{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2000:FGYEC733N2PTJH4TBYUUDRRDW4","short_pith_number":"pith:FGYEC733","schema_version":"1.0","canonical_sha256":"29b0417f7b6e9f349f930e2941c623b706d158750ed20ac50be073bc4b5a2e48","source":{"kind":"arxiv","id":"hep-ph/0007093","version":2},"attestation_state":"computed","paper":{"title":"Finite Temperature Meson Correlation Functions in HTL Approximation","license":"","headline":"","cross_cats":["hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"F. Karsch, M. G. Mustafa, M. H. Thoma","submitted_at":"2000-07-11T09:15:09Z","abstract_excerpt":"We calculate temporal correlators and their spectral functions with meson quantum numbers in the deconfined phase of QCD using the hard thermal loop (HTL) approximation for the quark propagator. Although this approach does not result in a complete next-to-leading order perturbative calculation it takes into account important medium effects such as thermal quark masses and Landau damping in the quark-gluon plasma. We show that both effects lead to competing modifications of the free mesonic correlation functions. We find that correlators in scalar channels are only moderately influenced by the "},"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":"hep-ph/0007093","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2000-07-11T09:15:09Z","cross_cats_sorted":["hep-lat","nucl-th"],"title_canon_sha256":"45d23f498f27e75277666145e0461f34b88e810190bbe6179c23e27e15dbf56b","abstract_canon_sha256":"23853625dea1f4f015a2d60364a29016c932c9b9ce2f62f885098481d15dbfc9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:20:14.205265Z","signature_b64":"XVuv8ptJwxyO5VXIxosaSjS/JVKpGRA0/g/gJms24nhcCCn1+sEP9UvX7qajpBretS0O1D0EsIaLgFMQ2r0pDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"29b0417f7b6e9f349f930e2941c623b706d158750ed20ac50be073bc4b5a2e48","last_reissued_at":"2026-07-04T16:20:14.204871Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:20:14.204871Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Finite Temperature Meson Correlation Functions in HTL Approximation","license":"","headline":"","cross_cats":["hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"F. Karsch, M. G. Mustafa, M. H. Thoma","submitted_at":"2000-07-11T09:15:09Z","abstract_excerpt":"We calculate temporal correlators and their spectral functions with meson quantum numbers in the deconfined phase of QCD using the hard thermal loop (HTL) approximation for the quark propagator. Although this approach does not result in a complete next-to-leading order perturbative calculation it takes into account important medium effects such as thermal quark masses and Landau damping in the quark-gluon plasma. We show that both effects lead to competing modifications of the free mesonic correlation functions. We find that correlators in scalar channels are only moderately influenced by the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0007093","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/hep-ph/0007093/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":"hep-ph/0007093","created_at":"2026-07-04T16:20:14.204948+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0007093v2","created_at":"2026-07-04T16:20:14.204948+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0007093","created_at":"2026-07-04T16:20:14.204948+00:00"},{"alias_kind":"pith_short_12","alias_value":"FGYEC733N2PT","created_at":"2026-07-04T16:20:14.204948+00:00"},{"alias_kind":"pith_short_16","alias_value":"FGYEC733N2PTJH4T","created_at":"2026-07-04T16:20:14.204948+00:00"},{"alias_kind":"pith_short_8","alias_value":"FGYEC733","created_at":"2026-07-04T16:20:14.204948+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1907.03990","citing_title":"Effect of anomalous magnetic moment of quarks on the phase structure and mesonic properties in the NJL model","ref_index":79,"is_internal_anchor":true},{"citing_arxiv_id":"2604.21633","citing_title":"Dilepton Production as a Probe of Pion Condensation in Hot and Dense QCD Matter","ref_index":53,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FGYEC733N2PTJH4TBYUUDRRDW4","json":"https://pith.science/pith/FGYEC733N2PTJH4TBYUUDRRDW4.json","graph_json":"https://pith.science/api/pith-number/FGYEC733N2PTJH4TBYUUDRRDW4/graph.json","events_json":"https://pith.science/api/pith-number/FGYEC733N2PTJH4TBYUUDRRDW4/events.json","paper":"https://pith.science/paper/FGYEC733"},"agent_actions":{"view_html":"https://pith.science/pith/FGYEC733N2PTJH4TBYUUDRRDW4","download_json":"https://pith.science/pith/FGYEC733N2PTJH4TBYUUDRRDW4.json","view_paper":"https://pith.science/paper/FGYEC733","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0007093&json=true","fetch_graph":"https://pith.science/api/pith-number/FGYEC733N2PTJH4TBYUUDRRDW4/graph.json","fetch_events":"https://pith.science/api/pith-number/FGYEC733N2PTJH4TBYUUDRRDW4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FGYEC733N2PTJH4TBYUUDRRDW4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FGYEC733N2PTJH4TBYUUDRRDW4/action/storage_attestation","attest_author":"https://pith.science/pith/FGYEC733N2PTJH4TBYUUDRRDW4/action/author_attestation","sign_citation":"https://pith.science/pith/FGYEC733N2PTJH4TBYUUDRRDW4/action/citation_signature","submit_replication":"https://pith.science/pith/FGYEC733N2PTJH4TBYUUDRRDW4/action/replication_record"}},"created_at":"2026-07-04T16:20:14.204948+00:00","updated_at":"2026-07-04T16:20:14.204948+00:00"}