{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:KUQPHQDB7GTXXPSGNTQJPSVNOK","short_pith_number":"pith:KUQPHQDB","schema_version":"1.0","canonical_sha256":"5520f3c061f9a77bbe466ce097caad7282b3f389e41638cdbb2bfab30616a408","source":{"kind":"arxiv","id":"hep-ph/0611300","version":2},"attestation_state":"computed","paper":{"title":"Real-time static potential in hot QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"M. Laine, M. Tassler, O. Philipsen, P. Romatschke","submitted_at":"2006-11-23T16:00:10Z","abstract_excerpt":"We derive a static potential for a heavy quark-antiquark pair propagating in Minkowski time at finite temperature, by defining a suitable gauge-invariant Green's function and computing it to first non-trivial order in Hard Thermal Loop resummed perturbation theory. The resulting Debye-screened potential could be used in models that attempt to describe the ``melting'' of heavy quarkonium at high temperatures. We show, in particular, that the potential develops an imaginary part, implying that thermal effects generate a finite width for the quarkonium peak in the dilepton production rate. For qu"},"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/0611300","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2006-11-23T16:00:10Z","cross_cats_sorted":[],"title_canon_sha256":"c795a739c439a1bf58635b05a06eb358a1ec47d12280b79ea78a2d89f62857b9","abstract_canon_sha256":"6a4d3e96c3dd6842dc9f4ede5e6472851728024bd0fc45406c2157937ac41b82"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:38:27.446339Z","signature_b64":"mUXWaNgBSeXmU3odmSe5TvjMtF7FZIkw40N0YhsUyYYVA6TLWgV9IUliDvwrG36nOCeH4APzZlppnj9/lA5+BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5520f3c061f9a77bbe466ce097caad7282b3f389e41638cdbb2bfab30616a408","last_reissued_at":"2026-05-18T04:38:27.445902Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:38:27.445902Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Real-time static potential in hot QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"M. Laine, M. Tassler, O. Philipsen, P. Romatschke","submitted_at":"2006-11-23T16:00:10Z","abstract_excerpt":"We derive a static potential for a heavy quark-antiquark pair propagating in Minkowski time at finite temperature, by defining a suitable gauge-invariant Green's function and computing it to first non-trivial order in Hard Thermal Loop resummed perturbation theory. The resulting Debye-screened potential could be used in models that attempt to describe the ``melting'' of heavy quarkonium at high temperatures. We show, in particular, that the potential develops an imaginary part, implying that thermal effects generate a finite width for the quarkonium peak in the dilepton production rate. For qu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0611300","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/0611300","created_at":"2026-05-18T04:38:27.445966+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0611300v2","created_at":"2026-05-18T04:38:27.445966+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0611300","created_at":"2026-05-18T04:38:27.445966+00:00"},{"alias_kind":"pith_short_12","alias_value":"KUQPHQDB7GTX","created_at":"2026-05-18T12:25:54.717736+00:00"},{"alias_kind":"pith_short_16","alias_value":"KUQPHQDB7GTXXPSG","created_at":"2026-05-18T12:25:54.717736+00:00"},{"alias_kind":"pith_short_8","alias_value":"KUQPHQDB","created_at":"2026-05-18T12:25:54.717736+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.20034","citing_title":"Charmonium properties at high temperatures from lattice QCD","ref_index":8,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KUQPHQDB7GTXXPSGNTQJPSVNOK","json":"https://pith.science/pith/KUQPHQDB7GTXXPSGNTQJPSVNOK.json","graph_json":"https://pith.science/api/pith-number/KUQPHQDB7GTXXPSGNTQJPSVNOK/graph.json","events_json":"https://pith.science/api/pith-number/KUQPHQDB7GTXXPSGNTQJPSVNOK/events.json","paper":"https://pith.science/paper/KUQPHQDB"},"agent_actions":{"view_html":"https://pith.science/pith/KUQPHQDB7GTXXPSGNTQJPSVNOK","download_json":"https://pith.science/pith/KUQPHQDB7GTXXPSGNTQJPSVNOK.json","view_paper":"https://pith.science/paper/KUQPHQDB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0611300&json=true","fetch_graph":"https://pith.science/api/pith-number/KUQPHQDB7GTXXPSGNTQJPSVNOK/graph.json","fetch_events":"https://pith.science/api/pith-number/KUQPHQDB7GTXXPSGNTQJPSVNOK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KUQPHQDB7GTXXPSGNTQJPSVNOK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KUQPHQDB7GTXXPSGNTQJPSVNOK/action/storage_attestation","attest_author":"https://pith.science/pith/KUQPHQDB7GTXXPSGNTQJPSVNOK/action/author_attestation","sign_citation":"https://pith.science/pith/KUQPHQDB7GTXXPSGNTQJPSVNOK/action/citation_signature","submit_replication":"https://pith.science/pith/KUQPHQDB7GTXXPSGNTQJPSVNOK/action/replication_record"}},"created_at":"2026-05-18T04:38:27.445966+00:00","updated_at":"2026-05-18T04:38:27.445966+00:00"}