{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:B2MX554JDV6J24ZSSJM6BVIKUD","short_pith_number":"pith:B2MX554J","schema_version":"1.0","canonical_sha256":"0e997ef7891d7c9d73329259e0d50aa0c6c36c160be40252373ce0ef3bb0f1a4","source":{"kind":"arxiv","id":"2211.09575","version":1},"attestation_state":"computed","paper":{"title":"Shedding light on thermal photon and dilepton production","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Greg Jackson","submitted_at":"2022-11-17T15:00:58Z","abstract_excerpt":"Electromagnetic radiation from the quark-gluon plasma (QGP) is an important observable to be considered in heavy ion collision experiments. I will provide an update on recent advancements from perturbation theory and quenched lattice simulations. The resummed next-to-leading order (NLO) emission rate has recently been decomposed into transverse and longitudinal components, and extended to non-zero baryon chemical potential. The associated spectral function has also been tested against the Euclidean correlator, for continuum-extrapolated lattice data (at $\\mu_{\\rm B}=0$)."},"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":"2211.09575","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2022-11-17T15:00:58Z","cross_cats_sorted":[],"title_canon_sha256":"5dd77ae49780afa4b84eb1febb7ac33184f779efb945e7dd992ef17009923689","abstract_canon_sha256":"300d244c297943042d5b2ad5e5d4c014f4910fce9a06e425c5d631f0d2eb5628"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:31:59.373935Z","signature_b64":"zHB8gey3j71MDctsBY1dm+B+l2WH/QPme2jX7jjL9TykKUpSuWpzE/LBI4OerGqU35jKjgpDUKdJBZSDm5xnCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0e997ef7891d7c9d73329259e0d50aa0c6c36c160be40252373ce0ef3bb0f1a4","last_reissued_at":"2026-07-05T05:31:59.373419Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:31:59.373419Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Shedding light on thermal photon and dilepton production","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Greg Jackson","submitted_at":"2022-11-17T15:00:58Z","abstract_excerpt":"Electromagnetic radiation from the quark-gluon plasma (QGP) is an important observable to be considered in heavy ion collision experiments. I will provide an update on recent advancements from perturbation theory and quenched lattice simulations. The resummed next-to-leading order (NLO) emission rate has recently been decomposed into transverse and longitudinal components, and extended to non-zero baryon chemical potential. The associated spectral function has also been tested against the Euclidean correlator, for continuum-extrapolated lattice data (at $\\mu_{\\rm B}=0$)."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2211.09575","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/2211.09575/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":"2211.09575","created_at":"2026-07-05T05:31:59.373484+00:00"},{"alias_kind":"arxiv_version","alias_value":"2211.09575v1","created_at":"2026-07-05T05:31:59.373484+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2211.09575","created_at":"2026-07-05T05:31:59.373484+00:00"},{"alias_kind":"pith_short_12","alias_value":"B2MX554JDV6J","created_at":"2026-07-05T05:31:59.373484+00:00"},{"alias_kind":"pith_short_16","alias_value":"B2MX554JDV6J24ZS","created_at":"2026-07-05T05:31:59.373484+00:00"},{"alias_kind":"pith_short_8","alias_value":"B2MX554J","created_at":"2026-07-05T05:31:59.373484+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.30180","citing_title":"The polarization of thermal dileptons emitted in high-energy heavy-ion collisions","ref_index":48,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/B2MX554JDV6J24ZSSJM6BVIKUD","json":"https://pith.science/pith/B2MX554JDV6J24ZSSJM6BVIKUD.json","graph_json":"https://pith.science/api/pith-number/B2MX554JDV6J24ZSSJM6BVIKUD/graph.json","events_json":"https://pith.science/api/pith-number/B2MX554JDV6J24ZSSJM6BVIKUD/events.json","paper":"https://pith.science/paper/B2MX554J"},"agent_actions":{"view_html":"https://pith.science/pith/B2MX554JDV6J24ZSSJM6BVIKUD","download_json":"https://pith.science/pith/B2MX554JDV6J24ZSSJM6BVIKUD.json","view_paper":"https://pith.science/paper/B2MX554J","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2211.09575&json=true","fetch_graph":"https://pith.science/api/pith-number/B2MX554JDV6J24ZSSJM6BVIKUD/graph.json","fetch_events":"https://pith.science/api/pith-number/B2MX554JDV6J24ZSSJM6BVIKUD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/B2MX554JDV6J24ZSSJM6BVIKUD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/B2MX554JDV6J24ZSSJM6BVIKUD/action/storage_attestation","attest_author":"https://pith.science/pith/B2MX554JDV6J24ZSSJM6BVIKUD/action/author_attestation","sign_citation":"https://pith.science/pith/B2MX554JDV6J24ZSSJM6BVIKUD/action/citation_signature","submit_replication":"https://pith.science/pith/B2MX554JDV6J24ZSSJM6BVIKUD/action/replication_record"}},"created_at":"2026-07-05T05:31:59.373484+00:00","updated_at":"2026-07-05T05:31:59.373484+00:00"}