Abstract

We find a simple brane configuration in the IKKT matrix model which resembles the standard model at low energies, with a second Higgs doublet and right-handed neutrinos. The electroweak sector is realized geometrically in terms of two minimal fuzzy ellipsoids, which can be interpreted in terms of four point-branes in the extra dimensions. The electroweak Higgs connects these branes and is an indispensable part of the geometry. Fermionic would-be zero modes arise at the intersections with two larger branes, leading precisely to the correct chiral matter fields at low energy, along with right-handed neutrinos which can acquire a Majorana mass due to a Higgs singlet. The larger branes give rise to $SU(3)_c$, extended by $U(1)_B$ and another $U(1)$ which are anomalous at low energies and expected to disappear. At higher energies, mirror fermions and additional fields arise, completing the full ${\cal N}=4$ supersymmetry. The brane configuration is a solution of the model, assuming a suitable effective potential and a non-linear stabilization of the singlet Higgs. The basic results can be carried over to ${\cal N}=4$ $SU(N)$ super-Yang-Mills on ordinary Minkowski space with sufficiently large $N$.

Highlights

  • IntroductionThe main result of this paper is to establish a background of the IKKT or IIB model [1] with lowenergy physics close to that of the standard model

  • In order to recover the standard model from the matrix model, all fields must be realized as matrices in the adjoint of some big U (N ) gauge group

  • We have shown that the IKKT model can behave very to the standard model at low energies, for suitable backgrounds

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Summary

Introduction

The main result of this paper is to establish a background of the IKKT or IIB model [1] with lowenergy physics close to that of the standard model. Zahn dimensions, which lead to fermionic and bosonic low-energy excitations governed by an effective action which is close to the standard model, with all the correct quantum numbers. This is a very remarkable result, given the non-chiral nature of N = 4 SYM. Both problems are resolved, by realizing the Higgs as an intrinsic part of two minimal fuzzy ellipsoids (consisting of two quantum cells) which are part of Du and Dd , respectively These ellipsoids intersect DB and Dl at their antipodal points, leading to localized chiral fermions. We elaborate the reduction of the fermions to four dimensions

The matrix model
Noncommutative branes and gauge theory
Fields and symmetries
Higgs from deconstructing compact branes
Intersecting brane solutions
Nl be embedded as
S2 intersecting R2
Gauginos
Fermion masses and Yukawas
Symmetry breaking and four-dimensional fields
Hierarchical symmetry breaking
Four-dimensional gauge bosons and masses
Further aspects
Findings
Discussion and conclusion
Full Text
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