{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1997:W45WE5VKY5U4KAPFMWQ2Z5X5ZQ","short_pith_number":"pith:W45WE5VK","schema_version":"1.0","canonical_sha256":"b73b6276aac769c501e565a1acf6fdcc02314d096fd6063e51f8f3630889e7dd","source":{"kind":"arxiv","id":"hep-ph/9701354","version":2},"attestation_state":"computed","paper":{"title":"Production of energetic dileptons with small invariant masses from the quark-gluon plasma","license":"","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"C.T. Traxler (Univ. Giessen), M.H. Thoma","submitted_at":"1997-01-23T10:43:24Z","abstract_excerpt":"The resummation technique of Braaten and Pisarski is used for a complete calculation of the $\\alpha^2 \\alpha_s$-contribution to the production rate of dileptons with energy E >> T and invariant mass M <~ T from a quark-gluon plasma. In particular the cancellation of the infrared singularity by medium effects is discussed in detail."},"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/9701354","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1997-01-23T10:43:24Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"d4ecb25efea2083a0e694a9c4c0052acc47cb0d520ac13c0334ce5d27edfb56d","abstract_canon_sha256":"c5cdac145ea4f6c7e57de91db58269c434e06f78370bfe1164827a5872191211"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:08:05.379243Z","signature_b64":"ZaYsawTot05xfoCq7LK+RSUSQONntNch0J3TnX1CTybfdTARZ2PyeI8Huhqps+vlZA84eafQKgmQggl8qDUiCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b73b6276aac769c501e565a1acf6fdcc02314d096fd6063e51f8f3630889e7dd","last_reissued_at":"2026-05-18T01:08:05.378828Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:08:05.378828Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Production of energetic dileptons with small invariant masses from the quark-gluon plasma","license":"","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"C.T. Traxler (Univ. Giessen), M.H. Thoma","submitted_at":"1997-01-23T10:43:24Z","abstract_excerpt":"The resummation technique of Braaten and Pisarski is used for a complete calculation of the $\\alpha^2 \\alpha_s$-contribution to the production rate of dileptons with energy E >> T and invariant mass M <~ T from a quark-gluon plasma. In particular the cancellation of the infrared singularity by medium effects is discussed in detail."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9701354","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":"hep-ph/9701354","created_at":"2026-05-18T01:08:05.378904+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9701354v2","created_at":"2026-05-18T01:08:05.378904+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9701354","created_at":"2026-05-18T01:08:05.378904+00:00"},{"alias_kind":"pith_short_12","alias_value":"W45WE5VKY5U4","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_16","alias_value":"W45WE5VKY5U4KAPF","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_8","alias_value":"W45WE5VK","created_at":"2026-05-18T12:25:48.327863+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/W45WE5VKY5U4KAPFMWQ2Z5X5ZQ","json":"https://pith.science/pith/W45WE5VKY5U4KAPFMWQ2Z5X5ZQ.json","graph_json":"https://pith.science/api/pith-number/W45WE5VKY5U4KAPFMWQ2Z5X5ZQ/graph.json","events_json":"https://pith.science/api/pith-number/W45WE5VKY5U4KAPFMWQ2Z5X5ZQ/events.json","paper":"https://pith.science/paper/W45WE5VK"},"agent_actions":{"view_html":"https://pith.science/pith/W45WE5VKY5U4KAPFMWQ2Z5X5ZQ","download_json":"https://pith.science/pith/W45WE5VKY5U4KAPFMWQ2Z5X5ZQ.json","view_paper":"https://pith.science/paper/W45WE5VK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9701354&json=true","fetch_graph":"https://pith.science/api/pith-number/W45WE5VKY5U4KAPFMWQ2Z5X5ZQ/graph.json","fetch_events":"https://pith.science/api/pith-number/W45WE5VKY5U4KAPFMWQ2Z5X5ZQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/W45WE5VKY5U4KAPFMWQ2Z5X5ZQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/W45WE5VKY5U4KAPFMWQ2Z5X5ZQ/action/storage_attestation","attest_author":"https://pith.science/pith/W45WE5VKY5U4KAPFMWQ2Z5X5ZQ/action/author_attestation","sign_citation":"https://pith.science/pith/W45WE5VKY5U4KAPFMWQ2Z5X5ZQ/action/citation_signature","submit_replication":"https://pith.science/pith/W45WE5VKY5U4KAPFMWQ2Z5X5ZQ/action/replication_record"}},"created_at":"2026-05-18T01:08:05.378904+00:00","updated_at":"2026-05-18T01:08:05.378904+00:00"}