{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:WC5H5A6FTEF6Q4PTPJPXWG5MJB","short_pith_number":"pith:WC5H5A6F","schema_version":"1.0","canonical_sha256":"b0ba7e83c5990be871f37a5f7b1bac486e22e13491a4379e5ff92f648b5687e6","source":{"kind":"arxiv","id":"1506.08684","version":1},"attestation_state":"computed","paper":{"title":"A gauge invariant Debye mass and the complex heavy-quark potential","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"Alexander Rothkopf, Yannis Burnier","submitted_at":"2015-06-29T15:36:38Z","abstract_excerpt":"Following the original idea of Debye, we define and extract a gauge-invariant screening mass from the complex static in-medium heavy-quark potential $V_{Q\\bar{Q}}$, recently obtained from lattice QCD. To this end we derive a field theoretically motivated analytic formula that faithfully reproduces both the screened real- as well as the imaginary part of the lattice potential with a single temperature dependent fit parameter $m_D(T)$. Using values of the real part of $V_{Q\\bar{Q}}$ in a gluonic medium, we obtain Debye masses compatible with predictions from HTL perturbation theory."},"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":"1506.08684","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-06-29T15:36:38Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"2f63481348753487a7570d24b61c03727e355f51590b6f8abcae152b783b4415","abstract_canon_sha256":"e5719787a3c3ab93156a11b168c31d43ad9b791bce8e169ce699c66ccda4d58c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:49:25.232903Z","signature_b64":"0r6IZa4Pp+u8L8lYc3RZ3N388ahqKGuc618tDvuaRCoCOE1mTXa08Y8ItezK3CPymhS/GhKG5ritWVZiHdjaCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b0ba7e83c5990be871f37a5f7b1bac486e22e13491a4379e5ff92f648b5687e6","last_reissued_at":"2026-05-18T00:49:25.232261Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:49:25.232261Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A gauge invariant Debye mass and the complex heavy-quark potential","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"Alexander Rothkopf, Yannis Burnier","submitted_at":"2015-06-29T15:36:38Z","abstract_excerpt":"Following the original idea of Debye, we define and extract a gauge-invariant screening mass from the complex static in-medium heavy-quark potential $V_{Q\\bar{Q}}$, recently obtained from lattice QCD. To this end we derive a field theoretically motivated analytic formula that faithfully reproduces both the screened real- as well as the imaginary part of the lattice potential with a single temperature dependent fit parameter $m_D(T)$. Using values of the real part of $V_{Q\\bar{Q}}$ in a gluonic medium, we obtain Debye masses compatible with predictions from HTL perturbation theory."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1506.08684","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":""},"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":"1506.08684","created_at":"2026-05-18T00:49:25.232390+00:00"},{"alias_kind":"arxiv_version","alias_value":"1506.08684v1","created_at":"2026-05-18T00:49:25.232390+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1506.08684","created_at":"2026-05-18T00:49:25.232390+00:00"},{"alias_kind":"pith_short_12","alias_value":"WC5H5A6FTEF6","created_at":"2026-05-18T12:29:47.479230+00:00"},{"alias_kind":"pith_short_16","alias_value":"WC5H5A6FTEF6Q4PT","created_at":"2026-05-18T12:29:47.479230+00:00"},{"alias_kind":"pith_short_8","alias_value":"WC5H5A6F","created_at":"2026-05-18T12:29:47.479230+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.10889","citing_title":"Heavy-quark transport across the QCD crossover driven by a lattice-constrained in-medium potential","ref_index":29,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WC5H5A6FTEF6Q4PTPJPXWG5MJB","json":"https://pith.science/pith/WC5H5A6FTEF6Q4PTPJPXWG5MJB.json","graph_json":"https://pith.science/api/pith-number/WC5H5A6FTEF6Q4PTPJPXWG5MJB/graph.json","events_json":"https://pith.science/api/pith-number/WC5H5A6FTEF6Q4PTPJPXWG5MJB/events.json","paper":"https://pith.science/paper/WC5H5A6F"},"agent_actions":{"view_html":"https://pith.science/pith/WC5H5A6FTEF6Q4PTPJPXWG5MJB","download_json":"https://pith.science/pith/WC5H5A6FTEF6Q4PTPJPXWG5MJB.json","view_paper":"https://pith.science/paper/WC5H5A6F","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1506.08684&json=true","fetch_graph":"https://pith.science/api/pith-number/WC5H5A6FTEF6Q4PTPJPXWG5MJB/graph.json","fetch_events":"https://pith.science/api/pith-number/WC5H5A6FTEF6Q4PTPJPXWG5MJB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WC5H5A6FTEF6Q4PTPJPXWG5MJB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WC5H5A6FTEF6Q4PTPJPXWG5MJB/action/storage_attestation","attest_author":"https://pith.science/pith/WC5H5A6FTEF6Q4PTPJPXWG5MJB/action/author_attestation","sign_citation":"https://pith.science/pith/WC5H5A6FTEF6Q4PTPJPXWG5MJB/action/citation_signature","submit_replication":"https://pith.science/pith/WC5H5A6FTEF6Q4PTPJPXWG5MJB/action/replication_record"}},"created_at":"2026-05-18T00:49:25.232390+00:00","updated_at":"2026-05-18T00:49:25.232390+00:00"}