{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1999:JYEE6JSM2HD4YMOCZUSSLCQKND","short_pith_number":"pith:JYEE6JSM","canonical_record":{"source":{"id":"hep-th/9904149","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1999-04-21T19:23:53Z","cross_cats_sorted":[],"title_canon_sha256":"de197a9070aa501b5acb898ca05924a1a214bb7b31c810038682aa7ef5d26e05","abstract_canon_sha256":"6a44a0d0dfa23f19100ffeab38b3dc2cb1c7f9e83bd533ae00451d2175e33fe9"},"schema_version":"1.0"},"canonical_sha256":"4e084f264cd1c7cc31c2cd25258a0a68e8de28d215fc32b8a4ff943044597ecf","source":{"kind":"arxiv","id":"hep-th/9904149","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9904149","created_at":"2026-07-04T16:14:49Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9904149v1","created_at":"2026-07-04T16:14:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9904149","created_at":"2026-07-04T16:14:49Z"},{"alias_kind":"pith_short_12","alias_value":"JYEE6JSM2HD4","created_at":"2026-07-04T16:14:49Z"},{"alias_kind":"pith_short_16","alias_value":"JYEE6JSM2HD4YMOC","created_at":"2026-07-04T16:14:49Z"},{"alias_kind":"pith_short_8","alias_value":"JYEE6JSM","created_at":"2026-07-04T16:14:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1999:JYEE6JSM2HD4YMOCZUSSLCQKND","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/9904149","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1999-04-21T19:23:53Z","cross_cats_sorted":[],"title_canon_sha256":"de197a9070aa501b5acb898ca05924a1a214bb7b31c810038682aa7ef5d26e05","abstract_canon_sha256":"6a44a0d0dfa23f19100ffeab38b3dc2cb1c7f9e83bd533ae00451d2175e33fe9"},"schema_version":"1.0"},"canonical_sha256":"4e084f264cd1c7cc31c2cd25258a0a68e8de28d215fc32b8a4ff943044597ecf","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:14:49.384192Z","signature_b64":"pZOWYAfytwEWb2+95rP8p9Kz1BTuhwBfzGBoUB6+aHSehxey5AMHR6A/jtJAusL5Pxp2PNMftwvfYmFKvEo6AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4e084f264cd1c7cc31c2cd25258a0a68e8de28d215fc32b8a4ff943044597ecf","last_reissued_at":"2026-07-04T16:14:49.383808Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:14:49.383808Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/9904149","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T16:14:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wA9UNOlSgTRRadOYCAhVVb921Qs9/ux9JHRRaVYFHfQ4HSoUZL9MhABlJ4wp9201xZIdjClnpNdm39e5dGywCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T13:57:33.386532Z"},"content_sha256":"c7e3d8febff6b66d4e4326fe476c7c2e21c9bca75c5627f9f2d1576fb6ef050f","schema_version":"1.0","event_id":"sha256:c7e3d8febff6b66d4e4326fe476c7c2e21c9bca75c5627f9f2d1576fb6ef050f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1999:JYEE6JSM2HD4YMOCZUSSLCQKND","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Wilson Loop Correlator in the AdS/CFT Correspondence","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"K. Zarembo","submitted_at":"1999-04-21T19:23:53Z","abstract_excerpt":"The AdS/CFT correspondence predicts a phase transition in Wilson loop correlators in the strong coupling N=4, D=4 SYM theory which arises due to instability of the classical string stretched between the loops. We study this transition in detail by solving equations of motion for the string in the particular case of two circular Wilson loops. The transition is argued to be smoothened at finite `t Hooft coupling by fluctuations of the string world sheet and to be promoted to a sharp crossover. Some general comments about Wilson loop correlators in gauge theories are made."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9904149","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/9904149/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T16:14:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5TsZeTsELbgA/BVT14rtjbbOtedfAZ+pdVl40f5VssDRoveIyjEMdMOpkshpedYb3xPk3Ei7Zzf0jc/VpjwfBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T13:57:33.387426Z"},"content_sha256":"af4e4246be6524e3bed49d42ba3686522bc5a972b0fcab972f40ce29d70fc62e","schema_version":"1.0","event_id":"sha256:af4e4246be6524e3bed49d42ba3686522bc5a972b0fcab972f40ce29d70fc62e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JYEE6JSM2HD4YMOCZUSSLCQKND/bundle.json","state_url":"https://pith.science/pith/JYEE6JSM2HD4YMOCZUSSLCQKND/