Stiefel Liquids: Possible Non-Lagrangian Quantum Criticality from Intertwined Orders

We propose a new type of quantum liquids, dubbed Stiefel liquids, based on (2+1)-dimensional nonlinear sigma models on target space SO(N)/SO(4), supplemented with Wess-Zumino-Witten terms. We argue that the Stiefel liquids form a class of critical quantum liquids with extraordinary properties, such...

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Autores principales: Liujun Zou, Yin-Chen He, Chong Wang
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Publicado: American Physical Society 2021
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spelling oai:doaj.org-article:18dc49ddf42f4ba8b96ab8e07fc5b5702021-12-02T18:00:43ZStiefel Liquids: Possible Non-Lagrangian Quantum Criticality from Intertwined Orders10.1103/PhysRevX.11.0310432160-3308https://doaj.org/article/18dc49ddf42f4ba8b96ab8e07fc5b5702021-08-01T00:00:00Zhttp://doi.org/10.1103/PhysRevX.11.031043http://doi.org/10.1103/PhysRevX.11.031043https://doaj.org/toc/2160-3308We propose a new type of quantum liquids, dubbed Stiefel liquids, based on (2+1)-dimensional nonlinear sigma models on target space SO(N)/SO(4), supplemented with Wess-Zumino-Witten terms. We argue that the Stiefel liquids form a class of critical quantum liquids with extraordinary properties, such as large emergent symmetries, a cascade structure, and nontrivial quantum anomalies. We show that the well-known deconfined quantum critical point and U(1) Dirac spin liquid are unified as two special examples of Stiefel liquids, N=5 and N=6, respectively. Furthermore, we conjecture that Stiefel liquids with N>6 are non-Lagrangian, in the sense that under renormalization group they flow to infrared (conformally invariant) fixed points that cannot be described by any renormalizable continuum Lagrangian. Such non-Lagrangian states are beyond the paradigm of parton gauge mean-field theory familiar in the study of exotic quantum liquids in condensed matter physics. The intrinsic absence of (conventional or partonlike) mean-field construction also means that, within the traditional approaches, will be difficult to decide whether a non-Lagrangian state can actually emerge from a specific UV system (such as a lattice spin system). For this purpose we hypothesize that a quantum state is emergible from a lattice system if its quantum anomalies match with the constraints from the (generalized) Lieb-Schultz-Mattis theorems. Based on this hypothesis, we find that some of the non-Lagrangian Stiefel liquids can indeed be realized in frustrated quantum spin systems, for example, on triangular or kagome lattice, through the intertwinement between noncoplanar magnetic orders and valence-bond-solid orders.Liujun ZouYin-Chen HeChong WangAmerican Physical SocietyarticlePhysicsQC1-999ENPhysical Review X, Vol 11, Iss 3, p 031043 (2021)
institution DOAJ
collection DOAJ
language EN
topic Physics
QC1-999
spellingShingle Physics
QC1-999
Liujun Zou
Yin-Chen He
Chong Wang
Stiefel Liquids: Possible Non-Lagrangian Quantum Criticality from Intertwined Orders
description We propose a new type of quantum liquids, dubbed Stiefel liquids, based on (2+1)-dimensional nonlinear sigma models on target space SO(N)/SO(4), supplemented with Wess-Zumino-Witten terms. We argue that the Stiefel liquids form a class of critical quantum liquids with extraordinary properties, such as large emergent symmetries, a cascade structure, and nontrivial quantum anomalies. We show that the well-known deconfined quantum critical point and U(1) Dirac spin liquid are unified as two special examples of Stiefel liquids, N=5 and N=6, respectively. Furthermore, we conjecture that Stiefel liquids with N>6 are non-Lagrangian, in the sense that under renormalization group they flow to infrared (conformally invariant) fixed points that cannot be described by any renormalizable continuum Lagrangian. Such non-Lagrangian states are beyond the paradigm of parton gauge mean-field theory familiar in the study of exotic quantum liquids in condensed matter physics. The intrinsic absence of (conventional or partonlike) mean-field construction also means that, within the traditional approaches, will be difficult to decide whether a non-Lagrangian state can actually emerge from a specific UV system (such as a lattice spin system). For this purpose we hypothesize that a quantum state is emergible from a lattice system if its quantum anomalies match with the constraints from the (generalized) Lieb-Schultz-Mattis theorems. Based on this hypothesis, we find that some of the non-Lagrangian Stiefel liquids can indeed be realized in frustrated quantum spin systems, for example, on triangular or kagome lattice, through the intertwinement between noncoplanar magnetic orders and valence-bond-solid orders.
format article
author Liujun Zou
Yin-Chen He
Chong Wang
author_facet Liujun Zou
Yin-Chen He
Chong Wang
author_sort Liujun Zou
title Stiefel Liquids: Possible Non-Lagrangian Quantum Criticality from Intertwined Orders
title_short Stiefel Liquids: Possible Non-Lagrangian Quantum Criticality from Intertwined Orders
title_full Stiefel Liquids: Possible Non-Lagrangian Quantum Criticality from Intertwined Orders
title_fullStr Stiefel Liquids: Possible Non-Lagrangian Quantum Criticality from Intertwined Orders
title_full_unstemmed Stiefel Liquids: Possible Non-Lagrangian Quantum Criticality from Intertwined Orders
title_sort stiefel liquids: possible non-lagrangian quantum criticality from intertwined orders
publisher American Physical Society
publishDate 2021
url https://doaj.org/article/18dc49ddf42f4ba8b96ab8e07fc5b570
work_keys_str_mv AT liujunzou stiefelliquidspossiblenonlagrangianquantumcriticalityfromintertwinedorders
AT yinchenhe stiefelliquidspossiblenonlagrangianquantumcriticalityfromintertwinedorders
AT chongwang stiefelliquidspossiblenonlagrangianquantumcriticalityfromintertwinedorders
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