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The Randall-Sundrum model with gauge fields and fermions in the bulk has several attractive features including the gauge coupling unification, a candidate for the dark matter, and an explanation for the hierarchical Yukawa couplings. In…

High Energy Physics - Phenomenology · Physics 2007-05-25 Hiroto Nakajima

Dark matter could emerge along with the Higgs as a composite pseudo-Nambu-Goldstone boson $\chi$ with decay constant $f\sim \mathrm{TeV}$. This type of WIMP is especially compelling because its leading interaction with the Standard Model,…

High Energy Physics - Phenomenology · Physics 2018-12-20 Reuven Balkin , Maximilian Ruhdorfer , Ennio Salvioni , Andreas Weiler

Dark matter particles interacting via the exchange of very light spin-0 mediators can have large self-interaction rates and obtain their relic abundance from thermal freeze-out. At the same time, these models face strong bounds from direct…

High Energy Physics - Phenomenology · Physics 2017-12-25 Felix Kahlhoefer , Kai Schmidt-Hoberg , Sebastian Wild

Subterrestrial neutron spectra show weak but consistent anomalies at multiplicities ~100 and above [1-3]. The data of the available measurements are of low statistical significance [4] but indicate an excess of events not correlated with…

High Energy Physics - Phenomenology · Physics 2023-12-05 Thomas Ward , Wladyslaw H. Trzaska

Coupling dark matter to light new particles is an attractive way to combine thermal production with strong velocity-dependent self-interactions. Here we point out that in such models the dark matter annihilation rate is generically enhanced…

High Energy Physics - Phenomenology · Physics 2017-04-12 Torsten Bringmann , Felix Kahlhoefer , Kai Schmidt-Hoberg , Parampreet Walia

In this article, we propose different background models of extended theories of gravity, which are minimally coupled to the SM fields, to explain the possibility of genesis of dark matter without affecting the SM particle sector. We modify…

High Energy Physics - Phenomenology · Physics 2016-09-14 Sayantan Choudhury , Manibrata Sen , Soumya Sadhukhan

There exists a general model framework where dark matter can be a vanilla WIMP-like thermal relic with a mass of ${\cal O}$(100 GeV), but it still escapes direct detection. This happens, if the dark matter particle is a Goldstone boson…

High Energy Physics - Phenomenology · Physics 2019-05-01 Tommi Alanne , Matti Heikinheimo , Venus Keus , Niko Koivunen , Kimmo Tuominen

We conduct a comprehensive analysis of potential annihilation processes of light dark matter (DM) in minimal Higgs portal models near supermassive black hole (Sgr A$^{\star}$) in the Galactic Center, considering interactions between DM…

High Energy Physics - Phenomenology · Physics 2025-01-14 Chih-Ting Lu , Xiao-Yi Luo , Zi-Qing Xia

If dark matter self-annihilates then it may produce an observable signal when its density is high. The details depend on the intrinsic properties of dark matter and how it clusters in space. For example, the density profile of some dark…

High Energy Astrophysical Phenomena · Physics 2015-06-03 Benjamin C. Bromley

We explore the possible signatures of dark matter (DM) pair annihilations in the nearby dwarf spheroidal galaxy Draco. After investigating the mass models for Draco in the light of available observational data, we carefully model the DM…

Astrophysics · Physics 2008-11-26 S. Colafrancesco , S. Profumo , P. Ullio

Semi-annihilation is a generic feature of dark matter theories stabilised by symmetries larger than a $Z_2$. It contributes to thermal freeze out, but is irrelevant for direct and collider searches. This allows semi-annihilating dark matter…

High Energy Physics - Phenomenology · Physics 2017-03-08 Yi Cai , Andrew Spray

We construct a model based on an extra gauge symmetry, SU(2)_X x U(1)_{B-L}, which can provide gauge bosons to serve as weakly-interacting massive particle dark matter. The stability of the dark matter is naturally guaranteed by a discrete…

