Higher-group symmetry of (3+1)D fermionic $\mathbb{Z}_2$ gauge theory: logical CCZ, CS, and T gates from higher symmetry
- URL: http://arxiv.org/abs/2311.05674v3
- Date: Sat, 6 Apr 2024 13:41:10 GMT
- Title: Higher-group symmetry of (3+1)D fermionic $\mathbb{Z}_2$ gauge theory: logical CCZ, CS, and T gates from higher symmetry
- Authors: Maissam Barkeshli, Po-Shen Hsin, Ryohei Kobayashi,
- Abstract summary: We study the higher-group structure in (3+1)D $mathbbZ$ gauge theory with an emergent fermion.
Our considerations also imply the possibility of a logical $T$ gate by placing the code on $mathbbRP3$ and pumping a $p+ip$ topological state.
- Score: 0.0
- License: http://creativecommons.org/licenses/by/4.0/
- Abstract: It has recently been understood that the complete global symmetry of finite group topological gauge theories contains the structure of a higher-group. Here we study the higher-group structure in (3+1)D $\mathbb{Z}_2$ gauge theory with an emergent fermion, and point out that pumping chiral $p+ip$ topological states gives rise to a $\mathbb{Z}_{8}$ 0-form symmetry with mixed gravitational anomaly. This ordinary symmetry mixes with the other higher symmetries to form a 3-group structure, which we examine in detail. We then show that in the context of stabilizer quantum codes, one can obtain logical CCZ and CS gates by placing the code on a discretization of $T^3$ (3-torus) and $T^2 \rtimes_{C_2} S^1$ (2-torus bundle over the circle) respectively, and pumping $p+ip$ states. Our considerations also imply the possibility of a logical $T$ gate by placing the code on $\mathbb{RP}^3$ and pumping a $p+ip$ topological state.
Related papers
- Geometry of degenerate quantum states, configurations of $m$-planes and invariants on complex Grassmannians [55.2480439325792]
We show how to reduce the geometry of degenerate states to the non-abelian connection $A$.
We find independent invariants associated with each triple of subspaces.
Some of them generalize the Berry-Pancharatnam phase, and some do not have analogues for 1-dimensional subspaces.
arXiv Detail & Related papers (2024-04-04T06:39:28Z) - Quantum charges of harmonic oscillators [55.2480439325792]
We show that the energy eigenfunctions $psi_n$ with $nge 1$ are complex coordinates on orbifolds $mathbbR2/mathbbZ_n$.
We also discuss "antioscillators" with opposite quantum charges and the same positive energy.
arXiv Detail & Related papers (2024-04-02T09:16:18Z) - Quantum Current and Holographic Categorical Symmetry [62.07387569558919]
A quantum current is defined as symmetric operators that can transport symmetry charges over an arbitrary long distance.
The condition for quantum currents to be superconducting is also specified, which corresponds to condensation of anyons in one higher dimension.
arXiv Detail & Related papers (2023-05-22T11:00:25Z) - Higher-group symmetry in finite gauge theory and stabilizer codes [3.8769921482808116]
A large class of gapped phases of matter can be described by topological finite group gauge theories.
We derive the $d$-group global symmetry and its 't Hooft anomaly for topological finite group gauge theories in $(d+1) space-time dimensions.
We discuss several applications, including the classification of fermionic SPT phases in (3+1)D for general fermionic symmetry groups.
arXiv Detail & Related papers (2022-11-21T19:00:00Z) - Non-perturbative constraints from symmetry and chirality on Majorana
zero modes and defect quantum numbers in (2+1)D [0.0]
In (1)D topological phases, unpaired Majorana zero modes (MZMs) can arise only if the internal symmetry group $G_f$ of the ground state splits as $G_f = G_b times mathbbZf$.
In contrast, (2+1)D topological superconductors (TSC) can host unpaired MZMs at defects even when $G_f$ is not of the form $G_b times mathbbZf$.
arXiv Detail & Related papers (2022-10-05T18:00:00Z) - Beyond the Berry Phase: Extrinsic Geometry of Quantum States [77.34726150561087]
We show how all properties of a quantum manifold of states are fully described by a gauge-invariant Bargmann.
We show how our results have immediate applications to the modern theory of polarization.
arXiv Detail & Related papers (2022-05-30T18:01:34Z) - Classification of (2+1)D invertible fermionic topological phases with
symmetry [2.74065703122014]
We classify invertible fermionic topological phases of interacting fermions with symmetry in two spatial dimensions for general fermionic symmetry groups $G_f$.
Our results also generalize and provide a different approach to the recent classification of fermionic symmetry-protected topological phases by Wang and Gu.
arXiv Detail & Related papers (2021-09-22T21:02:07Z) - Fermion and meson mass generation in non-Hermitian Nambu--Jona-Lasinio
models [77.34726150561087]
We investigate the effects of non-Hermiticity on interacting fermionic systems.
We do this by including non-Hermitian bilinear terms into the 3+1 dimensional Nambu--Jona-Lasinio (NJL) model.
arXiv Detail & Related papers (2021-02-02T13:56:11Z) - A $H^{3}(G,{\mathbb T})$-valued index of symmetry protected topological
phases with on-site finite group symmetry for two-dimensional quantum spin
systems [0.0]
We consider SPT-phases with on-site finite group $G$ symmetry $beta$ for two-dimensional quantum spin systems.
We show that they have $H3(G,mathbb T)$-valued invariant.
arXiv Detail & Related papers (2021-01-02T11:22:55Z) - The Geometry of Time in Topological Quantum Gravity of the Ricci Flow [62.997667081978825]
We continue the study of nonrelativistic quantum gravity associated with a family of Ricci flow equations.
This topological gravity is of the cohomological type, and it exhibits an $cal N=2$ extended BRST symmetry.
We demonstrate a standard one-step BRST gauge-fixing of a theory whose fields are $g_ij$, $ni$ and $n$, and whose gauge symmetries consist of (i) the topological deformations of $g_ij$, and (ii) the ultralocal nonrelativistic limit of space
arXiv Detail & Related papers (2020-11-12T06:57:10Z) - Absolute anomalies in (2+1)D symmetry-enriched topological states and
exact (3+1)D constructions [0.0]
We show how to compute the anomaly for symmetry-enriched topological (SET) states of bosons in complete generality.
We present an exactly solvable Hamiltonian for the system and demonstrate explicitly a (2+1)D $G$ symmetric surface termination.
Our results can also be viewed as providing a method to compute the $mathcalH4(G, U(1))$ obstruction that arises in the theory of $G$-crossed braided tensor categories.
arXiv Detail & Related papers (2020-03-25T18:00:03Z)
This list is automatically generated from the titles and abstracts of the papers in this site.
This site does not guarantee the quality of this site (including all information) and is not responsible for any consequences.