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In this work, the mass of the Higgs boson is calculated, its comparison with the W and Z boson masses established, and the μ 2 and λ parameters of the Higgs potential are fixed. This is done by looking at the ground states of three and four dimensional harmonic oscillators, and getting inferences from the strong black hole as well the MIT bag model formalisms. An "exact" relationship linking the masses of these bosons, advanced by DNA Forrester, is also taken in account. The Standard Model (SM) of Particle Physics is a theory describing the visible part of the stuff of the universe [1]. The SM Lagrangian contains fermionic fields, which excitations are quarks and leptons, and bosonic fields the mediators of the interactions and having as excitations the photon, W and Z bosons, and gluons. However, in order to give leptons and quarks (current) masses, and also to give masses to the W and Z bosons of the weak interactions, these fermionic and bosonic fields must interact (couple) with another spin-zero field:-the Higgs field. The quantum excitation of the Higgs field produces a Higgs boson (please see: "Higgs boson" in Wikipedia [2], and references cited therein). The Higgs mechanism, indeed also proposed by Robert Brout and François Englert; Gerald Guralnik, C. Richard Hagen, and Tom Kibble; besides Peter Higgs himself, gives particles their masses (current masses in the quark case).[3,4,5].The Higgs mechanism works through the process called spontaneous symmetry breaking [6]. As was pointed out by Wilczek [7], the mass of the Higgs particle itself is not explained in the theory, but appears as a free parameter. Here we are going to focus on the Higgs and Electroweak sectors of the SM.
We will describe the Higgs mechanism, a theory accounting for the mass of fundamental particles which make up the baryonic matter in our universe. The mathematical methods needed to investigate the nature of the coupling between the Higgs field and soon-to-be massive gauge field will be discussed, and we will explore how a mass term arises.
EPJ Web of Conferences, 2013
The present knowledge on the Higgs-like boson discovered at the LHC is summarized. The data accumulated so far are consistent with the Standard Model predictions and put interesting constraints on alternative scenarios of electroweak symmetry breaking. The measured couplings to gauge bosons and third-generation fermions indicate that a Higgs particle has indeed been found. More precise data are needed to clarify whether it is the unique Higgs boson of the Standard Model or the first member of a new variety of dynamical (either elementary or composite) fields.
Indian Journal of Physics, 2023
The Higgs boson plays a central role in the Standard Model, as well as in theories which go beyond it. This article is therefore divided into two parts. The first takes s historical approach and shows how the mass problem entered weak interaction theory from the beginning and how it was solved by invoking the Higgs boson. This is followed by a construction of the Glashow-Salam-Weinberg model, again stressing the role played by the Higgs doublet. This part culminates in the Higgs boson discovery of 2012. The second part first discusses the shortcomings of the Standard Model and then touches upon the major theories which try to improve upon it, mostly with profound consequences on the Higgs sector. This is followed up by short descriptions of a number of popular extensions of the Higgs sector, and culminates in a brief introduction to effective field theory approaches to studying the Higgs sector.
International Studies in the Philosophy of Science, 2008
This paper explores the argument structure of the concept of spontaneous symmetry breaking in the electroweak gauge theory of the Standard Model: the so-called Higgs mechanism. As commonly understood, the Higgs argument is designed to introduce the masses of the gauge bosons by a spontaneous breaking of the gauge symmetry of an additional field, the Higgs field. The technical derivation of the Higgs mechanism, however, consists in a mere re-shuffling of degrees of freedom by transforming the Higgs Lagrangian in a gauge-invariant manner. This already raises serious doubts about the adequacy of the entire manoeuvre. It will be shown that no straightforward ontic interpretation of the Higgs mechanism is tenable since gauge transformations possess no real instantiations. In addition, the explanatory value of the Higgs argument will be critically examined.
2012
This paper is an overview of Higgs particle physics. This discusses the particle physics behind why the Higgs particle was presumed to exist, some aspects of its detection and how the Higgs particle might be a door into deeper foundations. 1 How the Higgs particle saved physics The reasons for the Higgs particle are often not discussed. It is common to hear the lore that that Higgs field produces the mass of particles. While this is the case, the most important role the Higgs field plays is in rescuing quantum field theory from a complicated problem with massive vector bosons. The weak interactions at low energy are mediated by massive vector bosons. At sufficiently high energy this theory is not causally consistent. The mass is a degree of freedom, or equivalently a longitudinal mode, which is absorbed by the gauge bosons that is massless at higher energy. This means weak interactions at high energy are mediated by massless gauge bosons at high energy. This prevents the theory of w...
Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics, 2013
I examine the construction process of the Higgs mechanism and its subsequent use by Steven Weinberg to formulate the electroweak theory in particle physics. I characterize the development of the Higgs mechanism to be a historical process that is guided through analogies drawn to the theories of solid-state physics and that is progressive through diverse contributions from a number of physicists working independently. I also offer a detailed comparative study that analyzes the similarities and differences in these contributions. 7 In quantum mechanics, "parity" transformations refer to the inversions of coordinate-axes in the form r -r. The conservation of parity states that the field equations describing a quantum mechanical system remain unchanged under parity transformations.
Journal of Modern Physics, 2023
The electromagnetic force, strong nuclear force, weak nuclear force, and gravitational force are the four fundamental forces of nature. The Standard Model (SM) succeeded in combining the first three forces to describe the most basic building blocks of matter and govern the universe. Despite the model’s great success in resolving many issues in particle physics but still has several setbacks and limitations. The model failed to incorporate the fourth force of gravity. It infers that all fermions and bosons are massless contrary to experimental facts. In addition, the model addresses neither the 95% of the universe’s energy of Dark Matter (DM) and Dark Energy (DE) nor the universe’s expansion. The Complex Field Theory (CFT) identifies DM and DE as complex fields of complex masses and charges that encompasses the whole universe, and pervade all matter. This presumption resolves the issue of failing to detect DM and DE for the last five decades. The theory also presents a model for the universe’s expansion and presumes that every material object carries a fraction of this complex field proportional to its mass. These premises clearly explain the physical nature of the gravitational force and its complex field and pave the way for gravity into the SM. On the other hand, to solve the issue of massless bosons and fermions in the SM, Higgs mechanism introduces a pure and abstractive theoretical model of unimaginable four potentials to generate fictitious bosons as mass donors to fermions and W} and Z bosons. The CFT in this paper introduces, for the first time, a physical explanation to the mystery of the mass formation of particles rather than Higgs’pure mathematical derivations. The analyses lead to uncovering the mystery of electron-positron production near heavy nuclei and never in a vacuum. In addition, it puts a constraint on Einstein’s mass-energy equation that energy can never be converted to mass without the presence of dense dark matter and cannot be true in a vacuum. Furthermore, CFT provides different perspectives and resolves real-world physics concepts such as the nuclear force, Casimir force, Lamb’s shift, and the anomalous magnetic moment to be published elsewhere.
AIP Conference Proceedings, 2008
Old and new ideas regarding Higgs physics are reviewed. We first summarize the quadratic divergence / hierarchy problem which strongly suggests that the SM Higgs sector will be supplemented by new physics at high scales. We next consider means for delaying the hierarchy problem of the SM Higgs sector to unexpectedly high scales. We then outline the properties of the most ideal Higgs boson. The main advantages of a supersymmetric solution to the high scale problems are summarized and the reasons for preferring the next-to-minimal supersymmetric model over the minimal supersymmetric model in order to achieve an ideal Higgs are emphasized. This leads us to the strongly motivated scenario in which there is a Higgs h with SM-like WW, ZZ couplings and m h ∼ 100 GeV that decays via h → aa with m a < 2m b , where m a > 2m τ is preferred, implying a → τ + τ -. The means for detecting an h → aa → 4τ signal are then discussed. Some final cautionary and concluding remarks are given.
2021
The spontaneous symmetry breaking for the massless scalar field naturally arises from the frame-work of the effective theory (the non-minimal coupling of gravity to a scalar field). A magic key ingredient is to add the large vacuum energy density, contributing to the cosmological constant, to the Lagrangian density. By applying this modified spontaneous symmetry breaking with the gauge theory (called modified Higgs mechanism), the inflation physics and the electroweak phase transition can be generated from the same framework. However, this comes with the huge price-the large cosmological constant which is known as the dark energy problem. The possible solution of this issue is also discussed.
viXra, 2021
In this paper we use the Metre-Second System (MS System) of Units to derive a precise theoretical value for the magnitude of the Higgs field and explore its implications. E H = 9.638732018E-32 [m-2 s-4 ] Higgs field In addition, we use the value of the Higgs field to derive the mass values for the Higgs boson, the W boson, the Tau lepton, the proton and the electron. M H = 2.235682861E-25 kg [m 1 s-6 ] = 125.412616 GeV/c 2 mass of Higgs boson M W = 1.433217602E-25 kg [m 1 s-6 ] = 80.397576348 GeV/c 2 mass of W boson M = 3.168372989E-27 kg [m 1 s-6 ] = 1777.3269 MeV/c 2 mass of Tau lepton m p = 1.672621898E-27 kg [m 1 s-6 ] = 938.27211 MeV/c 2 proton rest mass m e = 9.109383558E-31 kg [m 1 s-6 ] = 0.51099894 MeV/c 2 electron rest mass
A brief overview is given of the theory of Higgs bosons and electroweak symmetry breaking that is relevant for the Higgs physics program at the Linear Collider.