High Energy Physics - Phenomenology · Physics 2014-03-07 Cheng-Wei Chiang , Takaaki Nomura , Jusak Tandean

We explore the possibility that the high energy neutrino flux observed by terrestrial telescopes originates from dark matter (DM) annihilation. Specifically, we study a minimal, UV-complete $U(1)$ extension of the Standard Model with a…

High Energy Physics - Phenomenology · Physics 2025-09-10 Arindam Basu , Basabendu Barman , Arindam Das

Extensive searches to probe the particle nature of dark matter (DM) have been going on for some decades now but, so far, no conclusive evidence has been found. Among various options, the Weakly Interacting Massive Particles (WIMP) remains…

High Energy Physics - Phenomenology · Physics 2021-03-01 Debottam Das , Bibhabasu De , Subhadip Mitra

A strongly self-interacting component of asymmetric dark matter can collapse and form compact objects, provided there is an efficient mechanism of energy evacuation. If the dark matter quantum number is not completely conserved but it is…

High Energy Physics - Phenomenology · Physics 2025-03-11 Chris Kouvaris , Dimitris Zavitsanos

We present a search for an excess of neutrino interactions due to dark matter in the form of Weakly Interacting Massive Particles (WIMPs) annihilating in the galactic center or halo based on the data set of Super-Kamiokande-I, -II, -III and…

