{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:57LTMBUILXJ2GL7FKJLM2FKYEM","short_pith_number":"pith:57LTMBUI","schema_version":"1.0","canonical_sha256":"efd73606885dd3a32fe55256cd15582304334b3c0db8d571d49e486ebf3a9688","source":{"kind":"arxiv","id":"hep-th/9803135","version":2},"attestation_state":"computed","paper":{"title":"Wilson-Polyakov Loop at Finite Temperature in Large N Gauge Theory and Anti-de Sitter Supergravity","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Jung-Tay Yee, Soo-Jong Rey, Stefan Theisen","submitted_at":"1998-03-18T00:51:17Z","abstract_excerpt":"Aspects of d=4, N=4 superconformal U(N) gauge theory are studied at finite temperature. Utilizing dual description of large $N$ and strong coupling limit via Type IIB string theory compactification on Schwarzschild anti-de Sitter spacetime, we study correlations of Wilson-Polyakov loops and heavy quark potential thereof. We find that the heavy quark potential is Coulomb-like and has a finite range, as expected for gauge theory in high temperature, deconfinement phase. The potential exhibits finite temperature scaling consistent with underlying conformal invariance. We also study isolated heavy"},"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-th/9803135","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1998-03-18T00:51:17Z","cross_cats_sorted":[],"title_canon_sha256":"bee5b2e01e0646e3c5d96eb0b8a3cbd9accebef4807bd1c74b4cf4bda5c0d71c","abstract_canon_sha256":"b448b96b60f6dfaecf771d782b761b8044617263a74a0721b771bc6d96537b3f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:28:46.026437Z","signature_b64":"ND7JHAnEvw6QVYBazygSA2WdcGfrQZ+JjVGbsPJPWop3E/R15Q8OkSExdodlMjUefJtR+k94YWDgYFfXdLNXBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"efd73606885dd3a32fe55256cd15582304334b3c0db8d571d49e486ebf3a9688","last_reissued_at":"2026-05-18T04:28:46.025707Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:28:46.025707Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Wilson-Polyakov Loop at Finite Temperature in Large N Gauge Theory and Anti-de Sitter Supergravity","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Jung-Tay Yee, Soo-Jong Rey, Stefan Theisen","submitted_at":"1998-03-18T00:51:17Z","abstract_excerpt":"Aspects of d=4, N=4 superconformal U(N) gauge theory are studied at finite temperature. Utilizing dual description of large $N$ and strong coupling limit via Type IIB string theory compactification on Schwarzschild anti-de Sitter spacetime, we study correlations of Wilson-Polyakov loops and heavy quark potential thereof. We find that the heavy quark potential is Coulomb-like and has a finite range, as expected for gauge theory in high temperature, deconfinement phase. The potential exhibits finite temperature scaling consistent with underlying conformal invariance. We also study isolated heavy"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9803135","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-th/9803135","created_at":"2026-05-18T04:28:46.025815+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9803135v2","created_at":"2026-05-18T04:28:46.025815+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9803135","created_at":"2026-05-18T04:28:46.025815+00:00"},{"alias_kind":"pith_short_12","alias_value":"57LTMBUILXJ2","created_at":"2026-05-18T12:25:49.038998+00:00"},{"alias_kind":"pith_short_16","alias_value":"57LTMBUILXJ2GL7F","created_at":"2026-05-18T12:25:49.038998+00:00"},{"alias_kind":"pith_short_8","alias_value":"57LTMBUI","created_at":"2026-05-18T12:25:49.038998+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2512.05514","citing_title":"Wilson loops on the Coulomb branch of $N=4$ super-Yang-Mills","ref_index":11,"is_internal_anchor":true},{"citing_arxiv_id":"2601.11136","citing_title":"Confinement and chiral symmetry breaking in holography: a smooth switch-off","ref_index":20,"is_internal_anchor":true},{"citing_arxiv_id":"2604.20498","citing_title":"Anisotropic drag force in finite-density QGP from charged rotating 5D black holes","ref_index":47,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/57LTMBUILXJ2GL7FKJLM2FKYEM","json":"https://pith.science/pith/57LTMBUILXJ2GL7FKJLM2FKYEM.json","graph_json":"https://pith.science/api/pith-number/57LTMBUILXJ2GL7FKJLM2FKYEM/graph.json","events_json":"https://pith.science/api/pith-number/57LTMBUILXJ2GL7FKJLM2FKYEM/events.json","paper":"https://pith.science/paper/57LTMBUI"},"agent_actions":{"view_html":"https://pith.science/pith/57LTMBUILXJ2GL7FKJLM2FKYEM","download_json":"https://pith.science/pith/57LTMBUILXJ2GL7FKJLM2FKYEM.json","view_paper":"https://pith.science/paper/57LTMBUI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9803135&json=true","fetch_graph":"https://pith.science/api/pith-number/57LTMBUILXJ2GL7FKJLM2FKYEM/graph.json","fetch_events":"https://pith.science/api/pith-number/57LTMBUILXJ2GL7FKJLM2FKYEM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/57LTMBUILXJ2GL7FKJLM2FKYEM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/57LTMBUILXJ2GL7FKJLM2FKYEM/action/storage_attestation","attest_author":"https://pith.science/pith/57LTMBUILXJ2GL7FKJLM2FKYEM/action/author_attestation","sign_citation":"https://pith.science/pith/57LTMBUILXJ2GL7FKJLM2FKYEM/action/citation_signature","submit_replication":"https://pith.science/pith/57LTMBUILXJ2GL7FKJLM2FKYEM/action/replication_record"}},"created_at":"2026-05-18T04:28:46.025815+00:00","updated_at":"2026-05-18T04:28:46.025815+00:00"}