{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:DCGJ7TJNUOS3IWB5MGPJ5RZRM6","short_pith_number":"pith:DCGJ7TJN","schema_version":"1.0","canonical_sha256":"188c9fcd2da3a5b4583d619e9ec731679c7e4e5ee90dd91fdeba84e703c5bf0a","source":{"kind":"arxiv","id":"1708.08536","version":2},"attestation_state":"computed","paper":{"title":"Electrodynamics of dual superconducting chiral medium","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con","nucl-th"],"primary_cat":"hep-ph","authors_text":"Kirill Tuchin, Yang Li","submitted_at":"2017-08-28T21:43:00Z","abstract_excerpt":"We study the electrodynamics of a chiral medium with electric and magnetic charges using the effective Maxwell-Chern-Simons theory extended to include the magnetic current. The exchange of helicity between the chiral medium and the magnetic field, known as the inverse cascade, is controlled by the chiral anomaly equation. In the presence of the magnetic current, the magnetic helicity is dissipated, so that the inverse cascade stops when the magnetic helicity vanishes while the chiral conductivity reaches a non-vanishing stationary value satisfying $\\sigma_\\chi^2< 4\\sigma_e\\sigma_m$, where $\\si"},"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":"1708.08536","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-08-28T21:43:00Z","cross_cats_sorted":["cond-mat.supr-con","nucl-th"],"title_canon_sha256":"dfcc7ebec50272fd638746adcad878efe646506c659dbfd50cd521d19ee90323","abstract_canon_sha256":"b41e766a28e51958a8065d3a7c4f22413de8fe3662ec37cd06f275ce23aaf583"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:28:22.720255Z","signature_b64":"3ft4hcr0wA1w7LjavorO1FxCXghS0AuCi58X3I936bvpZN/xgedLXFnpchQFeX1oetx2MHzJN4KM5j6YPzTlBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"188c9fcd2da3a5b4583d619e9ec731679c7e4e5ee90dd91fdeba84e703c5bf0a","last_reissued_at":"2026-05-18T00:28:22.719664Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:28:22.719664Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electrodynamics of dual superconducting chiral medium","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con","nucl-th"],"primary_cat":"hep-ph","authors_text":"Kirill Tuchin, Yang Li","submitted_at":"2017-08-28T21:43:00Z","abstract_excerpt":"We study the electrodynamics of a chiral medium with electric and magnetic charges using the effective Maxwell-Chern-Simons theory extended to include the magnetic current. The exchange of helicity between the chiral medium and the magnetic field, known as the inverse cascade, is controlled by the chiral anomaly equation. In the presence of the magnetic current, the magnetic helicity is dissipated, so that the inverse cascade stops when the magnetic helicity vanishes while the chiral conductivity reaches a non-vanishing stationary value satisfying $\\sigma_\\chi^2< 4\\sigma_e\\sigma_m$, where $\\si"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.08536","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":"1708.08536","created_at":"2026-05-18T00:28:22.719756+00:00"},{"alias_kind":"arxiv_version","alias_value":"1708.08536v2","created_at":"2026-05-18T00:28:22.719756+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.08536","created_at":"2026-05-18T00:28:22.719756+00:00"},{"alias_kind":"pith_short_12","alias_value":"DCGJ7TJNUOS3","created_at":"2026-05-18T12:31:10.602751+00:00"},{"alias_kind":"pith_short_16","alias_value":"DCGJ7TJNUOS3IWB5","created_at":"2026-05-18T12:31:10.602751+00:00"},{"alias_kind":"pith_short_8","alias_value":"DCGJ7TJN","created_at":"2026-05-18T12:31:10.602751+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/DCGJ7TJNUOS3IWB5MGPJ5RZRM6","json":"https://pith.science/pith/DCGJ7TJNUOS3IWB5MGPJ5RZRM6.json","graph_json":"https://pith.science/api/pith-number/DCGJ7TJNUOS3IWB5MGPJ5RZRM6/graph.json","events_json":"https://pith.science/api/pith-number/DCGJ7TJNUOS3IWB5MGPJ5RZRM6/events.json","paper":"https://pith.science/paper/DCGJ7TJN"},"agent_actions":{"view_html":"https://pith.science/pith/DCGJ7TJNUOS3IWB5MGPJ5RZRM6","download_json":"https://pith.science/pith/DCGJ7TJNUOS3IWB5MGPJ5RZRM6.json","view_paper":"https://pith.science/paper/DCGJ7TJN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1708.08536&json=true","fetch_graph":"https://pith.science/api/pith-number/DCGJ7TJNUOS3IWB5MGPJ5RZRM6/graph.json","fetch_events":"https://pith.science/api/pith-number/DCGJ7TJNUOS3IWB5MGPJ5RZRM6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DCGJ7TJNUOS3IWB5MGPJ5RZRM6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DCGJ7TJNUOS3IWB5MGPJ5RZRM6/action/storage_attestation","attest_author":"https://pith.science/pith/DCGJ7TJNUOS3IWB5MGPJ5RZRM6/action/author_attestation","sign_citation":"https://pith.science/pith/DCGJ7TJNUOS3IWB5MGPJ5RZRM6/action/citation_signature","submit_replication":"https://pith.science/pith/DCGJ7TJNUOS3IWB5MGPJ5RZRM6/action/replication_record"}},"created_at":"2026-05-18T00:28:22.719756+00:00","updated_at":"2026-05-18T00:28:22.719756+00:00"}