{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:HOUPHT23YOPCGESLMH3WHZPQTA","short_pith_number":"pith:HOUPHT23","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"},"canonical_sha256":"3ba8f3cf5bc39e23124b61f763e5f0981d4051f5eb59d607a087b6820073d7bd","source":{"kind":"arxiv","id":"1502.01942","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1502.01942","created_at":"2026-05-18T02:27:07Z"},{"alias_kind":"arxiv_version","alias_value":"1502.01942v2","created_at":"2026-05-18T02:27:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1502.01942","created_at":"2026-05-18T02:27:07Z"},{"alias_kind":"pith_short_12","alias_value":"HOUPHT23YOPC","created_at":"2026-05-18T12:29:25Z"},{"alias_kind":"pith_short_16","alias_value":"HOUPHT23YOPCGESL","created_at":"2026-05-18T12:29:25Z"},{"alias_kind":"pith_short_8","alias_value":"HOUPHT23","created_at":"2026-05-18T12:29:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:HOUPHT23YOPCGESLMH3WHZPQTA","target":"record","payload":{"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"},"canonical_sha256":"3ba8f3cf5bc39e23124b61f763e5f0981d4051f5eb59d607a087b6820073d7bd","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"},"source_kind":"arxiv","source_id":"1502.01942","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:27:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"K4RJZH5xOy7nF7CgZeCmwjCkRwe4xChDJAAaMTWi1tSQSL8mnevAEzeJnTLifD7X+OUTptdoWRY/dkMfYjzOCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T15:24:26.490686Z"},"content_sha256":"39930d2a0076ed8e1db1ad83f378fe140b5ae9a7ade03da8db792dfb075c0632","schema_version":"1.0","event_id":"sha256:39930d2a0076ed8e1db1ad83f378fe140b5ae9a7ade03da8db792dfb075c0632"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:HOUPHT23YOPCGESLMH3WHZPQTA","target":"graph","payload":{"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:27:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1XbbBja1ZgLyuRAmAXShDt+D8BtovClVtD7JhEH/wMd7lNyo19GWO5CK24sU6dHMwiB6ycMMVzq0DwwZ1WW+Cg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T15:24:26.491346Z"},"content_sha256":"cb6a570e3b005d848eaa1ffc72a349368487dbebf68f594892b2d341b17cc9c6","schema_version":"1.0","event_id":"sha256:cb6a570e3b005d848eaa1ffc72a349368487dbebf68f594892b2d341b17cc9c6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HOUPHT23YOPCGESLMH3WHZPQTA/bundle.json","state_url":"https://pith.science/pith/HOUPHT23YOPCGESLMH3WHZPQTA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HOUPHT23YOPCGESLMH3WHZPQTA/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-08T15:24:26Z","links":{"resolver":"https://pith.science/pith/HOUPHT23YOPCGESLMH3WHZPQTA","bundle":"https://pith.science/pith/HOUPHT23YOPCGESLMH3WHZPQTA/bundle.json","state":"https://pith.science/pith/HOUPHT23YOPCGESLMH3WHZPQTA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HOUPHT23YOPCGESLMH3WHZPQTA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:HOUPHT23YOPCGESLMH3WHZPQTA","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"d611235e42f42cf2ecac6ca6f9c8b9c632f84cfa8f450170899d60384e6280ad","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-02-06T16:40:04Z","title_canon_sha256":"10bd6e45739d2b862e82f713c213f4eeaa8c458a2608de3aa9d4dbd850b5991c"},"schema_version":"1.0","source":{"id":"1502.01942","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1502.01942","created_at":"2026-05-18T02:27:07Z"},{"alias_kind":"arxiv_version","alias_value":"1502.01942v2","created_at":"2026-05-18T02:27:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1502.01942","created_at":"2026-05-18T02:27:07Z"},{"alias_kind":"pith_short_12","alias_value":"HOUPHT23YOPC","created_at":"2026-05-18T12:29:25Z"},{"alias_kind":"pith_short_16","alias_value":"HOUPHT23YOPCGESL","created_at":"2026-05-18T12:29:25Z"},{"alias_kind":"pith_short_8","alias_value":"HOUPHT23","created_at":"2026-05-18T12:29:25Z"}],"graph_snapshots":[{"event_id":"sha256:cb6a570e3b005d848eaa1ffc72a349368487dbebf68f594892b2d341b17cc9c6","target":"graph","created_at":"2026-05-18T02:27:07Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"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*.","authors_text":"Konstantin Zarembo, Xinyi Chen-Lin","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-02-06T16:40:04Z","title":"Higher Rank Wilson Loops in N = 2* Super-Yang-Mills Theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1502.01942","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:39930d2a0076ed8e1db1ad83f378fe140b5ae9a7ade03da8db792dfb075c0632","target":"record","created_at":"2026-05-18T02:27:07Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"d611235e42f42cf2ecac6ca6f9c8b9c632f84cfa8f450170899d60384e6280ad","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-02-06T16:40:04Z","title_canon_sha256":"10bd6e45739d2b862e82f713c213f4eeaa8c458a2608de3aa9d4dbd850b5991c"},"schema_version":"1.0","source":{"id":"1502.01942","kind":"arxiv","version":2}},"canonical_sha256":"3ba8f3cf5bc39e23124b61f763e5f0981d4051f5eb59d607a087b6820073d7bd","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3ba8f3cf5bc39e23124b61f763e5f0981d4051f5eb59d607a087b6820073d7bd","first_computed_at":"2026-05-18T02:27:07.242616Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:27:07.242616Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"f3XofLq1PhaIhV8OlBrizkgG75Cl0d1UBeihGIlKnP7cwreBxY/O+FmmfczqxSlezSDFvhX+0bYAOMQklexICQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:27:07.243560Z","signed_message":"canonical_sha256_bytes"},"source_id":"1502.01942","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:39930d2a0076ed8e1db1ad83f378fe140b5ae9a7ade03da8db792dfb075c0632","sha256:cb6a570e3b005d848eaa1ffc72a349368487dbebf68f594892b2d341b17cc9c6"],"state_sha256":"8fd52da0cf858fcac845c3dd24fa72a718d2825b630260585e09d5f35ef37c3c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"q2KO6F+Bv0Aa4RDbZ5sXiieLjwNL2a00MhuntrPnAYRjcYwl1fM1hXYdwY3vrqQzOKnL+ruQHWHekv1ck1lkAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-08T15:24:26.495621Z","bundle_sha256":"0fd007073f43849aee5f2ad2ee97befe9456de46a925e4e19ad87dd12c0182ee"}}