English
Related papers

Related papers: Composite Dark Matter and LHC Interplay

200 papers

We construct a self-interacting scalar dark matter (DM) model with local discrete $Z_{3}$ symmetry that stabilizes a weak scale scalar dark matter $X$. The model assumes a hidden sector with a local $U(1)_X$ dark gauge symmetry, which is…

High Energy Physics - Phenomenology · Physics 2014-05-30 P. Ko , Yong Tang

We present `twin Higgs models', simple realizations of the Higgs as a pseudo-Goldstone boson that protect the weak scale from radiative corrections up to scales of order 5 - 10 TeV. In the ultra-violet these theories have a discrete…

High Energy Physics - Phenomenology · Physics 2015-02-10 Z. Chacko , Hock-Seng Goh , Roni Harnik

The thermal relic abundance of Dark Matter motivates the existence of new electroweak scale particles, independent of naturalness considerations. However, most unnatural Dark Matter models do not ensure the presence of new particles charged…

High Energy Physics - Phenomenology · Physics 2009-01-06 Aaron Pierce , Jesse Thaler

Little Higgs models - which can most easily be thought of as a variant of composite Higgs models - explain a light Higgs boson at 125 GeV as an pseudo-Nambu-Goldstone boson of a spontaneously broken global symmetry. The mechanism of…

High Energy Physics - Phenomenology · Physics 2018-11-07 Jürgen Reuter , Daniel Dercks , Gudrid Moortgat-Pick , So Young Shim

The LHC has been built to understand the dynamics at the origin of the breaking of the electroweak symmetry. Weakly coupled models with a fundamental Higgs boson have focused most of the attention of the experimental searches. We will…

High Energy Physics - Phenomenology · Physics 2015-06-04 J. R. Espinosa , C. Grojean , M. Muehlleitner

We consider a minimal model where the Higgs boson arises as an elementary pseudo-Nambu-Goldstone boson. The model is based on an extended scalar sector with global SO(5)/SO(4) symmetry. To achieve the correct electroweak symmetry breaking…

High Energy Physics - Phenomenology · Physics 2018-08-15 Helene Gertov , Sofie Gregersen , Francesco Sannino , Kimmo Tuominen

In all scalar extensions of the standard model of particle interactions, the one Higgs boson responsible for electroweak symmetry breaking always mixes with other neutral scalars at tree level unless a symmetry prevents it. An unexplored…

High Energy Physics - Phenomenology · Physics 2016-02-17 Ernest Ma

We study an economical model of weakly-interacting massive particle dark matter (DM) which has spin 3/2 and interacts with the 125-GeV Higgs boson via effective scalar and pseudoscalar operators. We apply constraints on the model from the…

High Energy Physics - Phenomenology · Physics 2017-12-01 Chia-Feng Chang , Xiao-Gang He , Jusak Tandean

One of the simplest extensions of the Standard Model (SM) consists in adding a scalar singlet. This second Higgs boson is able to solve several fundamental problems of SM. Additional scalar particles arise naturally in composite Higgs…

High Energy Physics - Phenomenology · Physics 2023-04-06 S. S. Afonin

We propose a framework for natural breaking of electroweak symmetry in supersymmetric models, where elementary Higgs fields are semi-perturbatively coupled to a strong superconformal sector. The Higgs VEVs break conformal symmetry in the…

High Energy Physics - Phenomenology · Physics 2015-06-05 Ryuichiro Kitano , Markus A. Luty , Yuichiro Nakai

Recent LHC searches have not found a clear signal of the Higgs boson h of the standard model (SM) with three or four families in the mass range m_h = 120-600 GeV. If the Higgs had an unexpectedly large invisible branching ratio, the…

High Energy Physics - Phenomenology · Physics 2011-10-28 Xiao-Gang He , Jusak Tandean

We propose UV complete (Partially) Composite Higgs models with compositeness scale up to the Planck scale assisted by a novel mechanism. This mechanism is based on softly breaking a global $ \mathbb{Z}_2 $ symmetry by technically natural…

High Energy Physics - Phenomenology · Physics 2022-07-28 Martin Rosenlyst

We examine the possibility that dark matter may be the manifestation of dark forces of a hidden sector, i.e. "Dark Force = Dark Matter." As an illustrative and minimal example we consider the hidden SU(2)_h x U(1)_h gauge group. The hidden…

High Energy Physics - Phenomenology · Physics 2014-04-02 Hooman Davoudiasl , Ian M. Lewis

We study a scenario in which the dilaton, a pseudo-Goldstone boson of the spontaneous breaking of conformal symmetry, provides a portal between dark matter and the visible sector. We consider the low-energy description of the theory in…

High Energy Physics - Phenomenology · Physics 2015-06-23 Aielet Efrati , Eric Kuflik , Shmuel Nussinov , Yotam Soreq , Tomer Volansky

In a previous paper \cite{Khlopov:2007ic}, we showed how the minimal walking technicolor model (WTC) can provide a composite dark matter candidate, by forming bound states between a -2 electrically charged techniparticle and a $^4He^{++}$.…

Astrophysics · Physics 2008-11-26 Maxim Yu. Khlopov , Chris Kouvaris

The mass spectra of the standard model particles are reproduced in the $SO(11)$ gauge-Higgs grand unification in the six-dimensional warped space without introducing exotic light fermions. Light neutrino masses are explained by the…

High Energy Physics - Phenomenology · Physics 2018-02-27 Yutaka Hosotani , Naoki Yamatsu

In the unified subquark model of all fundamental particles and forces, the mass of the Higgs boson in the standard model of electroweak interactions ($m_H$) is predicted to be about $2\sqrt{6}m_W/3$ (where $m_W$ is the mass of the charged…

High Energy Physics - Phenomenology · Physics 2015-06-18 Hidezumi Terazawa , Masaki Yasue

The requirements of electroweak symmetry breaking (EWSB) and correct thermal relic density of Dark Matter (DM) predict large spin-independent direct detection cross section in scalar DM models based on underlying SO(10) non-supersymmetric…

High Energy Physics - Phenomenology · Physics 2009-12-25 M. Kadastik , K. Kannike , A. Racioppi , M. Raidal

We investigate an electroweak interacting dark matter (DM) model in which the DM is the neutral component of the SU$(2)_L$ triplet fermion that couples to the standard model (SM) Higgs sector via an SM singlet Higgs boson. In this setup,…

High Energy Physics - Phenomenology · Physics 2015-09-16 Cheng-Wei Chiang , Eibun Senaha

In scenarios of strongly coupled electroweak symmetry breaking, heavy composite particles of different spin and parity may arise and cause observable effects on signals that appear at loop levels. The recently observed process of Higgs to…

High Energy Physics - Phenomenology · Physics 2015-10-27 A. E. Cárcamo Hernández , Claudio O. Dib , Alfonso R. Zerwekh