{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2021:RICM3YVOZFGZ6TUTELFHX5XXDT","short_pith_number":"pith:RICM3YVO","canonical_record":{"source":{"id":"2106.11323","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2021-06-21T18:00:02Z","cross_cats_sorted":["cond-mat.str-el","hep-ph"],"title_canon_sha256":"efe3b548a8a678979c1e590adc744c65646a04f864428530a5b61496e27b0c06","abstract_canon_sha256":"50c7c93cab3071b61d5f037bcdfd0a34bc3ce230ad6dab67cbc0801c156f12d5"},"schema_version":"1.0"},"canonical_sha256":"8a04cde2aec94d9f4e9322ca7bf6f71cebedc4b7b073e33f123d04f9c9ce9c44","source":{"kind":"arxiv","id":"2106.11323","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2106.11323","created_at":"2026-07-05T03:14:20Z"},{"alias_kind":"arxiv_version","alias_value":"2106.11323v2","created_at":"2026-07-05T03:14:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2106.11323","created_at":"2026-07-05T03:14:20Z"},{"alias_kind":"pith_short_12","alias_value":"RICM3YVOZFGZ","created_at":"2026-07-05T03:14:20Z"},{"alias_kind":"pith_short_16","alias_value":"RICM3YVOZFGZ6TUT","created_at":"2026-07-05T03:14:20Z"},{"alias_kind":"pith_short_8","alias_value":"RICM3YVO","created_at":"2026-07-05T03:14:20Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2021:RICM3YVOZFGZ6TUTELFHX5XXDT","target":"record","payload":{"canonical_record":{"source":{"id":"2106.11323","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2021-06-21T18:00:02Z","cross_cats_sorted":["cond-mat.str-el","hep-ph"],"title_canon_sha256":"efe3b548a8a678979c1e590adc744c65646a04f864428530a5b61496e27b0c06","abstract_canon_sha256":"50c7c93cab3071b61d5f037bcdfd0a34bc3ce230ad6dab67cbc0801c156f12d5"},"schema_version":"1.0"},"canonical_sha256":"8a04cde2aec94d9f4e9322ca7bf6f71cebedc4b7b073e33f123d04f9c9ce9c44","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:14:20.369610Z","signature_b64":"+euXll7W7yIxge2gFPAFyr4NZNkYdmRwyMczv2yWacrBOuok+R3jFSwX9w2RoLK+Jok8YIhmO2wVolLO0BP2Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8a04cde2aec94d9f4e9322ca7bf6f71cebedc4b7b073e33f123d04f9c9ce9c44","last_reissued_at":"2026-07-05T03:14:20.369255Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:14:20.369255Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2106.11323","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":"2026-07-05T03:14:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FXE+QYyBK/W9kbeaXZfuXxL+kb6m48ClqYsIVS/hcaSjIYk4KSeUMOl8YEidpk1eMPO1Xd69389Xgf4R5094Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-09T09:19:39.211264Z"},"content_sha256":"3d9bc0de9996c25129e81b8fe724ef8dfbdddb79ade6777c11b9b15c1b5bbb32","schema_version":"1.0","event_id":"sha256:3d9bc0de9996c25129e81b8fe724ef8dfbdddb79ade6777c11b9b15c1b5bbb32"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2021:RICM3YVOZFGZ6TUTELFHX5XXDT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Symmetry breaking at high temperatures in large N gauge theories","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.str-el","hep-ph"],"primary_cat":"hep-th","authors_text":"Eliezer Rabinovici, Soumyadeep Chaudhuri","submitted_at":"2021-06-21T18:00:02Z","abstract_excerpt":"Considering marginally relevant and relevant deformations of the weakly coupled $(3+1)$-dimensional large $N$ conformal gauge theories introduced in arXiv:2011.13981, we study the patterns of phase transitions in these systems that lead to a symmetry-broken phase in the high temperature limit. These deformations involve only the scalar fields in the models. The marginally relevant deformations are obtained by varying certain double trace quartic couplings between the scalar fields. The relevant deformations, on the other hand, are obtained by adding masses to the scalar fields while keeping al"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2106.11323","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2106.11323/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":"2026-07-05T03:14:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oUSI3dgCbsIwIftS3lybci6sBm1Iw/yzs5z0KDIxDb9Bn+2YIYAhUS6vqIwgDJupV4AdSuoCaYf4JaLoDK8KBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-09T09:19:39.211765Z"},"content_sha256":"70885e9f2cefe22b2ff4bef9427019f193c122badba4110041b736e8149abc93","schema_version":"1.0","event_id":"sha256:70885e9f2cefe22b2ff4bef9427019f193c122badba4110041b736e8149abc93"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RICM3YVOZFGZ6TUTELFHX5XXDT/bundle.json","state_url":"https://pith.science/pith