{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:XA5BYF24QRJ55HBCA35HWGFUQE","short_pith_number":"pith:XA5BYF24","schema_version":"1.0","canonical_sha256":"b83a1c175c8453de9c2206fa7b18b481197c65d78c8e21edfc03f2ba2679d0a7","source":{"kind":"arxiv","id":"2304.09187","version":2},"attestation_state":"computed","paper":{"title":"Soft gluon self-energy at finite temperature and density: hard NLO corrections in general covariant gauge","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Kaapo Sepp\\\"anen, Risto Paatelainen, Saga S\\\"appi, Tyler Gorda","submitted_at":"2023-04-18T18:00:00Z","abstract_excerpt":"We compute the next-to-leading order (NLO) hard correction to the gluon self-energy tensor with arbitrary soft momenta in a hot and/or dense weakly coupled plasma in Quantum Chromodynamics. Our diagrammatic computations of the two-loop and power corrections are performed within the hard-thermal-loop (HTL) framework and in general covariant gauge, using the real-time formalism. We find that after renormalization our individual results are finite and gauge-dependent, and they reproduce previously computed results in Quantum Electrodynamics in the appropriate limit. Combining our results, we also"},"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":"2304.09187","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2023-04-18T18:00:00Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"767bc872bb205c2461b076e07942622996fcd48454a6385fc59df26adfffc941","abstract_canon_sha256":"c918e418cd19a6cf02f4a273f48e8d0133c48e7ae889e1f77d90bb7e1acd151c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:11:55.290433Z","signature_b64":"f/BeBB1QU4/VsqOAjexoGBta7Q14zK4JnqgI8FbSAJL5w/IP4boKMfzGSpp5lTMZ9si4IKDnIyV4PEEuV7raCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b83a1c175c8453de9c2206fa7b18b481197c65d78c8e21edfc03f2ba2679d0a7","last_reissued_at":"2026-07-05T07:11:55.289952Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:11:55.289952Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Soft gluon self-energy at finite temperature and density: hard NLO corrections in general covariant gauge","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Kaapo Sepp\\\"anen, Risto Paatelainen, Saga S\\\"appi, Tyler Gorda","submitted_at":"2023-04-18T18:00:00Z","abstract_excerpt":"We compute the next-to-leading order (NLO) hard correction to the gluon self-energy tensor with arbitrary soft momenta in a hot and/or dense weakly coupled plasma in Quantum Chromodynamics. Our diagrammatic computations of the two-loop and power corrections are performed within the hard-thermal-loop (HTL) framework and in general covariant gauge, using the real-time formalism. We find that after renormalization our individual results are finite and gauge-dependent, and they reproduce previously computed results in Quantum Electrodynamics in the appropriate limit. Combining our results, we also"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2304.09187","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/2304.09187/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":"2304.09187","created_at":"2026-07-05T07:11:55.290010+00:00"},{"alias_kind":"arxiv_version","alias_value":"2304.09187v2","created_at":"2026-07-05T07:11:55.290010+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2304.09187","created_at":"2026-07-05T07:11:55.290010+00:00"},{"alias_kind":"pith_short_12","alias_value":"XA5BYF24QRJ5","created_at":"2026-07-05T07:11:55.290010+00:00"},{"alias_kind":"pith_short_16","alias_value":"XA5BYF24QRJ55HBC","created_at":"2026-07-05T07:11:55.290010+00:00"},{"alias_kind":"pith_short_8","alias_value":"XA5BYF24","created_at":"2026-07-05T07:11:55.290010+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.17090","citing_title":"Non-extensive Hard Thermal Loop Resummation and Its Applications: Analysis in Zero and Finite Magnetic Fields","ref_index":90,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XA5BYF24QRJ55HBCA35HWGFUQE","json":"https://pith.science/pith/XA5BYF24QRJ55HBCA35HWGFUQE.json","graph_json":"https://pith.science/api/pith-number/XA5BYF24QRJ55HBCA35HWGFUQE/graph.json","events_json":"https://pith.science/api/pith-number/XA5BYF24QRJ55HBCA35HWGFUQE/events.json","paper":"https://pith.science/paper/XA5BYF24"},"agent_actions":{"view_html":"https://pith.science/pith/XA5BYF24QRJ55HBCA35HWGFUQE","download_json":"https://pith.science/pith/XA5BYF24QRJ55HBCA35HWGFUQE.json","view_paper":"https://pith.science/paper/XA5BYF24","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2304.09187&json=true","fetch_graph":"https://pith.science/api/pith-number/XA5BYF24QRJ55HBCA35HWGFUQE/graph.json","fetch_events":"https://pith.science/api/pith-number/XA5BYF24QRJ55HBCA35HWGFUQE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XA5BYF24QRJ55HBCA35HWGFUQE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XA5BYF24QRJ55HBCA35HWGFUQE/action/storage_attestation","attest_author":"https://pith.science/pith/XA5BYF24QRJ55HBCA35HWGFUQE/action/author_attestation","sign_citation":"https://pith.science/pith/XA5BYF24QRJ55HBCA35HWGFUQE/action/citation_signature","submit_replication":"https://pith.science/pith/XA5BYF24QRJ55HBCA35HWGFUQE/action/replication_record"}},"created_at":"2026-07-05T07:11:55.290010+00:00","updated_at":"2026-07-05T07:11:55.290010+00:00"}