{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:WCG5LDA2WAJSQPKBP4WTRPDPRT","short_pith_number":"pith:WCG5LDA2","schema_version":"1.0","canonical_sha256":"b08dd58c1ab013283d417f2d38bc6f8cecfd169c3b7219bede6012526728e69e","source":{"kind":"arxiv","id":"2011.13981","version":4},"attestation_state":"computed","paper":{"title":"Thermal order in large N conformal 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":"Changha Choi, Eliezer Rabinovici, Soumyadeep Chaudhuri","submitted_at":"2020-11-27T20:20:14Z","abstract_excerpt":"In this work we explore the possibility of spontaneous breaking of global symmetries at all nonzero temperatures for conformal field theories (CFTs) in $D = 4$ space-time dimensions. We show that such a symmetry-breaking indeed occurs in certain families of non-supersymmetric large $N$ gauge theories at a planar limit. We also show that this phenomenon is accompanied by the system remaining in a persistent Brout-Englert-Higgs (BEH) phase at any temperature. These analyses are motivated by the work done in arXiv:2005.03676 where symmetry-breaking was observed in all thermal states for certain C"},"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":"2011.13981","kind":"arxiv","version":4},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2020-11-27T20:20:14Z","cross_cats_sorted":["cond-mat.str-el","hep-ph"],"title_canon_sha256":"b07e3b14ed7d52c85a001f21b923d120b0f8f89d98089d2fc32ede81fd1702fa","abstract_canon_sha256":"8c3e9c4f7fbf811bf464b2345a67957eda3267a87b0019a14c9fa495058d83f4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:39:08.028279Z","signature_b64":"YhG1D3ASdof0z4WRoVw43euD/icJMLBGdnKQ9lfCcfWXDyAZraL2jwzG0VsHeDJmetV+XPJyjdaFY8AQ+Jk8AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b08dd58c1ab013283d417f2d38bc6f8cecfd169c3b7219bede6012526728e69e","last_reissued_at":"2026-07-05T02:39:08.027782Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:39:08.027782Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermal order in large N conformal 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":"Changha Choi, Eliezer Rabinovici, Soumyadeep Chaudhuri","submitted_at":"2020-11-27T20:20:14Z","abstract_excerpt":"In this work we explore the possibility of spontaneous breaking of global symmetries at all nonzero temperatures for conformal field theories (CFTs) in $D = 4$ space-time dimensions. We show that such a symmetry-breaking indeed occurs in certain families of non-supersymmetric large $N$ gauge theories at a planar limit. We also show that this phenomenon is accompanied by the system remaining in a persistent Brout-Englert-Higgs (BEH) phase at any temperature. These analyses are motivated by the work done in arXiv:2005.03676 where symmetry-breaking was observed in all thermal states for certain C"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2011.13981","kind":"arxiv","version":4},"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/2011.13981/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2011.13981","created_at":"2026-07-05T02:39:08.027844+00:00"},{"alias_kind":"arxiv_version","alias_value":"2011.13981v4","created_at":"2026-07-05T02:39:08.027844+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2011.13981","created_at":"2026-07-05T02:39:08.027844+00:00"},{"alias_kind":"pith_short_12","alias_value":"WCG5LDA2WAJS","created_at":"2026-07-05T02:39:08.027844+00:00"},{"alias_kind":"pith_short_16","alias_value":"WCG5LDA2WAJSQPKB","created_at":"2026-07-05T02:39:08.027844+00:00"},{"alias_kind":"pith_short_8","alias_value":"WCG5LDA2","created_at":"2026-07-05T02:39:08.027844+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.18694","citing_title":"Exploring Entropic Orders: High Temperature Continuous Symmetry Breaking, Chiral Topological States and Local Commuting Projector Models","ref_index":8,"is_internal_anchor":false},{"citing_arxiv_id":"2604.15420","citing_title":"Local CFTs extremise $F$","ref_index":51,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WCG5LDA2WAJSQPKBP4WTRPDPRT","json":"https://pith.science/pith/WCG5LDA2WAJSQPKBP4WTRPDPRT.json","graph_json":"https://pith.science/api/pith-number/WCG5LDA2WAJSQPKBP4WTRPDPRT/graph.json","events_json":"https://pith.science/api/pith-number/WCG5LDA2WAJSQPKBP4WTRPDPRT/events.json","paper":"https://pith.science/paper/WCG5LDA2"},"agent_actions":{"view_html":"https://pith.science/pith/WCG5LDA2WAJSQPKBP4WTRPDPRT","download_json":"https://pith.science/pith/WCG5LDA2WAJSQPKBP4WTRPDPRT.json","view_paper":"https://pith.science/paper/WCG5LDA2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2011.13981&json=true","fetch_graph":"https://pith.science/api/pith-number/WCG5LDA2WAJSQPKBP4WTRPDPRT/graph.json","fetch_events":"https://pith.science/api/pith-number/WCG5LDA2WAJSQPKBP4WTRPDPRT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WCG5LDA2WAJSQPKBP4WTRPDPRT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WCG5LDA2WAJSQPKBP4WTRPDPRT/action/storage_attestation","attest_author":"https://pith.science/pith/WCG5LDA2WAJSQPKBP4WTRPDPRT/action/author_attestation","sign_citation":"https://pith.science/pith/WCG5LDA2WAJSQPKBP4WTRPDPRT/action/citation_signature","submit_replication":"https://pith.science/pith/WCG5LDA2WAJSQPKBP4WTRPDPRT/action/replication_record"}},"created_at":"2026-07-05T02:39:08.027844+00:00","updated_at":"2026-07-05T02:39:08.027844+00:00"}