Physics Letters B, 2013
We investigate the physical implications of formulating the electroweak (EW) part of the Standard Model (SM) in terms of a superconnection involving the supergroup SU (2/1). In particular, we relate the observed Higgs mass to new physics at around 4 TeV. The ultraviolet incompleteness of the superconnection approach points to its emergent nature. The new physics beyond the SM is associated with the emergent supergroup SU (2/2), which is natural from the point of view of the Pati-Salam model. Given that the Pati-Salam group is robust in certain constructions of string vacua, these results suggest a deeper connection between low energy (4 TeV) and high energy (Planck scale) physics via the violation of decoupling in the Higgs sector.
A version of the Standard Model is considered, where the electroweak symmetry breaking is provided by cosmological initial data given for the zeroth Fourier harmonic of the Higgs field $<\phi>$. The initial data symmetry breaking mechanism removes the Higgs field contribution to the vacuum energy density, possible creation of monopoles, and tachion behavior at high energies, if one imposes an ``inertial'' condition on the Higgs potential $\textsf{V}_{\rm Higgs}(<\phi>)=0$. The requirement of zero radiative corrections to this {\em inertial} condition coincides with the limiting point of the vacuum stability in the Standard Model. The latter together with the direct experimental limit gives the prediction for the mass of the Higgs boson to be in the range $114 < m_h \lsim 134$ GeV.
Chaos Solitons & Fractals, 2007
The Higgs mechanism is an essential but elusive component of the Standard Model of particle physics. Without it Yang-Mills gauge theories would have been little more than a warm-up exercise in the attempt to quantize gravity rather than serving as the basis for the Standard Model. This article focuses on two problems related to the Higgs mechanism clearly posed in Earman’s recent papers (Earman 2003, 2004a, 2004b): what is the gauge-invariant content of the Higgs mechanism, and what does it mean to break a local gauge symmetry?
where m is the rest mass of the particle and the value of k, 1 ≤ k ≤ 2, need not be fixed at this time.
Physical Review D, 2012
The purpose of this paper is to present a unified description of mass generation mechanisms that have been investigated so far and that are called the Mach and Higgs proposals. In our mechanism, gravity acts merely as a catalyst and the final expression of the mass depends neither on the intensity nor on the particular properties of the gravitational field. We shall see that these two strategies to provide mass for all bodies that operate independently and competitively can be combined into a single unified theoretical framework. As a consequence of this new formulation we are able to present an answer to the question: what is the origin of the mass of the Higgs boson?
A short review of the theory and phenomenology of Higgs bosons is given, with focus on the Standard Model (SM) and the minimal supersymmetric extension of the Standard Model (MSSM). The potential for Higgs boson discovery at the Tevatron and LHC, and precision Higgs studies at the LHC and a future e + e − linear collider are briefly surveyed. The phenomenological challenge of the approach to the decoupling limit, where the properties of the lightest CP-even Higgs boson of the MSSM are nearly indistinguishable from those of the SM Higgs boson is emphasized.
Physical Review D, 2010
An updated global analysis within the Standard Model (SM) of all relevant electroweak precision and Higgs boson search data is presented with special emphasis on the implications for the Higgs boson mass, MH . Included are, in particular, the most recent results on the top quark and W boson masses, updated and significantly shifted constraints on the strong coupling constant, αs, from τ decays and other low energy measurements such as from atomic parity violation and neutrino deep inelastic scattering. The latest results from searches for Higgs production and decay at the Tevatron are incorporated together with the older constraints from LEP 2. I find a trimodal probability distribution for MH with a fairly narrow preferred 90% CL window, 115 GeV ≤ MH ≤ 148 GeV.
International Journal of Theoretical Physics, 2015
As it is commonly understood, the Higgs mechanism is designed to introduce the masses of the gauge bosons by a spontaneous breaking of the gauge symmetry by an additional field. In this paper we present three approaches outlining a conceptually and mathematically neat frameworks within which we reproduce the mass generation mechanism essential for the Standard Model. The first framework is based on the idea of the field transformations, where the only fields that remain in the theory are gauge invariant. More precisely, the fields that do transform under a gauge transformation are factored out from the theory. These fields are what could be seen as the Goldstone bosons. The second framework is based on the inclusion into the theory of the gauge-group parameters as the scalar dynamical fields, in parallel with the standard Goldstone bosons. The third approach present a spontaneously broken noncommutative theory, which is broken by a scalar field, providing a new symmetry breaking term to the gauge field, a term not belonging to the gauge field itself.
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