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We revisit the annihilation of dark matter to neutrinos in the Sun near the WW and tt kinematic thresholds. We investigate the potential importance of annihilation to WW* in a minimal dark matter model in which a Majorana singlet is mixed…

High Energy Physics - Phenomenology · Physics 2013-05-30 John Kearney , Aaron Pierce

Weakly Interacting Massive Particle (WIMP) direct detection experiments are closing in on the region of parameter space where relic neutralinos may constitute the galactic halo dark matter. We discuss two issues in the interpretation of…

High Energy Physics - Phenomenology · Physics 2007-05-23 Anne M. Green

We explore the gravitational wave probes of a two-component dark matter framework, consisting of an $SU(2)_L$ triplet scalar and a Standard Model singlet fermion. The triplet scalar dark matter typically remains underabundant in the region…

High Energy Physics - Phenomenology · Physics 2025-05-16 Pankaj Borah , Pradipta Ghosh , Abhijit Kumar Saha

Given the recent progress in dark matter direction detection experiments, we examine a light bino-higgsino dark matter (DM) scenario ($M_1<100$ GeV and $\mu<300$ GeV) in natural supersymmetry with the electroweak fine tuning measure…

High Energy Physics - Phenomenology · Physics 2018-01-17 Murat Abdughani , Lei Wu , Jin Min Yang

We perform a detailed and quasi model-independent analysis of direct annihilation of Dark Matter into neutrinos. Considering different cases for scalar and fermionic Dark Matter, we identify several settings in which this annihilation is…

High Energy Physics - Phenomenology · Physics 2011-01-20 Manfred Lindner , Alexander Merle , Viviana Niro

Direct detection experiments rule out fermion dark matter that is a chiral representation of the electroweak gauge group. Non-chiral real, complex and singlet representations, however, provide viable fermion dark matter candidates. Although…

High Energy Physics - Phenomenology · Physics 2009-09-17 Rouven Essig

The Milky Way halo is the brightest source of dark matter annihilation on the sky. Indeed, the potential strength of the Galactic dark matter signal can supersede that expected from dwarf galaxies and galaxy groups even in regions away from…

Cosmology and Nongalactic Astrophysics · Physics 2018-12-20 Laura J. Chang , Mariangela Lisanti , Siddharth Mishra-Sharma

Minimal Dark Matter is among the simplest and most predictive Dark Matter frameworks, with the Majorana SU(2) 5-plet as its smallest accidentally stable real representation. We present a comprehensive reassessment of its indirect-detection…

High Energy Physics - Phenomenology · Physics 2025-07-24 Mohammad Aghaie , Alessandro Dondarini , Giulio Marino , Paolo Panci

The era of precision cosmology has revealed that about 85% of the matter in the universe is dark matter. Two well-motivated candidates are weakly interacting massive particles (WIMPs) and weakly interacting sub-eV particles (WISPs) (e.g.…

High energy particles are produced by the annihilation of dark matter particles in our galaxy. These are presently searched for using balloon-borne antiproton and positron detectors and large area, deep underground neutrino telescopes. Dark…

High Energy Physics - Phenomenology · Physics 2016-09-01 F. Halzen , J. E Jacobsen

The thermal relic density of the wino-like neutralino dark matter in the brane world cosmology is studied. The expansion law at a high energy regime in the brane world cosmology is modified from the one in the standard cosmology, and the…

High Energy Physics - Phenomenology · Physics 2009-11-11 Takeshi Nihei , Nobuchika Okada , Osamu Seto

Here we examine the detectability of collisionless dark matter candidates that may constitute not all but only a subdominant component of galactic cold dark matter. We show that current axion searches are not suited for a subdominant…

High Energy Physics - Phenomenology · Physics 2009-11-07 Gintaras Duda , Graciela Gelmini , Paolo Gondolo

We examine the detectability through indirect means of weakly interacting dark matter candidates that may constitute not all but only a subdominant component of galactic cold dark matter. We show that the possibility of indirect detection…

High Energy Physics - Phenomenology · Physics 2009-11-07 Gintaras Duda , Graciela Gelmini , Paolo Gondolo , Joakim Edsjo , Joseph Silk

In natural SUSY models higgsinos are always light because \mu^2 cannot be much larger than M_Z^2, while squarks and gluinos may be very heavy. Unless gluinos are discovered at LHC13, the commonly assumed unification of gaugino mass…

High Energy Physics - Phenomenology · Physics 2017-01-17 Howard Baer , Vernon Barger , Peisi Huang , Dan Mickelson , Maren Padeffke-Kirkland , Xerxes Tata

The H.E.S.S. experiment is an array of four identical imaging atmospheric Cherenkov telescopes in the Southern hemisphere, designed to observe very high energy gamma-rays (E > 100 GeV). These high energy gamma-rays can be used to search for…

High Energy Astrophysical Phenomena · Physics 2011-11-28 A. Viana

There is strong evidence about the existence of unknown dark matter in the Universe. Many different theories about this dark matter exist, but most probably it is made of a new kind of fundamental particle that has to be massive, stable,…

High Energy Astrophysical Phenomena · Physics 2019-09-04 Dorit Glawion , Denys Malyshev , Emmanuel Moulin , Louise Oakes , Lucia Rinchiuso , Aion Viana

The minimal seesaw extension of the Standard Model requires two electroweak singlet fermions in order to accommodate the neutrino oscillation parameters at tree level. Here we consider a next to minimal extension where light neutrino masses…

High Energy Physics - Phenomenology · Physics 2016-06-15 Roberto A. Lineros

We explore the whole parameter space of the singlet fermionic cold dark matter model with respect to constraints on, first, the relic density and second, gamma-ray lines up to 10 TeV. We investigate 44000 random sample models which…

High Energy Physics - Phenomenology · Physics 2020-08-25 Reza Moazzemi

We observe that in SUSY models with non-universal GUT scale gaugino mass parameters, raising the GUT scale SU(2) gaugino mass |M_2| from its unified value results in a smaller value of -m_{H_u}^2 at the weak scale. By the electroweak…

High Energy Physics - Phenomenology · Physics 2008-11-26 Howard Baer , Azar Mustafayev , Heaya Summy , Xerxes Tata

Almost degenerate bino and wino masses at the weak scale is one of unique features of gauge messenger models. The lightest neutralino is a mixture of bino, wino and higgsino and can produce the correct amount of the dark matter density if…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kyu Jung Bae , Radovan Dermisek , Hyung Do Kim , Ian-Woo Kim