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JYEE6JSM2HD4YMOCZUSSLCQKND/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":"2026-08-12T13:57:33Z","links":{"resolver":"https://pith.science/pith/JYEE6JSM2HD4YMOCZUSSLCQKND","bundle":"https://pith.science/pith/JYEE6JSM2HD4YMOCZUSSLCQKND/bundle.json","state":"https://pith.science/pith/JYEE6JSM2HD4YMOCZUSSLCQKND/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JYEE6JSM2HD4YMOCZUSSLCQKND/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1999:JYEE6JSM2HD4YMOCZUSSLCQKND","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":"6a44a0d0dfa23f19100ffeab38b3dc2cb1c7f9e83bd533ae00451d2175e33fe9","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1999-04-21T19:23:53Z","title_canon_sha256":"de197a9070aa501b5acb898ca05924a1a214bb7b31c810038682aa7ef5d26e05"},"schema_version":"1.0","source":{"id":"hep-th/9904149","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9904149","created_at":"2026-07-04T16:14:49Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9904149v1","created_at":"2026-07-04T16:14:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9904149","created_at":"2026-07-04T16:14:49Z"},{"alias_kind":"pith_short_12","alias_value":"JYEE6JSM2HD4","created_at":"2026-07-04T16:14:49Z"},{"alias_kind":"pith_short_16","alias_value":"JYEE6JSM2HD4YMOC","created_at":"2026-07-04T16:14:49Z"},{"alias_kind":"pith_short_8","alias_value":"JYEE6JSM","created_at":"2026-07-04T16:14:49Z"}],"graph_snapshots":[{"event_id":"sha256:af4e4246be6524e3bed49d42ba3686522bc5a972b0fcab972f40ce29d70fc62e","target":"graph","created_at":"2026-07-04T16:14:49Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-th/9904149/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The AdS/CFT correspondence predicts a phase transition in Wilson loop correlators in the strong coupling N=4, D=4 SYM theory which arises due to instability of the classical string stretched between the loops. We study this transition in detail by solving equations of motion for the string in the particular case of two circular Wilson loops. The transition is argued to be smoothened at finite `t Hooft coupling by fluctuations of the string world sheet and to be promoted to a sharp crossover. Some general comments about Wilson loop correlators in gauge theories are made.","authors_text":"K. Zarembo","cross_cats":[],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"1999-04-21T19:23:53Z","title":"Wilson Loop Correlator in the AdS/CFT Correspondence"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9904149","kind":"arxiv","version":1},"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:c7e3d8febff6b66d4e4326fe476c7c2e21c9bca75c5627f9f2d1576fb6ef050f","target":"record","created_at":"2026-07-04T16:14:49Z","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":"6a44a0d0dfa23f19100ffeab38b3dc2cb1c7f9e83bd533ae00451d2175e33fe9","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1999-04-21T19:23:53Z","title_canon_sha256":"de197a9070aa501b5acb898ca05924a1a214bb7b31c810038682aa7ef5d26e05"},"schema_version":"1.0","source":{"id":"hep-th/9904149","kind":"arxiv","version":1}},"canonical_sha256":"4e084f264cd1c7cc31c2cd25258a0a68e8de28d215fc32b8a4ff943044597ecf","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4e084f264cd1c7cc31c2cd25258a0a68e8de28d215fc32b8a4ff943044597ecf","first_computed_at":"2026-07-04T16:14:49.383808Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:14:49.383808Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"pZOWYAfytwEWb2+95rP8p9Kz1BTuhwBfzGBoUB6+aHSehxey5AMHR6A/jtJAusL5Pxp2PNMftwvfYmFKvEo6AA==","signature_status":"signed_v1","signed_at":"2026-07-04T16:14:49.384192Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/9904149","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c7e3d8febff6b66d4e4326fe476c7c2e21c9bca75c5627f9f2d1576fb6ef050f","sha256:af4e4246be6524e3bed49d42ba3686522bc5a972b0fcab972f40ce29d70fc62e"],"state_sha256":"e75d2a1656c2c67901ddbb9153c61034cc9b06812da3ed7fe591ebac3600db82"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uJcH8YNrbIPqNziQ7vH+Qf0JPw+VRgMsoGJwPpXWI35UOWBseVoS8S8sghGVQmgtmIepXM2jO1jthZhMa9T0Bw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-12T13:57:33.408986Z","bundle_sha256":"858e5a0edd18c38c233bb5edc52a2bbc6c478e82ca79f1565607b9c1f12a89e4"}}