{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:HOUPHT23YOPCGESLMH3WHZPQTA","short_pith_number":"pith:HOUPHT23","schema_version":"1.0","canonical_sha256":"3ba8f3cf5bc39e23124b61f763e5f0981d4051f5eb59d607a087b6820073d7bd","source":{"kind":"arxiv","id":"1502.01942","version":2},"attestation_state":"computed","paper":{"title":"Higher Rank Wilson Loops in N = 2* Super-Yang-Mills Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Konstantin Zarembo, Xinyi Chen-Lin","submitted_at":"2015-02-06T16:40:04Z","abstract_excerpt":"The N=2* Super-Yang-Mills theory (SYM*) undergoes an infinite sequence of large-N quantum phase transitions. We compute expectation values of Wilson loops in k-symmetric and antisymmetric representations of the SU(N) gauge group in this theory and show that the same phenomenon that causes the phase transitions at finite coupling leads to a non-analytic dependence of Wilson loops on k/N when the coupling is strictly infinite, thus making the higher-representation Wilson loops ideal holographic probes of the non-trivial phase structure of SYM*."},"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":"1502.01942","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-02-06T16:40:04Z","cross_cats_sorted":[],"title_canon_sha256":"10bd6e45739d2b862e82f713c213f4eeaa8c458a2608de3aa9d4dbd850b5991c","abstract_canon_sha256":"d611235e42f42cf2ecac6ca6f9c8b9c632f84cfa8f450170899d60384e6280ad"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:27:07.243560Z","signature_b64":"f3XofLq1PhaIhV8OlBrizkgG75Cl0d1UBeihGIlKnP7cwreBxY/O+FmmfczqxSlezSDFvhX+0bYAOMQklexICQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3ba8f3cf5bc39e23124b61f763e5f0981d4051f5eb59d607a087b6820073d7bd","last_reissued_at":"2026-05-18T02:27:07.242616Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:27:07.242616Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higher Rank Wilson Loops in N = 2* Super-Yang-Mills Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Konstantin Zarembo, Xinyi Chen-Lin","submitted_at":"2015-02-06T16:40:04Z","abstract_excerpt":"The N=2* Super-Yang-Mills theory (SYM*) undergoes an infinite sequence of large-N quantum phase transitions. We compute expectation values of Wilson loops in k-symmetric and antisymmetric representations of the SU(N) gauge group in this theory and show that the same phenomenon that causes the phase transitions at finite coupling leads to a non-analytic dependence of Wilson loops on k/N when the coupling is strictly infinite, thus making the higher-representation Wilson loops ideal holographic probes of the non-trivial phase structure of SYM*."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1502.01942","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":"1502.01942","created_at":"2026-05-18T02:27:07.242775+00:00"},{"alias_kind":"arxiv_version","alias_value":"1502.01942v2","created_at":"2026-05-18T02:27:07.242775+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1502.01942","created_at":"2026-05-18T02:27:07.242775+00:00"},{"alias_kind":"pith_short_12","alias_value":"HOUPHT23YOPC","created_at":"2026-05-18T12:29:25.134429+00:00"},{"alias_kind":"pith_short_16","alias_value":"HOUPHT23YOPCGESL","created_at":"2026-05-18T12:29:25.134429+00:00"},{"alias_kind":"pith_short_8","alias_value":"HOUPHT23","created_at":"2026-05-18T12:29:25.134429+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/HOUPHT23YOPCGESLMH3WHZPQTA","json":"https://pith.science/pith/HOUPHT23YOPCGESLMH3WHZPQTA.json","graph_json":"https://pith.science/api/pith-number/HOUPHT23YOPCGESLMH3WHZPQTA/graph.json","events_json":"https://pith.science/api/pith-number/HOUPHT23YOPCGESLMH3WHZPQTA/events.json","paper":"https://pith.science/paper/HOUPHT23"},"agent_actions":{"view_html":"https://pith.science/pith/HOUPHT23YOPCGESLMH3WHZPQTA","download_json":"https://pith.science/pith/HOUPHT23YOPCGESLMH3WHZPQTA.json","view_paper":"https://pith.science/paper/HOUPHT23","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1502.01942&json=true","fetch_graph":"https://pith.science/api/pith-number/HOUPHT23YOPCGESLMH3WHZPQTA/graph.json","fetch_events":"https://pith.science/api/pith-number/HOUPHT23YOPCGESLMH3WHZPQTA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HOUPHT23YOPCGESLMH3WHZPQTA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HOUPHT23YOPCGESLMH3WHZPQTA/action/storage_attestation","attest_author":"https://pith.science/pith/HOUPHT23YOPCGESLMH3WHZPQTA/action/author_attestation","sign_citation":"https://pith.science/pith/HOUPHT23YOPCGESLMH3WHZPQTA/action/citation_signature","submit_replication":"https://pith.science/pith/HOUPHT23YOPCGESLMH3WHZPQTA/action/replication_record"}},"created_at":"2026-05-18T02:27:07.242775+00:00","updated_at":"2026-05-18T02:27:07.242775+00:00"}