2004/11/30 by Ton Dijkstra, T. P. T. Dijkstra, L. R. Huiszoon +3 · 13 citations
Physics and Astronomy · #Black Holes and Theoretical Physics #Electron #Gauge (firearms) #Gauge boson #Gauge theory #Higgs boson #Lepton #Minimal Supersymmetric Standard Model #Orientifold #Particle physics #Particle physics theoretical and experimental studies #Physics #Quantum Chromodynamics and Particle Interactions #Quantum mechanics #Quark #Standard Model (mathematical formulation) #Supersymmetry #Theoretical physics #Vector boson #hep-th
paper · pdf · doi:10.1016/j.nuclphysb.2004.12.032
published as Nucl.Phys.B710:3-57,2005 · 59 pages, LaTeX. [v2]: References, some clarifications and data added. [v3]: Removed incorrect statement added in v2, modified references
arxiv created 2004/12/04 · openalex publication_date 2005/01/13 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We present supersymmetric, tadpole-free d=4,N=1 orientifold vacua with a three family chiral fermion spectrum that is identical to that of the Standard Model. Starting with all simple current orientifolds of all Gepner models we perform a systematic search for such spectra. We consider several variations of the standard four-stack intersection brane realization of the standard model, with all quarks and leptons realized as bifundamentals and perturbatively exact baryon and lepton number symmetries, and with a U(1)Y vector boson that does not acquire a mass from Green-Schwarz terms. The number of supersymmetric Higgs pairs H1 + H2 is left free. In order to cancel all tadpoles, we allow a "hidden" gauge group, which must bechirally decoupled from the standard model. We also allow for non-chiral mirror-pairs of quarks and leptons, non-chiral exotics and (possibly chiral) hidden, standard model singlet matter, as well as a massless B-L vector boson. All of these less desirable features are absent in some cases, although not simultaneously. In particular, we found cases with massless Chan-Paton gauge bosons generating nothing more than SU(3) x SU(2) x U(1). We obtain almost 180000 rationally distinct solutions (not counting hidden sector degrees of freedom), and present distributions of various quantities. We analyse the tree level gauge couplings, and find a large range of values, remarkably centered around the unification point.