SearcharxivSearch

arXiv · 2407.00807

Spontaneous Symmetry Breaking: From the Effective Action to Cosmological Phase Transitions in the Standard Model and Beyond

Abstract

The primary objective of this work is to investigate the cosmological phase transitions in the early Universe, with a focus on the electroweak phase transition in the Standard Model and its extensions. In the Standard Model, the spontaneously broken electroweak symmetry at zero temperature is restored in the early Universe due to finite-temperature effects. This phenomenon is studied using the effective potential at finite temperatures, which determines the true vacuum state of the theory. Symmetry restoration at high temperatures is also studied by the finite-temperature field theory introduced to derive the Feynman rules at finite temperatures using the imaginary-time formalism. Furthermore, we present the theory of cosmological phase transitions, focusing on the concepts of thermal tunneling and bubble nucleation. We additionally discuss the observed baryon asymmetry of the Universe to formulate the conditions for baryogenesis and describe electroweak baryogenesis. Therefore, the one-loop effective potential in the Standard Model at finite temperatures is derived in detail including the ring corrections to study further the electroweak baryogenesis. Our results indicate that the electroweak phase transition is not strong enough to explain the observed baryon asymmetry of the Universe. On the other hand, the real singlet extensions of the Standard Model describe a strong enough electroweak phase transition and the observed baryon asymmetry of the Universe. These extensions are also discussed including a dimension-six operator, which originates from an effective field theory. In particular, the parameter space of this singlet extension is examined extensively, while it is restricted by numerous phenomenological constraints, such as the invisible Higgs decay width.

Explore related subjects

Keep this discovery

BibTeXRIS

Apostolos Giovanakis. 2024-06-30. Spontaneous Symmetry Breaking: From the Effective Action to Cosmological Phase Transitions in the Standard Model and Beyond. https://arxiv.org/abs/2407.00807

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