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Related papers: Vector boson mass generation without new fields

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We consider the contributions to the neutrinoless double beta decays in a $SU(3)_L\otimes U(1)_N$ electroweak model. We show that for a range of the parameters in the model there are diagrams involving vector-vector-scalar and trilinear…

High Energy Physics - Phenomenology · Physics 2009-10-31 J. C. Montero , C. A. de S. Pires , V. Pleitez

If a global chiral symmetry is explicitly broken by anomalies in nonabelian gauge theories, a pseudo Nambu-Goldstone boson (axion) associated with a spontaneous breakdown of such a global symmetry acquires a mass through nonperturbative…

High Energy Physics - Phenomenology · Physics 2009-09-29 Yasunori Nomura , T. Watari , T. Yanagida

We extend the left-right symmetric model with an additional non-abelian $SU(2)$ gauge symmetry. The particle content is augmented by one generation of vector-like fermions transforming under the fundamental representation of this new gauge…

High Energy Physics - Phenomenology · Physics 2026-03-10 Yassine Bouzeraib , Mohamed Sadek Zidi

Four apparently different bosonizations of the $U_q(su(2)_k)$ quantum current algebra for arbitrary level $k$ have recently been proposed in the literature. However, the relations among them have so far remained unclear except in one case.…

High Energy Physics - Theory · Physics 2009-10-22 A. H. Bougourzi

In a model with a gauge group $SU(3)_H\otimes G_{SM}$, where $SU(3)_H$ is a horizontal symmetry and $G_{SM}=SU(3)_C\otimes SU(2)_L\otimes U(1)_Y$ is the standard model, we propose a radiative mechanism of mass generation mediated by the…

High Energy Physics - Phenomenology · Physics 2014-11-17 Albino Hernandez-Galeana

We show that for a force mediated by a vector particle coupled to a conserved U(1) charge, the apparent range and strength can depend on the size and density of the source, and the proximity to other sources. This "chameleon" effect is due…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. E. Nelson , J. Walsh

An alternative for the Higgs mechanism is proposed. It predicts the appearance in the broken phase of a scalar background field which may be interpreted as describing an almost uniform (i.e., homogeneous and isotropic) superfluid condensate…

High Energy Physics - Phenomenology · Physics 2008-02-03 V. Delgado

The vector representation of the linearized gravitational field (the graviton field) or the so called quantum gravitodynamics which describes the motion of masses in a weak gravitational field is employed to understand the unity of the four…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ramchander R. Sastry

The reasons behind the gauge symmetry of the Standard Model, U(1)xSU(2)xSU(3), are still unsettled. One obvious feature is the low dimensionality of all its subgroups. Under certain conditions, a negative answer to the question "why not…

High Energy Physics - Phenomenology · Physics 2017-09-25 Felipe J. Llanes-Estrada , Guillermo Garcia Fernandez , Jesus Guerrero Rojas

We prove the renormalizability of the Curci-Ferrari model with and without auxiliary fields using BRST methods. In both cases we find 5 $Z$ factors instead of 3. We verify our results by explicit one loop calculations. We determine a set of…

High Energy Physics - Theory · Physics 2009-10-28 Jan de Boer , Kostas Skenderis , Peter van Nieuwenhuizen , Andrew Waldron

We make a careful re-examination of the possibility that, in a U(1) extension of the Standard Model, the extra Z' boson may acquire a mass from a Stueckelberg-type scalar. The model, when all issues of theoretical consistency are taken into…

High Energy Physics - Phenomenology · Physics 2021-10-26 Radhika Vinze , Sreerup Raychaudhuri

A new mechanism for mass generation of gauge fields is proposed in this paper. By introducing two sets of gauge fields and making the variatons of these two sets of gauge fields compensate each other under local gauge transformations, the…

High Energy Physics - Phenomenology · Physics 2018-01-17 Ning Wu

In a wide class of $G_L\times G_R$ invariant two-dimensional super-renormalizable field theories, the parity-odd part of the two-point function of global currents is completely determined by a fermion one-loop diagram. For any non-trivial…

High Energy Physics - Theory · Physics 2008-11-26 Hidenori Fukaya , Masashi Hayakawa , Issaku Kanamori , Hiroshi Suzuki , Tomohisa Takimi

The description of the internal spaces of fermion and boson fields with "basis vectors", which are the superposition of odd and even products of the operators $\gamma^a$, offers in $d=2(2n+1)$-dimensions, such as $d=(13+1)$, a unified…

High Energy Physics - Theory · Physics 2026-05-05 N. S. Mankoč Borštnik

The Coulomb problem for vector bosons W(+/-) propagating in an attractive Coulomb field incorporates a known difficulty, i.e. the total charge of the boson localized on the Coulomb center turns out infinite. This fact contradicts the…

High Energy Physics - Theory · Physics 2009-08-18 M. Yu. Kuchiev , V. V. Flambaum

A realistic extension of the minimal $SU(5)$ theory consisting of the addition of an adjoint fermion is known to predict light real fermion and scalar weak triplets, potentially accessible at the LHC. These particles, in addition to playing…

High Energy Physics - Phenomenology · Physics 2023-01-11 Goran Senjanović , Michael Zantedeschi

The vector curvaton paradigm is reviewed. The mechanism allows a massive vector boson field to contribute to or even generate the curvature perturbation in the Universe. Contribution of vector bosons is likely to generate statistical…

High Energy Physics - Phenomenology · Physics 2012-04-11 Konstantinos Dimopoulos

The bosonic contributions to the photon mass are shown to be of the same form as the fermionic contributions, but of opposite sign. A mass sum rule for bosons and fermions follows from gauge invariance. Assuming completeness of the standard…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. J. Lodder

We consider a massive vector Boson in a static patch of $D$-dimensional de Sitter space (dS$_D$). We argue that this field is controlled by an effective physical (squared) mass $\mu_{\mathrm{v}}^2 = m_{\mathrm{v}}^2 +…

High Energy Physics - Theory · Physics 2024-12-20 Adel A. Rahman , Leonard Susskind

The conditions for the cancellation of one loop contributions to vacuum energy (both U.V. divergent and finite) coming from the Standard Model (SM) fields are examined. It is proven that this is not possible unless one introduces besides…

High Energy Physics - Theory · Physics 2008-05-03 G. L. Alberghi , A. Y. Kamenshchik , A. Tronconi , G. P. Vacca , G. Venturi
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