","created_at":"2026-05-17T23:50:59.542330+00:00"},{"alias_kind":"pith_short_12","alias_value":"L6RBTTBIMASJ","created_at":"2026-05-18T12:32:33.847187+00:00"},{"alias_kind":"pith_short_16","alias_value":"L6RBTTBIMASJXK2Z","created_at":"2026-05-18T12:32:33.847187+00:00"},{"alias_kind":"pith_short_8","alias_value":"L6RBTTBI","created_at":"2026-05-18T12:32:33.847187+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/L6RBTTBIMASJXK2ZODMHQO5KC4","json":"https://pith.science/pith/L6RBTTBIMASJXK2ZODMHQO5KC4.json","graph_json":"https://pith.science/api/pith-number/L6RBTTBIMASJXK2ZODMHQO5KC4/graph.json","events_json":"https://pith.science/api/pith-number/L6RBTTBIMASJXK2ZODMHQO5KC4/events.json","paper":"https://pith.science/paper/L6RBTTBI"},"agent_actions":{"view_html":"https://pith.science/pith/L6RBTTBIMASJXK2ZODMHQO5KC4","download_json":"https://pith.science/pith/L6RBTTBIMASJXK2ZODMHQO5KC4.json","view_paper":"https://pith.science/paper/L6RBTTBI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1807.11908&json=true","fetch_graph":"https://pith.science/api/pith-number/L6RBTTBIMASJXK2ZODMHQO5KC4/graph.json","fetch_events":"https://pith.science/api/pith-number/L6RBTTBIMASJXK2ZODMHQO5KC4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/L6RBTTBIMASJXK2ZODMHQO5KC4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/L6RBTTBIMASJXK2ZODMHQO5KC4/action/storage_attestation","attest_author":"https://pith.science/pith/L6RBTTBIMASJXK2ZODMHQO5KC4/action/author_attestation","sign_citation":"https://pith.science/pith/L6RBTTBIMASJXK2ZODMHQO5KC4/action/citation_signature","submit_replication":"https://pith.science/pith/L6RBTTBIMASJXK2ZODMHQO5KC4/action/replication_record"}},"created_at":"2026-05-17T23:50:59.542330+00:00","updated_at":"2026-05-17T23:50:59.542330+00:00"}