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相关论文: Anomaly constraint on chiral central charge of (2+…

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A 2+1-dimensional topological quantum field theory (TQFT) may or may not admit topological (gapped) boundary conditions. A famous necessary, but not sufficient, condition for the existence of a topological boundary condition is that the…

高能物理 - 理论 · 物理学 2022-09-28 Justin Kaidi , Zohar Komargodski , Kantaro Ohmori , Sahand Seifnashri , Shu-Heng Shao

We study 't Hooft anomalies of symmetry-enriched rational conformal field theories (RCFT) in (1+1)d. Such anomalies determine whether a theory can be realized in a truly (1+1)d system with on-site symmetry, or on the edge of a (2+1)d…

强关联电子 · 物理学 2020-10-15 Meng Cheng , Dominic J. Williamson

We provide a mathematical proposal for the anomaly indicators of symmetries of (2+1)-d fermionic topological orders, and work out the consequences of our proposal in several nontrivial examples. Our proposal is an invariant of a super…

数学物理 · 物理学 2025-07-11 Arun Debray , Weicheng Ye , Matthew Yu

We describe a method to find the anomaly of the time-reversal symmetry of 2+1d topological quantum field theories, by computing the fractional anomalous momentum on the cross-cap background. This allows us, for example, to identify the…

高能物理 - 理论 · 物理学 2019-12-06 Yuji Tachikawa , Kazuya Yonekura

We study the implications of 't Hooft anomaly (i.e. obstruction to gauging) on conformal field theory, focusing on the case when the global symmetry is $\mathbb{Z_2}$. Using the modular bootstrap, universal bounds on (1+1)-dimensional…

高能物理 - 理论 · 物理学 2020-02-11 Ying-Hsuan Lin , Shu-Heng Shao

Some time-reversal symmetric topological orders are anomalous in that they cannot be realized in strictly two-dimensions without breaking time reversal symmetry; instead, they can only be realized on the surface of certain three-dimensional…

强关联电子 · 物理学 2017-10-04 Chenjie Wang , Michael Levin

We investigate symmetry-preserving gapped boundary of (2+1)D topological phases with global symmetry, which can be either bosonic or fermionic. We develop a general algebraic description for gapped boundary condition for symmetry-enriched…

强关联电子 · 物理学 2022-08-22 Ryohei Kobayashi

We consider the chiral anomaly for systems with a wide class of Hermitian Dirac operators ${Q}$ in 4D Euclidean spacetime. We suppose that $ Q$ is not necessarily linear in derivatives and also that it contains a coordinate inhomogeneity…

高能物理 - 理论 · 物理学 2025-11-26 Praveen D. Xavier , M. A. Zubkov

We develop a theory of anomalies of fermionic topological phases of matter in (2+1)D with a general fermionic symmetry group $G_f$. In general, $G_f$ can be a non-trivial central extension of the bosonic symmetry group $G_b$ by fermion…

强关联电子 · 物理学 2022-04-21 Daniel Bulmash , Maissam Barkeshli

We study a class of 4-dimensional $SU(N)$ chiral gauge theories with fermions in the 2-index symmetric and antisymmetric representations and classify their infrared phases. The choice $N=4\mathbb{Z}$ corresponds to gauging the fermion…

高能物理 - 理论 · 物理学 2022-03-02 Mohamed M. Anber , Sungwoo Hong , Minho Son

A (2+1)D topologically ordered phase may or may not have a gappable edge, even if its chiral central charge $c_-$ is vanishing. Recently, it is discovered that a quantity regarded as a "higher" version of chiral central charge gives a…

强关联电子 · 物理学 2024-01-08 Ryohei Kobayashi , Taige Wang , Tomohiro Soejima , Roger S. K. Mong , Shinsei Ryu

Framing anomaly is a key property of $(2+1)d$ chiral topological orders, for it reveals that the chirality is an intrinsic bulk property of the system, rather than a property of the boundary between two systems. Understanding framing…

高能物理 - 理论 · 物理学 2026-01-09 Ze-An Xu , Jing-Yuan Chen

We study time-reversal symmetry in $(2+1)$D abelian bosonic topological phases. Time-reversal anomalies in such systems are classified by $\mathbb{Z}_2 \times \mathbb{Z}_2$ symmetry-protected topological (SPT) phases in $(3+1)$D, and can be…

高能物理 - 理论 · 物理学 2026-01-21 Ippo Orii

Chiral anomaly is a key feature of Lorentz-invariant quantum field theories: in presence of parallel external electric and magnetic fields, the number of massless Weyl fermions of a given chirality is not conserved. In condensed matter,…

强关联电子 · 物理学 2026-02-20 Shantonu Mukherjee , Sayantan Sharma , Hridis K. Pal

We study constraints on thermal phase transitions of ${\rm SU}(N_c)$ gauge theories by using the 't Hooft anomaly involving the center symmetry and chiral symmetry. We consider two cases of massless fermions: (i) adjoint fermions, and (ii)…

高能物理 - 理论 · 物理学 2018-05-25 Hiroyuki Shimizu , Kazuya Yonekura

We discuss the central charge in supersymmetric ${\cal N}=2$ sigma models in two dimensions. The target space is a symmetric K\"ahler manifold, CP$(N-1)$ is an example. The U(1) isometries allow one to introduce twisted masses in the model.…

高能物理 - 理论 · 物理学 2009-11-11 M. Shifman , A. Vainshtein , R. Zwicky

We investigate (3+1)d topological orders in fermionic systems with an anomalous $\mathbb{Z}_{2N}^{\mathrm{F}}$ symmetry, where its $\mathbb{Z}_2^{\mathrm{F}}$ subgroup is the fermion parity. Such an anomalous symmetry arises as the discrete…

强关联电子 · 物理学 2026-03-09 Meng Cheng , Juven Wang , Xinping Yang

We study a class of anomalies associated with time-reversal and spatial reflection symmetry in (2+1)D topological phases of matter. In these systems, the topological quantum numbers of the quasiparticles, such as the fusion rules and…

强关联电子 · 物理学 2018-09-26 Maissam Barkeshli , Meng Cheng

We use the theory of topological modular forms to constrain bosonic holomorphic CFTs, which can be viewed as $(0,1)$ SCFTs with trivial right-moving supersymmetric sector. A conjecture by Segal, Stolz and Teichner requires the constant term…

高能物理 - 理论 · 物理学 2023-07-05 Ying-Hsuan Lin , Du Pei

It is well known that two-dimensional fermionic systems with a nonzero Chern number must break the time reversal symmetry, manifested by the appearance of chiral edge modes on an open boundary. Such an incompatibility between topology and…

强关联电子 · 物理学 2023-12-05 Shang-Qiang Ning , Yang Qi , Zheng-Cheng Gu , Chenjie Wang
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