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相关论文: The E6 route to multicomponent dark matter

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The dark matter may consist not of one elementary particle but of different species, each of them contributing a fraction of the observed dark matter density. A major theoretical difficulty with this scenario --dubbed multi-component dark…

高能物理 - 唯象学 · 物理学 2020-03-30 Carlos E. Yaguna , Óscar Zapata

We study the effect of all matter multiplets contained in {\bf 27} representation of $E_6$ GUT on gauge coupling unification in extra dimensions. Extra members of {\bf 27} multiplets of all three generations have their `zero modes' near…

高能物理 - 唯象学 · 物理学 2007-05-23 Biswajoy Brahmachari

Can dark matter be stabilized by charge conservation, just as the electron is in the standard model? We examine the possibility that dark matter is hidden, that is, neutral under all standard model gauge interactions, but charged under an…

高能物理 - 唯象学 · 物理学 2014-11-18 Jonathan L. Feng , Manoj Kaplinghat , Huitzu Tu , Hai-Bo Yu

In supersymmetric unified theories the dark matter particle can decay, just like the proton, through grand unified interactions with a lifetime of order of 10^{26} sec. Its decay products can be detected by several experiments -- including…

高能物理 - 唯象学 · 物理学 2009-09-24 Asimina Arvanitaki , Savas Dimopoulos , Sergei Dubovsky , Peter W. Graham , Roni Harnik , Surjeet Rajendran

An $SU(2)_N$ extension ($N$ stands for neutral) of the Standard Model (SM) is proposed with an additional $U(1)=S^{'}$ global symmetry, which stabilizes the lightest of the vector boson ($X,\bar{X}$) as dark matter (DM) through unbroken…

高能物理 - 唯象学 · 物理学 2018-09-26 Basabendu Barman , Subhaditya Bhattacharya , Mohammadreza Zakeri

A multi-component weakly-interacting dark matter scenario is analyzed, where the candidate dark matter states arise from the $SU(2)_{D}\to Z_{3}^{D}\times Z_{2}^{\text{acc}}$ symmetry breaking triggered by a VEV-developing scalar in the…

高能物理 - 唯象学 · 物理学 2025-05-16 Carlos Alvarado , Alfredo Aranda , Cesar Bonilla , Carlos Ramos Portalatino

We consider a scenario where a supersymmetric model has multiple dark matter particles. Adding a U(1)' gauge symmetry is a well-motivated extension of the Minimal Supersymmetric Standard Model (MSSM). It can cure the problems of the MSSM…

高能物理 - 唯象学 · 物理学 2008-11-26 Taeil Hur , Hye-Sung Lee , Salah Nasri

D3-brane probes of E-type Yukawa points lead to strongly coupled nearly conformal sectors nearby the Standard Model (visible sector) which are motivated by F-theory GUTs. Realistic visible sector brane configurations induce a seesaw mass…

高能物理 - 理论 · 物理学 2015-03-19 Jonathan J. Heckman , Soo-Jong Rey

We propose an extension of the Standard Model gauge symmetry by the gauge group $U(1)_{T3R}$ in order to address the Yukawa coupling hierarchy between the third generation fermions and the first two generation fermions of the SM. We assume…

高能物理 - 唯象学 · 物理学 2019-10-30 Bhaskar Dutta , Sumit Ghosh , Jason Kumar

Recent analysis of spontaneous breaking of SU(2) as a continuous gauged flavor symmetry to non-abelian discrete group Q4 as a residual symmetry motivates its consideration as a group for stabilizing dark matter. We determine the region of…

高能物理 - 唯象学 · 物理学 2012-12-06 I. Lovrekovic

A simple model of dark matter contains a light Dirac field charged under a hidden U(1) gauge symmetry. When a chiral matter content in a strong dynamics satisfies the t'Hooft anomaly matching condition, a massless baryon is a natural…

高能物理 - 唯象学 · 物理学 2019-09-04 Ayuki Kamada , Masaki Yamada , Tsutomu T. Yanagida

The asymmetric dark matter (ADM) paradigm is motivated by the apparent coincidence between the cosmological mass densities of visible and dark matter, $\Omega_\mathrm{DM} \simeq 5\Omega_\mathrm{VM}$. However, most ADM models only relate the…

高能物理 - 唯象学 · 物理学 2023-02-15 Alexander C. Ritter , Raymond R. Volkas

I present several scenarios developed in Zagreb, in which TeV-scale particles belonging to non-trivial weak-isospin multiplets give rise to neutrino-mass mechanisms different from conventional type I, II and III seesaw models. Two dim 9…

高能物理 - 唯象学 · 物理学 2019-03-29 Ivica Picek

Hidden sectors in connection with GeV-scale dark forces and dark matter are not only a common feature of physics beyond the Standard Model such as string theory and SUSY but are also phenomenologically of great interest regarding recent…

高能物理 - 唯象学 · 物理学 2012-11-22 Sarah Andreas

SU(N) Lie algebras possess discrete symmetries which can lead naturally to stable vector dark matter (DM). In this work, we consider the possibility that the dark SU(N) sector couples to the visible sector through the Higgs portal. We find…

高能物理 - 唯象学 · 物理学 2015-08-18 Christian Gross , Oleg Lebedev , Yann Mambrini

The idea of quark-lepton universality at high energies has been introduced as a natural extension to the standard model. This is achieved by endowing leptons with new degrees of freedom -- leptonic colour, an analogue of the familiar quark…

高能物理 - 唯象学 · 物理学 2014-11-18 Alison Demaria , Catherine I. Low , Raymond R. Volkas

Since the current evidence of its existence is revealed only through its gravitational influence, the way dark matter couples to gravity must be then of primary importance. Here, unlike the standard model sector which is typically coupled…

高能物理 - 唯象学 · 物理学 2020-10-21 Hemza Azri , Adil Jueid , Canan Karahan , Salah Nasri

Gauge Higgs Unification in Warped Extra Dimensions provides an attractive solution to the hierarchy problem. The extension of the Standard Model gauge symmetry to $SO(5)xU(1)_X$ allows the incorporation of the custodial symmetry $SU(2)_R$…

高能物理 - 唯象学 · 物理学 2010-12-09 Marcela Carena , Anibal D. Medina , Nausheen R. Shah , Carlos E. M. Wagner

The vector boson dark matter particles which stem from some broken gauge symmetries usually requires some unbroken symmetries to keep themselves stable. In the previous literature, some simplest cases have been discussed, in which the…

高能物理 - 唯象学 · 物理学 2025-02-13 Chun-Xue Yuan , Zhao Zhang , Chengfeng Cai , Yi-Lei Tang , Hong-Hao Zhang

Two theoretically well-motivated gauge extensions of the standard model are $SU(3)_C \times SU(3)_L \times SU(3)_R$ and $SU(3)_q \times SU(3)_L \times SU(3)_l \times SU(3)_R$, where $SU(3)_q$ is the same as $SU(3)_C$ and $SU(3)_l$ is its…

高能物理 - 唯象学 · 物理学 2018-01-17 Corey Kownacki , Ernest Ma , Nicholas Pollard , Oleg Popov , Mohammadreza Zakeri