{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:5MHK2SGHVW2R4YSJ6K3L7QKVA2","short_pith_number":"pith:5MHK2SGH","schema_version":"1.0","canonical_sha256":"eb0ead48c7adb51e6249f2b6bfc15506a3a9d8e6c98d03a6b433fb9d922667fa","source":{"kind":"arxiv","id":"1105.5144","version":1},"attestation_state":"computed","paper":{"title":"Generalized quark-antiquark potential at weak and strong coupling","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Nadav Drukker, Valentina Forini","submitted_at":"2011-05-25T20:05:23Z","abstract_excerpt":"We study a two-parameter family of Wilson loop operators in N=4 supersymmetric Yang-Mills theory which interpolates smoothly between the 1/2 BPS line or circle and a pair of antiparallel lines. These observables capture a natural generalization of the quark-antiquark potential. We calculate these loops on the gauge theory side to second order in perturbation theory and in a semiclassical expansion in string theory to one-loop order. The resulting determinants are given in integral form and can be evaluated numerically for general values of the parameters or analytically in a systematic expansi"},"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":"1105.5144","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-05-25T20:05:23Z","cross_cats_sorted":[],"title_canon_sha256":"b0136ddddd46ddd46f3987e6609c662d079ea69ac56c185dd51fc720f136dc75","abstract_canon_sha256":"a81af09dd5c33c162d299bb21c15e238036de8503e2890c3c70565a3d2e8238a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:01:50.727516Z","signature_b64":"g75SLXEekTsMPfYdY96ygdBJ7zOLlLCc5NYywk9ra1Jda6wK4wQtwp99ebr0FT9Cu1WEFy2ghRK24sySU7p8Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"eb0ead48c7adb51e6249f2b6bfc15506a3a9d8e6c98d03a6b433fb9d922667fa","last_reissued_at":"2026-05-18T02:01:50.726925Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:01:50.726925Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Generalized quark-antiquark potential at weak and strong coupling","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Nadav Drukker, Valentina Forini","submitted_at":"2011-05-25T20:05:23Z","abstract_excerpt":"We study a two-parameter family of Wilson loop operators in N=4 supersymmetric Yang-Mills theory which interpolates smoothly between the 1/2 BPS line or circle and a pair of antiparallel lines. These observables capture a natural generalization of the quark-antiquark potential. We calculate these loops on the gauge theory side to second order in perturbation theory and in a semiclassical expansion in string theory to one-loop order. The resulting determinants are given in integral form and can be evaluated numerically for general values of the parameters or analytically in a systematic expansi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.5144","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":"1105.5144","created_at":"2026-05-18T02:01:50.727002+00:00"},{"alias_kind":"arxiv_version","alias_value":"1105.5144v1","created_at":"2026-05-18T02:01:50.727002+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.5144","created_at":"2026-05-18T02:01:50.727002+00:00"},{"alias_kind":"pith_short_12","alias_value":"5MHK2SGHVW2R","created_at":"2026-05-18T12:26:20.644004+00:00"},{"alias_kind":"pith_short_16","alias_value":"5MHK2SGHVW2R4YSJ","created_at":"2026-05-18T12:26:20.644004+00:00"},{"alias_kind":"pith_short_8","alias_value":"5MHK2SGH","created_at":"2026-05-18T12:26:20.644004+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/5MHK2SGHVW2R4YSJ6K3L7QKVA2","json":"https://pith.science/pith/5MHK2SGHVW2R4YSJ6K3L7QKVA2.json","graph_json":"https://pith.science/api/pith-number/5MHK2SGHVW2R4YSJ6K3L7QKVA2/graph.json","events_json":"https://pith.science/api/pith-number/5MHK2SGHVW2R4YSJ6K3L7QKVA2/events.json","paper":"https://pith.science/paper/5MHK2SGH"},"agent_actions":{"view_html":"https://pith.science/pith/5MHK2SGHVW2R4YSJ6K3L7QKVA2","download_json":"https://pith.science/pith/5MHK2SGHVW2R4YSJ6K3L7QKVA2.json","view_paper":"https://pith.science/paper/5MHK2SGH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1105.5144&json=true","fetch_graph":"https://pith.science/api/pith-number/5MHK2SGHVW2R4YSJ6K3L7QKVA2/graph.json","fetch_events":"https://pith.science/api/pith-number/5MHK2SGHVW2R4YSJ6K3L7QKVA2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5MHK2SGHVW2R4YSJ6K3L7QKVA2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5MHK2SGHVW2R4YSJ6K3L7QKVA2/action/storage_attestation","attest_author":"https://pith.science/pith/5MHK2SGHVW2R4YSJ6K3L7QKVA2/action/author_attestation","sign_citation":"https://pith.science/pith/5MHK2SGHVW2R4YSJ6K3L7QKVA2/action/citation_signature","submit_replication":"https://pith.science/pith/5MHK2SGHVW2R4YSJ6K3L7QKVA2/action/replication_record"}},"created_at":"2026-05-18T02:01:50.727002+00:00","updated_at":"2026-05-18T02:01:50.727002+00:00"}