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The two discrete generators of the full Lorentz group $O(1,3)$ in $4D$ spacetime are typically chosen to be parity inversion symmetry $P$ and time reversal symmetry $T$, which are responsible for the four topologically separate components…

General Physics · Physics 2023-07-17 Wanpeng Tan

We present a calculating method for the quark and lepton mixing angles. After a general discussion in field theoretic models, we present a working model from a string compactification through $Z_{12-I}$ orbifold compactification. It is…

High Energy Physics - Phenomenology · Physics 2018-09-12 Jihn E. Kim

We study the flavor structures of zero-modes, which are originated from the modular symmetry on $T^2_1\times T^2_2$ and its orbifold with magnetic fluxes. We introduce the constraint on the moduli parameters by $\tau_2=N\tau_1$, where…

High Energy Physics - Theory · Physics 2024-09-05 Tatsuo Kobayashi , Kaito Nasu , Ryusei Nishida , Hajime Otsuka , Shohei Takada

We study moduli stabilization in 4D effective field theories with Sp(4,$\mathbb{Z}$) self-duality inspired by heterotic orbifold compactifications with Wilson lines. The target-space duality group of these theories is enhanced from…

High Energy Physics - Theory · Physics 2026-05-08 Jacob M. Leedom , Nicole Righi , Alexander Westphal

Starting from the superconformal algebras associated with $G_2$ manifolds, I extend the algebra to the manifolds with spin(7) holonomy. I show how the mirror symmetry in manifolds with spin(7) holonomy arises as the automorphism in the…

High Energy Physics - Theory · Physics 2011-10-26 Wu-yen Chuang

In orbifold family unification on the basis of $SU(N)$ gauge theory on the six-dimensional space-time $M^4\times T^2/Z_m$ ($m=2, 3, 4, 6$), enormous numbers of models with three families of the standard model matter multiplets are derived…

High Energy Physics - Phenomenology · Physics 2018-09-12 Yuhei Goto , Yoshiharu Kawamura

We demonstrate how to find modular discrete symmetry groups for $Z_N$ orbifolds. The $Z_7$ orbifold is treated in detail as a non-trivial example of a $(2,2)$ orbifold model. We give the generators of the modular group for this case which,…

High Energy Physics - Theory · Physics 2015-06-26 J. Erler , M. Spalinski

The framework of compactified heterotic string theory offers consistent ultraviolet (UV) completions of the Standard Model (SM) of particle physics. In this approach, the existence of flavor symmetries beyond the SM is imperative and the…

High Energy Physics - Phenomenology · Physics 2023-02-27 Andreas Trautner

We present a unified framework demonstrating how the spinor complex Lorentz group SL(2,C)/Z\_2 is realized as a canonical subgroup within a four-dimensional complex Riemannian manifold. Building on the complex, holomorphic metric extension…

High Energy Physics - Theory · Physics 2025-06-25 John. W. Moffat , Ethan. J. Thompson

In the four-dimensional effective theory from string compactification discrete flavor symmetries arise from symmetric structure of the compactified space and generally contain both the $R$ symmetry and non-$R$ symmetry. We point out that a…

High Energy Physics - Phenomenology · Physics 2009-11-07 Y. Abe , C. Hattori , M. Ito , M. Matsuda , M. Matsunaga , T. Matsuoka

We review efforts in string model building, focusing on the heterotic orbifold compactifications. We survey how one can, starting from an explicit string theory, obtain models which resemble Nature. These models exhibit the standard model…

High Energy Physics - Theory · Physics 2024-01-09 Saul Ramos-Sanchez , Michael Ratz

The square-root of Siegel modular forms of CHL Z_N orbifolds of type II compactifications are denominator formulae for some Borcherds-Kac-Moody Lie superalgebras for N=1,2,3,4. We study the decomposition of these Siegel modular forms in…

High Energy Physics - Theory · Physics 2023-02-22 Suresh Govindarajan , Mohammad Shabbir

Mirror symmetry was first observed in worldsheet string constructions and shown to have profound implications in the Effective Field Theory (EFT) limit of string compactifications, and for the properties of Calabi-Yau manifolds. It opened…

High Energy Physics - Theory · Physics 2024-11-07 Alon E. Faraggi

We study Gauge-Higgs unification model on the orbifold $S^{1}/Z_{2}$ based on the extended SM gauge group $G_{SM}^{ex}=SU(2)_{L} \times U(1)_{Y} \times SO(3)_{F}$. The group $SO(3)_{F}$ is treated as a chiral gauged flavour symmetry.…

High Energy Physics - Phenomenology · Physics 2007-06-01 Michael Olschewsky

Let M be a Weinstein four-manifold mirror to Y\D for (Y,D) a log Calabi--Yau surface; intuitively, this is typically the Milnor fibre of a smoothing of a cusp singularity. We introduce two families of symplectomorphisms of M: Lagrangian…

Symplectic Geometry · Mathematics 2026-03-25 Paul Hacking , Ailsa Keating

The framework of compactified heterotic string theory offers consistent ultraviolet (UV) completions of the Standard Model (SM) of particle physics. In this approach, the existence of flavor symmetries beyond the SM is imperative and the…

High Energy Physics - Theory · Physics 2022-04-15 Andreas Trautner

For any positive integer $g$, we introduce the moduli space $\mathcal{A}^F_g =[\mathcal{H}_g/P_g(\mathbb{Z})]$ parametrizing $g$-dimensional principally polarized abelian varieties $V_\tau$ together with a Strominger-Yau-Zalsow (SYZ)…

Symplectic Geometry · Mathematics 2025-03-28 Haniya Azam , Catherine Cannizzo , Heather Lee , Chiu-Chu Melissa Liu

The grand unification of flavor(GUF) in extra dimensions is discussed. After reviewing the old GUF, I present a GUF model SU(7) in 5D with the recently popular field theoretic orbifold compactification.

High Energy Physics - Phenomenology · Physics 2017-08-23 Jihn E. Kim

We associate a Jacobi form over a rank s lattice to N=2, D=4 heterotic string compactifications which have s Wilson lines at a generic point in the vector multiplet moduli space. Jacobi forms of index m=1 and m=2 have appeared earlier in…

High Energy Physics - Theory · Physics 2015-06-17 Caner Nazaroglu

We have investigated the modular binary octahedral group $2O$ as a flavor symmetry to explain the structure of Standard Model. The vector-valued modular forms in all irreducible representations of this group are constructed. We have…

High Energy Physics - Phenomenology · Physics 2024-10-22 Gui-Jun Ding , Xiang-Gan Liu , Jun-Nan Lu , Ming-Hua Weng