scholarly journals Vector Gauge Boson Dark Matter for the SU(N) Gauge Group Model

2013 ◽  
Vol 52 (12) ◽  
pp. 4374-4388 ◽  
Author(s):  
E. Koorambas
Keyword(s):  
Dark Matter ◽  
Gauge Group ◽  
Gauge Boson ◽  
Group Model ◽  
Vector Gauge

scholarly journals Vector dark matter from split SU(2) gauge bosons

2021 ◽  
Vol 2021 (7) ◽  
Author(s):  
Zexi Hu ◽  
Chengfeng Cai ◽  
Yi-Lei Tang ◽  
Zhao-Huan Yu ◽  
Hong-Hao Zhang
Keyword(s):  
Dark Matter ◽  
Gauge Group ◽  
Measurement Data ◽  
Indirect Detection ◽  
Gauge Bosons ◽  
Dark Matter Relic Density ◽  
Matter Model ◽  
Direct And Indirect Detection ◽  
Numerous Parameter ◽  
Dark Matter Model

Abstract We propose a vector dark matter model with an exotic dark SU(2) gauge group. Two Higgs triplets are introduced to spontaneously break the symmetry. All of the dark gauge bosons become massive, and the lightest one is a viable vector DM candidate. Its stability is guaranteed by a remaining Z2 symmetry. We study the parameter space constrained by the Higgs measurement data, the dark matter relic density, and direct and indirect detection experiments. We find numerous parameter points satisfying all the constraints, and they could be further tested in future experiments. Similar methodology can be used to construct vector dark matter models from an arbitrary SO(N) gauge group.

scholarly journals Feebly interacting U(1)B−L gauge boson warm dark matter and XENON1T anomaly

2020 ◽  
Vol 810 ◽  
pp. 135836 ◽  
Author(s):  
Gongjun Choi ◽  
Tsutomu T. Yanagida ◽  
Norimi Yokozaki
Keyword(s):  
Dark Matter ◽  
Gauge Boson

scholarly journals ELECTROWEAK UNIFICATION OF QUARKS AND LEPTONS IN A GAUGE GROUP SUC(3) × SU(4) × UX(1)

2012 ◽  
Vol 27 (21) ◽  
pp. 1250117 ◽  
Author(s):  
FAYYAZUDDIN
Keyword(s):  
Dark Matter ◽  
Standard Model ◽  
Gauge Group ◽  
Lower Limit ◽  
Z Boson ◽  
Early Stage ◽  
Mass Scale ◽  
The Standard Model ◽  
Vector Bosons ◽  
The Universe

A model for electroweak unification of quarks and leptons, in a gauge group SUC(3) × SU(4) × UX(1) is constructed. The model requires, three generations of quarks and leptons which are replicas (mirror) of the standard quarks and leptons. The gauge group SU(4) × UX(1) is broken in such a way so as to reproduce standard model and to generate heavy masses for the vector bosons [Formula: see text], the leptoquarks and mirror fermions. It is shown lower limit on mass scale of mirror fermions is [Formula: see text], E- being the lightest mirror fermion coupled to Z boson. As the universe expands, the heavy matter is decoupled at an early stage of expansion and may be a source of dark matter. Leptoquarks in the model connect the standard model and mirror fermions. Baryon genesis in our universe implies antibaryon genesis in mirror universe.

scholarly journals SYSTEMATIC STUDY OF THESU(3)c⊗SU(4)L⊗U(1)XGAUGE SYMMETRY

2007 ◽  
Vol 22 (06) ◽  
pp. 435-447 ◽  
Author(s):  
WILLIAM A. PONCE ◽  
LUIS A. SÁNCHEZ
Keyword(s):  
Standard Model ◽  
Gauge Group ◽  
Gauge Boson ◽  
Systematic Study ◽  
Infinite Number ◽  
Model Based ◽  
First Case ◽  
The Standard Model ◽  
Family Models

We carry out a systematic study of possible extensions of the standard model based on the gauge group SU (3)c⊗ SU (4)L⊗ U (1)X. We consider models with particles having exotic electric charges and also models which do not contain exotic electric charges in the gauge boson sector or in the fermion sector. For the first case an infinite number of models can, in principle, be constructed, while the restriction to non-exotic electric charges only allows for eight different anomaly-free models. Four of them are three-family models in the sense that anomalies cancel by an interplay between the three families, and another two are one-family models where anomalies cancel family by family as in the standard model. The remaining two are two-family models.

