{"title":"Ultraviolet-Complete Local Field Theory of Persistent Symmetry Breaking in 2+1 Dimensions","authors":"Bilal Hawashin, Junchen Rong, Michael M. Scherer","doi":"10.1103/physrevlett.134.041602","DOIUrl":null,"url":null,"abstract":"Spontaneous symmetry breaking can persist at all temperatures in certain biconical O</a:mi>(</a:mo>N</a:mi>)</a:mo>×</a:mo>Z</a:mi></a:mrow>2</a:mn></a:mrow></a:msub></a:mrow></a:math> vector models when the underlying field theories are ultraviolet complete. So far, the existence of such theories has been established in fractional dimensions for local but nonunitary models or in <g:math xmlns:g=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><g:mrow><g:mn>2</g:mn><g:mo>+</g:mo><g:mn>1</g:mn></g:mrow></g:math> dimensions but for nonlocal models. Here, we study local models at zero and finite temperature directly in <i:math xmlns:i=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><i:mrow><i:mn>2</i:mn><i:mo>+</i:mo><i:mn>1</i:mn></i:mrow></i:math> dimensions employing functional methods. At zero temperature, we establish that our approach describes the quantum critical behavior with good accuracy for all <k:math xmlns:k=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><k:mi>N</k:mi><k:mo>≥</k:mo><k:mn>2</k:mn></k:math>. We then exhibit the mechanism of discrete symmetry breaking from <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><m:mrow><m:mi mathvariant=\"normal\">O</m:mi><m:mo stretchy=\"false\">(</m:mo><m:mi>N</m:mi><m:mo stretchy=\"false\">)</m:mo><m:mo>×</m:mo><m:msub><m:mrow><m:mi mathvariant=\"double-struck\">Z</m:mi></m:mrow><m:mrow><m:mn>2</m:mn></m:mrow></m:msub><m:mo stretchy=\"false\">→</m:mo><m:mi mathvariant=\"normal\">O</m:mi><m:mo stretchy=\"false\">(</m:mo><m:mi>N</m:mi><m:mo stretchy=\"false\">)</m:mo></m:mrow></m:math> for increasing temperature near the biconical critical point when <w:math xmlns:w=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><w:mi>N</w:mi></w:math> is finite but large. We calculate the corresponding finite-temperature phase diagram and further show that the Hohenberg-Mermin-Wagner theorem is fully respected within this approach, i.e., symmetry breaking only occurs in the <y:math xmlns:y=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><y:msub><y:mi mathvariant=\"double-struck\">Z</y:mi><y:mn>2</y:mn></y:msub></y:math> sector. Finally, we determine the critical <bb:math xmlns:bb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><bb:mi>N</bb:mi></bb:math> above which this phenomenon can be observed to be <db:math xmlns:db=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><db:msub><db:mi>N</db:mi><db:mi>c</db:mi></db:msub><db:mo>≈</db:mo><db:mn>15</db:mn></db:math>. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"31 1","pages":""},"PeriodicalIF":8.1000,"publicationDate":"2025-01-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical review letters","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/physrevlett.134.041602","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
Spontaneous symmetry breaking can persist at all temperatures in certain biconical O(N)×Z2 vector models when the underlying field theories are ultraviolet complete. So far, the existence of such theories has been established in fractional dimensions for local but nonunitary models or in 2+1 dimensions but for nonlocal models. Here, we study local models at zero and finite temperature directly in 2+1 dimensions employing functional methods. At zero temperature, we establish that our approach describes the quantum critical behavior with good accuracy for all N≥2. We then exhibit the mechanism of discrete symmetry breaking from O(N)×Z2→O(N) for increasing temperature near the biconical critical point when N is finite but large. We calculate the corresponding finite-temperature phase diagram and further show that the Hohenberg-Mermin-Wagner theorem is fully respected within this approach, i.e., symmetry breaking only occurs in the Z2 sector. Finally, we determine the critical N above which this phenomenon can be observed to be Nc≈15. Published by the American Physical Society2025
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