{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:ZQTWVPFBBCD5QNTWA5ZMGLJTYJ","short_pith_number":"pith:ZQTWVPFB","schema_version":"1.0","canonical_sha256":"cc276abca10887d836760772c32d33c2667c1b286293f6c0bb12dba471ba1c0c","source":{"kind":"arxiv","id":"2508.16988","version":1},"attestation_state":"computed","paper":{"title":"Probing Dynamical Electrical Conductivity via Dilepton Emission: A Kinetic theory approach","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Ankit Kumar Panda, Ashutosh Dwibedi, Sabyasachi Ghosh, Victor Roy","submitted_at":"2025-08-23T11:03:55Z","abstract_excerpt":"Dileptons serve as a clean and penetrating probe of the Quark--Gluon Plasma created in high-energy heavy-ion collisions. In this work, we investigate thermal dilepton spectra and their elliptic flow through the dynamical conductivity that governs the production rate. The conductivity is obtained from the trace of the spectral function within relativistic kinetic theory using the Relaxation Time Approximation. This allows us to derive for the first time an analytical expression for the dilepton rate with explicit dependence on the relaxation time of quark-antiquark interactions. We find a non-m"},"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":"2508.16988","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2025-08-23T11:03:55Z","cross_cats_sorted":[],"title_canon_sha256":"8d2f5d001a554abf1075e158f99fd962ae643b03e590be3bd915b3ac3da28e1f","abstract_canon_sha256":"bb15f7daab3da6d38a0aa9802d1db3485b28f54ffe4f745cbbe48771ff5c5e6f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:58:07.754721Z","signature_b64":"asJq3kPVQ1vyZcPfVlLoXvgkY1lgSr0sNyuVR541n/z/SOGRdIAEVGnwHn/HmS8DPNpczWR6BVZez+g4Oc7LCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cc276abca10887d836760772c32d33c2667c1b286293f6c0bb12dba471ba1c0c","last_reissued_at":"2026-07-05T11:58:07.754198Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:58:07.754198Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Probing Dynamical Electrical Conductivity via Dilepton Emission: A Kinetic theory approach","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Ankit Kumar Panda, Ashutosh Dwibedi, Sabyasachi Ghosh, Victor Roy","submitted_at":"2025-08-23T11:03:55Z","abstract_excerpt":"Dileptons serve as a clean and penetrating probe of the Quark--Gluon Plasma created in high-energy heavy-ion collisions. In this work, we investigate thermal dilepton spectra and their elliptic flow through the dynamical conductivity that governs the production rate. The conductivity is obtained from the trace of the spectral function within relativistic kinetic theory using the Relaxation Time Approximation. This allows us to derive for the first time an analytical expression for the dilepton rate with explicit dependence on the relaxation time of quark-antiquark interactions. We find a non-m"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2508.16988","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/2508.16988/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":"2508.16988","created_at":"2026-07-05T11:58:07.754267+00:00"},{"alias_kind":"arxiv_version","alias_value":"2508.16988v1","created_at":"2026-07-05T11:58:07.754267+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2508.16988","created_at":"2026-07-05T11:58:07.754267+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZQTWVPFBBCD5","created_at":"2026-07-05T11:58:07.754267+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZQTWVPFBBCD5QNTW","created_at":"2026-07-05T11:58:07.754267+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZQTWVPFB","created_at":"2026-07-05T11:58:07.754267+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.13646","citing_title":"Observable Dependence of Viscous Corrections in QGP: Heavy Quarks and Dileptons in Chapman--Enskog Theory","ref_index":53,"is_internal_anchor":false},{"citing_arxiv_id":"2606.31749","citing_title":"Finite-Density Dynamics of Chemically Equilibrating QGP in Conformal Gubser Flow and Hard Thermal Photon Production","ref_index":63,"is_internal_anchor":false},{"citing_arxiv_id":"2604.27800","citing_title":"Electromagnetic response of a relativistic drifting plasma","ref_index":20,"is_internal_anchor":false},{"citing_arxiv_id":"2605.01807","citing_title":"Relativistic BDNK MHD Evolution in a Boost-Invariant Medium and Its Impact on Dilepton Production","ref_index":83,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZQTWVPFBBCD5QNTWA5ZMGLJTYJ","json":"https://pith.science/pith/ZQTWVPFBBCD5QNTWA5ZMGLJTYJ.json","graph_json":"https://pith.science/api/pith-number/ZQTWVPFBBCD5QNTWA5ZMGLJTYJ/graph.json","events_json":"https://pith.science/api/pith-number/ZQTWVPFBBCD5QNTWA5ZMGLJTYJ/events.json","paper":"https://pith.science/paper/ZQTWVPFB"},"agent_actions":{"view_html":"https://pith.science/pith/ZQTWVPFBBCD5QNTWA5ZMGLJTYJ","download_json":"https://pith.science/pith/ZQTWVPFBBCD5QNTWA5ZMGLJTYJ.json","view_paper":"https://pith.science/paper/ZQTWVPFB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2508.16988&json=true","fetch_graph":"https://pith.science/api/pith-number/ZQTWVPFBBCD5QNTWA5ZMGLJTYJ/graph.json","fetch_events":"https://pith.science/api/pith-number/ZQTWVPFBBCD5QNTWA5ZMGLJTYJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZQTWVPFBBCD5QNTWA5ZMGLJTYJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZQTWVPFBBCD5QNTWA5ZMGLJTYJ/action/storage_attestation","attest_author":"https://pith.science/pith/ZQTWVPFBBCD5QNTWA5ZMGLJTYJ/action/author_attestation","sign_citation":"https://pith.science/pith/ZQTWVPFBBCD5QNTWA5ZMGLJTYJ/action/citation_signature","submit_replication":"https://pith.science/pith/ZQTWVPFBBCD5QNTWA5ZMGLJTYJ/action/replication_record"}},"created_at":"2026-07-05T11:58:07.754267+00:00","updated_at":"2026-07-05T11:58:07.754267+00:00"}