High Energy Physics - Experiment · Physics 2020-10-14 Kamiokande Collaboration , K. Abe , C. Bronner , Y. Haga , Y. Hayato , M. Ikeda , S. Imaizumi , H. Ito , K. Iyogi , J. Kameda , Y. Kataoka , Y. Kato , Y. Kishimoto , Ll. Marti , M. Miura , S. Moriyama , T. Mochizuki , Y. Nagao , M. Nakahata , Y. Nakajima , T. Nakajima , S. Nakayama , T. Okada , K. Okamoto , A. Orii , G. Pronost , H. Sekiya , M. Shiozawa , Y. Sonoda , A. Takeda , A. Takenaka , H. Tanaka , S. Tasaka , T. Tomura , K. Ueno , T. Yano , T. Yokozawa , R. Akutsu , S. Han , T. Irvine , T. Kajita , I. Kametani , K. P. Lee , T. McLachlan , K. Okumura , E. Richard , T. Tashiro , R. Wang , J. Xia , D. Bravo-Berguño , L. Labarga , P. Fernandez , F. d. M. Blaszczyk , J. Gustafson , C. Kachulis , E. Kearns , J. L. Raaf , J. L. Stone , L. R. Sulak , S. Sussman , L. Wan , T. Wester , S. Berkman , S. Tobayama , J. Bian , G. Carminati , M. Elnimr , N. J. Griskevich , W. R. Kropp , S. Locke , S. Mine , A. Renshaw , M. B. Smy , H. W. Sobel , V. Takhistov , P. Weatherly , B. L. Hartfiel , J. Hill , W. E. Keig , N. Hong , J. Y. Kim , I. T. Lim , R. G. Park , T. Akiri , B. Bodur , A. Himmel , Z. Li , E. O'Sullivan , K. Scholberg , C. W. Walter , T. Wongjirad , A. Coffani , O. Drapier , S. El Hedri , A. Giampaolo , M. Gonin , J. Imber , Th. A. Mueller , P. Paganini , B. Quilain , T. Ishizuka , T. Nakamura , J. S. Jang , K. Choi , J. G. Learned , S. Matsuno , S. N. Smith , J. Amey , L. H. V. Anthony , R. P. Litchfield , W. Y. Ma , A. A. Sztuc , Y. Uchida , M. O. Wascko , V. Berardi , M. G. Catanesi , R. A. Intonti , E. Radicioni , N. F. Calabria , L. N. Machado , G. De Rosa , G. Collazuol , F. Iacob , M. Lamoureux , N. Ospina , L. Ludovici , T. Boschi , F. Di Lodovico , S. Molina Sedgwick , S. Zsoldos , Y. Nishimura , S. Cao , M. Friend , T. Hasegawa , T. Ishida , T. Ishii , T. Kobayashi , T. Nakadaira , K. Nakamura , Y. Oyama , K. Sakashita , T. Sekiguchi , T. Tsukamoto , KE. Abe , M. Hasegawa , Y. Isobe , H. Miyabe , Y. Nakano , T. Shiozawa , T. Sugimoto , A. T. Suzuki , Y. Takeuchi , S. Yamamoto , A. Ali , Y. Ashida , T. Hayashino , T. Hiraki , S. Hirota , K. Huang , K. Ieki , M. Jiang , T. Kikawa , M. Mori , A. Murakami , KE. Nakamura , T. Nakaya , N. D. Patel , K. Suzuki , S. Takahashi , K. Tateishi , R. A. Wendell , N. McCauley , P. Mehta , A. Pritchard , K. M. Tsui , Y. Fukuda , Y. Itow , H. Menjo , G. Mitsuka , M. Murase , F. Muto , T. Niwa , K. Sato , T. Suzuki , M. Taani , z M. Tsukada , P. Mijakowski , K. Frankiewicz , J. Hignight , C. K. Jung , X. Li , J. L. Palomino , G. Santucci , C. Vilela , M. J. Wilking , C. Yanagisawa , D. Fukuda , K. Hagiwara , M. Harada , T. Horai , H. Ishino , S. Ito , T. Kayano , A. Kibayashi , Y. Koshio , W. Ma , T. Mori , H. Nagata , N. Piplani , M. Sakuda , S. Seiya , Y. Takahira , C. Xu , R. Yamaguchi , Y. Kuno , G. Barr , D. Barrow , L. Cook , C. Simpson , D. Wark , F. Nova , R. Tacik , J. Y. Yang , A. Cole , S. J. Jenkins , J. McElwee , M. Thiesse , L. Thompson , H. Okazawa , S. B. Kim , Y. Choi , K. Ito , K. Nishijima , K. Iwamoto , M. Koshiba , Y. Suda , M. Yokoyama , R. G. Calland , A. Goldsack , K. Martens , M. Murdoch , Y. Suzuki , M. R. Vagins , D. Hamabe , M. Kuze , Y. Okajima , M. Tanaka , T. Yoshida , M. Inomoto , M. Ishitsuka , R. Matsumoto , K. Ohta , M. Shinoki , J. F. Martin , C. M. Nantais , H. A. Tanaka , T. Towstego , M. Hartz , A. Konaka , P. de Perio , N. W. Prouse , S. Chen , B. D. Xu , Y. Zhang , B. Richards , K. Connolly , R. J. Wilkes , B. Jamieson , J. Walker , P. Giorgio , A. Minamino , K. Okamoto , G. Pintaudi

Primary features of a new cosmological model, which is based on conjectures about an existence of the graviton background and superstrong gravitational quantum interaction, are considered. An expansion of the universe is impossible in such…

General Relativity and Quantum Cosmology · Physics 2007-05-23 Michael A. Ivanov

We discuss the possibility to observe the products of dark matter annihilation that was going on in the early Universe. Of all the particles that could be generated by this process we consider only photons, as they are both uncharged and…

Astrophysics · Physics 2009-10-08 Anton N. Baushev

A general prediction of the 5-d Randall-Sundrum (RS) hierarchy model is the emergence of spin-2 Kaluza Klein (KK) gravitons with weak scale masses and couplings. The lowest order effective theory of the RS model is given by 5-d Einstein…

High Energy Physics - Phenomenology · Physics 2009-11-07 Hooman Davoudiasl , Thomas G. Rizzo

We study the global dynamics of the universe within the framework of the Interacting Dark Matter (IDM) scenario. Assuming that the dark matter obeys the collisional Boltzmann equation, we can derive analytical solutions of the global…

Astrophysics · Physics 2015-05-13 S. Basilakos , M. Plionis