SearcharxivSearch

arXiv · hep-ph/9308357

Unification of Couplings and the Top Quark Sector in the Minimal Supersymmetric Standard Model

Abstract

I analyze the predictions for the strong gauge coupling, $α_3(M_Z) $, and the top quark and light Higgs masses in the framework of gauge and bottom-tau Yukawa coupling unification in the minimal supersymmetric standard model. These predictions depend on the effective supersymmetric threshold scale $T_{SUSY}$, which is only very slightly dependent on the squark and slepton masses, and strongly dependent on the Higgsino masses as well as on the mass ratio of the gauginos of the strong and weak interactions. Within the minimal supersymmetry breaking scheme and for supersymmetric masses below or of the order of 1 TeV, I obtain $α_3(M_Z) \geq 0.116$, while, if the running bottom quark mass at the physical mass is constrained to be $ m_b(M_b) \leq 4.1 $GeV, then, for moderate values of $\tan β$, perturbative unification is achieved only if $α_3(M_Z) \leq 0.124$. Unification of gauge and bottom-tau Yukawa couplings yield predictions for the top quark mass, 140 GeV $\leq M_t \leq 210 $ GeV for $1 \leq \tan β\leq 30$, which are remarkably close to the infrared quasi fixed point values for this quantity. For the light Higgs mass I obtain $m_h \leq 130(165)$ GeV if the characteristic squark mass is below 1 (10) TeV.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

M. Carena. 1993-08-29. Unification of Couplings and the Top Quark Sector in the Minimal Supersymmetric Standard Model. https://arxiv.org/abs/hep-ph/9308357

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Axionic Wormholes in Metric-Affine Gravity

The axion is a promising candidate for solving the strong CP problem. To solve this problem, the global U(1) symmetry must be preserved to a high degree of accuracy. However, it is well known that global symmetries are explicitly violated by quantum gravity effects, giving rise to what is referred to as the axion quality problem. In this paper, we investigate axionic wormholes as a source of explicit U(1) violation in Metric-Affine Gravity. This framework allows for spacetime torsion and non-metricity, which accommodate additional curvature-like and topological terms, such as the Holst and Nieh--Yan terms, that are absent from the metric and Palatini formalisms. We show that non-minimal couplings to these terms modify the wormhole dynamics and enhance the Euclidean wormhole action, thereby alleviating the axion quality problem. We also find that the viable parameter space is enlarged when two of these couplings are simultaneously present. We further identify representative parameter regions where the alleviation of the axion quality problem is compatible with inflationary constraints.

hep-ph

Qubit-Qutrit Quantum Tomography of hadronic $\Lambda\phi$ and $\Lambda K^{\ast 0}$ systems

Quantum-information observables have emerged in recent years as new tools in nuclear and particle physics, from entanglement in top-quark pairs to spin correlations in $\Lambda\bar{\Lambda}$ production. Extending these studies to unequal-spin hadronic final states poses a fundamental challenge: the $6\times6$ density matrix of a qubit-qutrit system contains 35 independent spin parameters, but the decays of $\Lambda V$ pairs, with $V=\phi$ or $K^{*0}$, provide access to only 23 due to the hidden vector polarization from the strong decay. In this Letter, we formulate a qubit-qutrit quantum tomography (QQQT) technique for these spin-$\tfrac{1}{2}\otimes1$ systems and establish exact criteria for entanglement certification from the \textit{incomplete} density matrix. Compared with the $\Lambda\bar{\Lambda}$ system, QQQT of $\Lambda\phi$ and $\Lambda K^{*0}$ provides a new probe of nonperturbative QCD hadronization, enabling a direct comparison of the spin evolution of entangled quark pairs produced from the vacuum as they hadronize into a baryon or a vector meson.

hep-ph

Twist decomposition of exclusive heavy meson production cross sections

We study the twist decomposition of the total cross sections for exclusive heavy vector meson electroproduction and photoproduction in the $\gamma^\ast p$ processes, within the leading logarithmic $1/x$ BFKL formalism. The Mellin transforms of the impact factors of the vector meson are calculated. We show that the higher twist contributions are strongly suppressed in the low-$x$ kinematical regime. Possible enhancement of the higher twists effects for nuclei targets is discussed.

hep-ph