EXTENDING THE STUECKELBERG MODEL FOR SPACETIME SYMMETRIES: COSMOLOGICAL IMPLICATIONS

2006 ◽  
Vol 21 (37) ◽  
pp. 2813-2825 ◽  
Author(s):  
V. ALDAYA ◽  
M. CALIXTO ◽  
E. SÁNCHEZ-SASTRE
Keyword(s):  
Dark Matter ◽  
Weyl Group ◽  
Lie Groups ◽  
Gauge Group ◽  
Gravitational Theory ◽  
Natural Source ◽  
Spacetime Symmetries ◽  
Minimal Coupling ◽  
Group Parameter ◽  
Scale Transformations

The so-called Stueckelberg transformation is introduced as a prescription of minimal coupling following the procedure of the Utiyama theory, for both internal and spacetime symmetry Lie groups. As a natural example, the theory is applied to the Weyl group and the corresponding gauge gravitational theory is developed. This context appears to be a natural source to account for some sort of dark matter intrinsically related to the gauge-group parameter associated with scale transformations.

scholarly journals Search for a vector gauge boson in ϕ meson decays with the KLOE detector

2012 ◽  
Vol 706 (4-5) ◽  
pp. 251-255 ◽  
Author(s):  
F. Archilli ◽  
D. Babusci ◽  
D. Badoni ◽  
I. Balwierz ◽  
G. Bencivenni ◽  
...  
Keyword(s):  
Gauge Boson ◽  
Meson Decays ◽  
Vector Gauge

scholarly journals COMPOSITE WEAK BOSONS AND DARK MATTER

2013 ◽  
Vol 28 (23) ◽  
pp. 1350106
Author(s):  
HARALD FRITZSCH
Keyword(s):  
Dark Matter ◽  
Gauge Group ◽  
Bound States ◽  
The Universe

The weak bosons are bound states of two fermions and their antiparticles, denoted as haplons. The confinement scale of the associated gauge group SU(2) is of the order of 0.3 TeV. Besides the weak bosons, there also exist new bosons, an SU(2)-triplet and a singlet, with a mass of the order of 0.5 TeV. The neutral singlet boson is stable and provides the dark matter in the universe.

scholarly journals Leptogenesis from a U(1)D resonance

2020 ◽  
Vol 2020 (8) ◽  
Author(s):  
Eung Jin Chun ◽  
Arnab Dasgupta ◽  
Sin Kyu Kang
Keyword(s):  
Dark Matter ◽  
Cp Violation ◽  
Imaginary Part ◽  
Gauge Boson ◽  
Lepton Number ◽  
Tree Level ◽  
Effective Coupling ◽  
Energy Correction ◽  
Self Energy

Abstract We propose a novel mechanism to realize leptogenesis through the Breit- Wigner resonance of a dark U(1)D gauge boson ZD , which mediates lepton number vi- olating annihilations of dark matter (DM) in the context of the scotogenic model with a U(1)D . The processes occur out of equilibrium and DM freezes out later giving rise to the observed abundance. The CP violation required for leptogenesis can be achieved by the interference between tree-level t-channel scattering of DM and the subsequent 1-loop mediated by ZD , which arises due to the unremovable imaginary part of either the ZD propagator coming from its self-energy correction or the 1-loop giving rise to the effective coupling of $$ {Z}_D\overline{\nu}\nu $$ Z D ν ¯ ν .

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