{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:R2F4LCUAAJAF3SK4CT5H23NJQX","short_pith_number":"pith:R2F4LCUA","schema_version":"1.0","canonical_sha256":"8e8bc58a8002405dc95c14fa7d6da985fd96a4f1d2a1cc26d22b094df8791889","source":{"kind":"arxiv","id":"hep-th/0105039","version":3},"attestation_state":"computed","paper":{"title":"Hidden functional relation in Large-N Quark-Monopole system at finite temperature","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"D. K. Park","submitted_at":"2001-05-03T19:12:18Z","abstract_excerpt":"The quark-monopole potential is computed at finite temperature in the context of $AdS/CFT$ correspondence. It is found that the potential is invariant under $g \\to 1/g$ and $U_T \\to U_T / g$. As in the quark-quark case there exists a maximum separation between quark and monopole, and $L$-dependence of the potential exhibits a bifurcation behavior. We find a functional relation $dE_{QM}^{Reg} / dL = [(1/E_{(1,0)}^{Reg}(U_0))^2 + (1/E_{(0,1)}^{Reg}(U_0))^2]^{-1/2}$ which is responsible for the bifurcation. The remarkable property of this relation is that it makes a relation between physical quan"},"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/0105039","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2001-05-03T19:12:18Z","cross_cats_sorted":[],"title_canon_sha256":"9f67cba042a752426c3f5e0fc11b171a014a75467db9a23dde576b80b6f205e2","abstract_canon_sha256":"06adb45b5dc54395d703d06a197e00624498eb506847d8226c7552e0c2083f6f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:27:51.734841Z","signature_b64":"5reV6SvaFM0du2a3nJxvsyepnj0hbeCTMRr5RFqiUKxL1bWu0BEqkYzo8niWHHlNTlUs9gXhf/Z6gWToALkpAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8e8bc58a8002405dc95c14fa7d6da985fd96a4f1d2a1cc26d22b094df8791889","last_reissued_at":"2026-07-04T16:27:51.734485Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:27:51.734485Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hidden functional relation in Large-N Quark-Monopole system at finite temperature","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"D. K. Park","submitted_at":"2001-05-03T19:12:18Z","abstract_excerpt":"The quark-monopole potential is computed at finite temperature in the context of $AdS/CFT$ correspondence. It is found that the potential is invariant under $g \\to 1/g$ and $U_T \\to U_T / g$. As in the quark-quark case there exists a maximum separation between quark and monopole, and $L$-dependence of the potential exhibits a bifurcation behavior. We find a functional relation $dE_{QM}^{Reg} / dL = [(1/E_{(1,0)}^{Reg}(U_0))^2 + (1/E_{(0,1)}^{Reg}(U_0))^2]^{-1/2}$ which is responsible for the bifurcation. The remarkable property of this relation is that it makes a relation between physical quan"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0105039","kind":"arxiv","version":3},"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-th/0105039/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-th/0105039","created_at":"2026-07-04T16:27:51.734536+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0105039v3","created_at":"2026-07-04T16:27:51.734536+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0105039","created_at":"2026-07-04T16:27:51.734536+00:00"},{"alias_kind":"pith_short_12","alias_value":"R2F4LCUAAJAF","created_at":"2026-07-04T16:27:51.734536+00:00"},{"alias_kind":"pith_short_16","alias_value":"R2F4LCUAAJAF3SK4","created_at":"2026-07-04T16:27:51.734536+00:00"},{"alias_kind":"pith_short_8","alias_value":"R2F4LCUA","created_at":"2026-07-04T16:27:51.734536+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.08391","citing_title":"A Simple Model of Superconductors: Insights from Free Fermion and Boson Gases","ref_index":12,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/R2F4LCUAAJAF3SK4CT5H23NJQX","json":"https://pith.science/pith/R2F4LCUAAJAF3SK4CT5H23NJQX.json","graph_json":"https://pith.science/api/pith-number/R2F4LCUAAJAF3SK4CT5H23NJQX/graph.json","events_json":"https://pith.science/api/pith-number/R2F4LCUAAJAF3SK4CT5H23NJQX/events.json","paper":"https://pith.science/paper/R2F4LCUA"},"agent_actions":{"view_html":"https://pith.science/pith/R2F4LCUAAJAF3SK4CT5H23NJQX","download_json":"https://pith.science/pith/R2F4LCUAAJAF3SK4CT5H23NJQX.json","view_paper":"https://pith.science/paper/R2F4LCUA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0105039&json=true","fetch_graph":"https://pith.science/api/pith-number/R2F4LCUAAJAF3SK4CT5H23NJQX/graph.json","fetch_events":"https://pith.science/api/pith-number/R2F4LCUAAJAF3SK4CT5H23NJQX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/R2F4LCUAAJAF3SK4CT5H23NJQX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/R2F4LCUAAJAF3SK4CT5H23NJQX/action/storage_attestation","attest_author":"https://pith.science/pith/R2F4LCUAAJAF3SK4CT5H23NJQX/action/author_attestation","sign_citation":"https://pith.science/pith/R2F4LCUAAJAF3SK4CT5H23NJQX/action/citation_signature","submit_replication":"https://pith.science/pith/R2F4LCUAAJAF3SK4CT5H23NJQX/action/replication_record"}},"created_at":"2026-07-04T16:27:51.734536+00:00","updated_at":"2026-07-04T16:27:51.734536+00:00"}