{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:66D3QQAAEMU5AFR5WZEEQ6FKLG","short_pith_number":"pith:66D3QQAA","schema_version":"1.0","canonical_sha256":"f787b840002329d0163db6484878aa59be2f5d2b1450640b6f5c5f9a9a1b6cb8","source":{"kind":"arxiv","id":"1201.0129","version":2},"attestation_state":"computed","paper":{"title":"Wilson loops in noncommutative Yang-Mills theory using gauge/gravity duality","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Najmul Haque, Shibaji Roy, Somdeb Chakraborty","submitted_at":"2011-12-30T14:09:22Z","abstract_excerpt":"By using the gauge/gravity duality and the Maldacena prescription we compute the expectation values of the Wilson loops in noncommutative Yang-Mills (NCYM) theory in (3+1) dimensions. We consider both the time-like and the light-like Wilson loops. The gravity dual background is given by a particular decoupling limit of (D1,D3) bound state of type IIB string theory. We obtain the velocity dependent quark-antiquark potential and numerically study how the dipole length and the potential change with velocity (for 0 < v < 1, i.e., the Wilson loop is time-like) of the dipole as well as noncommutativ"},"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":"1201.0129","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-12-30T14:09:22Z","cross_cats_sorted":[],"title_canon_sha256":"45760bcaf9e4bc29b4f3b69316fb9ab619b108d70db964ddbca42eec84d42651","abstract_canon_sha256":"e094ed0dd407da493f43d702a45446f5666a5e6011ee9f0e4f9d033d69da11db"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:28:12.371796Z","signature_b64":"d06zyjJDvX0i71pYKZ/tiamHeWudHlyM0ns45qw2zwKGmpIM0qvnIHje9POBwF7PtzEuRpPHYRBPuMNd5zzmBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f787b840002329d0163db6484878aa59be2f5d2b1450640b6f5c5f9a9a1b6cb8","last_reissued_at":"2026-05-18T02:28:12.371098Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:28:12.371098Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Wilson loops in noncommutative Yang-Mills theory using gauge/gravity duality","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Najmul Haque, Shibaji Roy, Somdeb Chakraborty","submitted_at":"2011-12-30T14:09:22Z","abstract_excerpt":"By using the gauge/gravity duality and the Maldacena prescription we compute the expectation values of the Wilson loops in noncommutative Yang-Mills (NCYM) theory in (3+1) dimensions. We consider both the time-like and the light-like Wilson loops. The gravity dual background is given by a particular decoupling limit of (D1,D3) bound state of type IIB string theory. We obtain the velocity dependent quark-antiquark potential and numerically study how the dipole length and the potential change with velocity (for 0 < v < 1, i.e., the Wilson loop is time-like) of the dipole as well as noncommutativ"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.0129","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":"1201.0129","created_at":"2026-05-18T02:28:12.371242+00:00"},{"alias_kind":"arxiv_version","alias_value":"1201.0129v2","created_at":"2026-05-18T02:28:12.371242+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.0129","created_at":"2026-05-18T02:28:12.371242+00:00"},{"alias_kind":"pith_short_12","alias_value":"66D3QQAAEMU5","created_at":"2026-05-18T12:26:22.705136+00:00"},{"alias_kind":"pith_short_16","alias_value":"66D3QQAAEMU5AFR5","created_at":"2026-05-18T12:26:22.705136+00:00"},{"alias_kind":"pith_short_8","alias_value":"66D3QQAA","created_at":"2026-05-18T12:26:22.705136+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/66D3QQAAEMU5AFR5WZEEQ6FKLG","json":"https://pith.science/pith/66D3QQAAEMU5AFR5WZEEQ6FKLG.json","graph_json":"https://pith.science/api/pith-number/66D3QQAAEMU5AFR5WZEEQ6FKLG/graph.json","events_json":"https://pith.science/api/pith-number/66D3QQAAEMU5AFR5WZEEQ6FKLG/events.json","paper":"https://pith.science/paper/66D3QQAA"},"agent_actions":{"view_html":"https://pith.science/pith/66D3QQAAEMU5AFR5WZEEQ6FKLG","download_json":"https://pith.science/pith/66D3QQAAEMU5AFR5WZEEQ6FKLG.json","view_paper":"https://pith.science/paper/66D3QQAA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1201.0129&json=true","fetch_graph":"https://pith.science/api/pith-number/66D3QQAAEMU5AFR5WZEEQ6FKLG/graph.json","fetch_events":"https://pith.science/api/pith-number/66D3QQAAEMU5AFR5WZEEQ6FKLG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/66D3QQAAEMU5AFR5WZEEQ6FKLG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/66D3QQAAEMU5AFR5WZEEQ6FKLG/action/storage_attestation","attest_author":"https://pith.science/pith/66D3QQAAEMU5AFR5WZEEQ6FKLG/action/author_attestation","sign_citation":"https://pith.science/pith/66D3QQAAEMU5AFR5WZEEQ6FKLG/action/citation_signature","submit_replication":"https://pith.science/pith/66D3QQAAEMU5AFR5WZEEQ6FKLG/action/replication_record"}},"created_at":"2026-05-18T02:28:12.371242+00:00","updated_at":"2026-05-18T02:28:12.371242+00:00"}