/RICM3YVOZFGZ6TUTELFHX5XXDT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RICM3YVOZFGZ6TUTELFHX5XXDT/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":"2026-08-09T09:19:39Z","links":{"resolver":"https://pith.science/pith/RICM3YVOZFGZ6TUTELFHX5XXDT","bundle":"https://pith.science/pith/RICM3YVOZFGZ6TUTELFHX5XXDT/bundle.json","state":"https://pith.science/pith/RICM3YVOZFGZ6TUTELFHX5XXDT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RICM3YVOZFGZ6TUTELFHX5XXDT/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:RICM3YVOZFGZ6TUTELFHX5XXDT","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":"50c7c93cab3071b61d5f037bcdfd0a34bc3ce230ad6dab67cbc0801c156f12d5","cross_cats_sorted":["cond-mat.str-el","hep-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2021-06-21T18:00:02Z","title_canon_sha256":"efe3b548a8a678979c1e590adc744c65646a04f864428530a5b61496e27b0c06"},"schema_version":"1.0","source":{"id":"2106.11323","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2106.11323","created_at":"2026-07-05T03:14:20Z"},{"alias_kind":"arxiv_version","alias_value":"2106.11323v2","created_at":"2026-07-05T03:14:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2106.11323","created_at":"2026-07-05T03:14:20Z"},{"alias_kind":"pith_short_12","alias_value":"RICM3YVOZFGZ","created_at":"2026-07-05T03:14:20Z"},{"alias_kind":"pith_short_16","alias_value":"RICM3YVOZFGZ6TUT","created_at":"2026-07-05T03:14:20Z"},{"alias_kind":"pith_short_8","alias_value":"RICM3YVO","created_at":"2026-07-05T03:14:20Z"}],"graph_snapshots":[{"event_id":"sha256:70885e9f2cefe22b2ff4bef9427019f193c122badba4110041b736e8149abc93","target":"graph","created_at":"2026-07-05T03:14:20Z","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/2106.11323/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Considering marginally relevant and relevant deformations of the weakly coupled $(3+1)$-dimensional large $N$ conformal gauge theories introduced in arXiv:2011.13981, we study the patterns of phase transitions in these systems that lead to a symmetry-broken phase in the high temperature limit. These deformations involve only the scalar fields in the models. The marginally relevant deformations are obtained by varying certain double trace quartic couplings between the scalar fields. The relevant deformations, on the other hand, are obtained by adding masses to the scalar fields while keeping al","authors_text":"Eliezer Rabinovici, Soumyadeep Chaudhuri","cross_cats":["cond-mat.str-el","hep-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2021-06-21T18:00:02Z","title":"Symmetry breaking at high temperatures in large N gauge theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2106.11323","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":"sha256:3d9bc0de9996c25129e81b8fe724ef8dfbdddb79ade6777c11b9b15c1b5bbb32","target":"record","created_at":"2026-07-05T03:14:20Z","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":"50c7c93cab3071b61d5f037bcdfd0a34bc3ce230ad6dab67cbc0801c156f12d5","cross_cats_sorted":["cond-mat.str-el","hep-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2021-06-21T18:00:02Z","title_canon_sha256":"efe3b548a8a678979c1e590adc744c65646a04f864428530a5b61496e27b0c06"},"schema_version":"1.0","source":{"id":"2106.11323","kind":"arxiv","version":2}},"canonical_sha256":"8a04cde2aec94d9f4e9322ca7bf6f71cebedc4b7b073e33f123d04f9c9ce9c44","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8a04cde2aec94d9f4e9322ca7bf6f71cebedc4b7b073e33f123d04f9c9ce9c44","first_computed_at":"2026-07-05T03:14:20.369255Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T03:14:20.369255Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"+euXll7W7yIxge2gFPAFyr4NZNkYdmRwyMczv2yWacrBOuok+R3jFSwX9w2RoLK+Jok8YIhmO2wVolLO0BP2Aw==","signature_status":"signed_v1","signed_at":"2026-07-05T03:14:20.369610Z","signed_message":"canonical_sha256_bytes"},"source_id":"2106.11323","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3d9bc0de9996c25129e81b8fe724ef8dfbdddb79ade6777c11b9b15c1b5bbb32","sha256:70885e9f2cefe22b2ff4bef9427019f193c122badba4110041b736e8149abc93"],"state_sha256":"1b5084965ec33f2e2c9f0893016d49fff67e275c61ce16c3101fcef7928f6b82"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"He/4UqDJpDd5wgZQE19vqjO8gt6T+udaFHJ/txG4PwBMQrB3wYVSM9sPDd8X2YnMrxSfQsIGCujLpcbzf4hVBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-09T09:19:39.215313Z","bundle_sha256":"db87813938864ede252c78c5dede97c4de1ac4882bf23e5df1e4c26bf2d86c2c"}}