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Related papers: TeV-Scale Thermal WIMPs: Unitarity and its Consequ…

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Dark matter dominates the matter content of the Universe, and its properties can be constrained through large-scale structure probes such as the cross-correlation between the unresolved gamma-ray background (UGRB) and weak gravitational…

We consider constraints on primordial black holes (PBHs) in the mass range $( 10^{-18}\text{-}10^{15} )\,M_{\odot}$ if the dark matter (DM) comprises weakly interacting massive particles (WIMPs) which form halos around them and generate…

Cosmology and Nongalactic Astrophysics · Physics 2021-07-29 Bernard Carr , Florian Kuhnel , Luca Visinelli

In this work we combine information from relic abundance, direct detection, cosmic microwave background, positron fraction, gamma rays, and colliders to explore the existing constraints on couplings between Dark Matter and Standard Model…

High Energy Physics - Phenomenology · Physics 2016-04-20 Mattias Blennow , Pilar Coloma , Enrique Fernandez-Martinez , Pedro A. N. Machado , Bryan Zaldivar

Over the past few decades, an anomalous 511 keV gamma-ray line has been observed from the centre of the Milky Way. Dark matter (DM) in the form of light weakly interacting massive particles (WIMPs) annihilating into electron-positron pairs…

Cosmology and Nongalactic Astrophysics · Physics 2016-12-01 Ryan J. Wilkinson , Aaron C. Vincent , Celine Boehm , Christopher McCabe

We consider dark matter annihilation into Standard Model particles and show that the least detectable final states, namely neutrinos, define an upper bound on the total cross section. Calculating the cosmic diffuse neutrino signal, and…

Astrophysics · Physics 2008-11-26 John F. Beacom , Nicole F. Bell , Gregory D. Mack

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

In the cosmological paradigm, cold dark matter dominates the mass content of the Universe and is present at every scale. Candidates for dark mater include many extensions of the standard model, with a Weakly Interacting Massive Particle…

High Energy Astrophysical Phenomena · Physics 2019-08-13 Matthieu Vivier

Dwarf spheroidal galaxies are known to be excellent targets for the detection of annihilating dark matter. We present new limits on the annihilation cross section of Weakly Interacting Massive Particles (WIMPs) based on the joint analysis…

Cosmology and Nongalactic Astrophysics · Physics 2012-03-20 Alex Geringer-Sameth , Savvas M. Koushiappas

We explore models in which weakly interacting massive particle (WIMP) dark matter annihilation is directly responsible for baryogenesis, thereby connecting dark matter with baryogenesis. We call this process "WIMPy baryogenesis". The dark…

High Energy Physics - Phenomenology · Physics 2015-06-03 Yanou Cui , Lisa Randall , Brian Shuve

We propose that dark matter is composed of particles that naturally have the correct thermal relic density, but have neither weak-scale masses nor weak interactions. These WIMPless models emerge naturally from gauge-mediated supersymmetry…

High Energy Physics - Phenomenology · Physics 2009-01-10 Jonathan L. Feng , Jason Kumar

There are many reasons to believe the present mass density of the universe is dominated by a weakly interacting massive particle (WIMP), a fossil relic of the early universe. Theoretical ideas and experimental efforts have focused mostly on…

High Energy Physics - Phenomenology · Physics 2007-05-23 Edward W. Kolb , Daniel J. H. Chung , Antonio Riotto

The AMS experiment onboard the International Space Station has recently provided cosmic ray electron and positron data with unprecedented precision in the range from 0.5 to 350 GeV. The observed rise in the positron fraction at energies…

High Energy Astrophysical Phenomena · Physics 2013-10-29 Lars Bergstrom , Torsten Bringmann , Ilias Cholis , Dan Hooper , Christoph Weniger

Particles with TeV mass and strong self-interactions generically have the right annihilation cross section to explain an observed excess of cosmic electrons and positrons if the end-product of the annihilation is charged leptons. We present…

High Energy Physics - Phenomenology · Physics 2010-08-12 Yi Cai , David E. Kaplan , Markus A. Luty

We impose new severe constraints on the self-interactions of fermionic asymmetric dark matter based on observations of nearby old neutron stars. WIMP self-interactions mediated by Yukawa- type interactions can lower significantly the number…

Cosmology and Nongalactic Astrophysics · Physics 2015-06-03 Chris Kouvaris

The $\Lambda$CDM cosmological framework predicts the existence of thousands of subhalos in our own Galaxy not massive enough to retain baryons and become visible. Yet, some of them may shine in gamma rays provided that the dark matter (DM)…

High Energy Astrophysical Phenomena · Physics 2020-04-20 Javier Coronado-Blazquez , Miguel A. Sanchez-Conde

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…

High Energy Physics - Phenomenology · Physics 2009-09-24 Asimina Arvanitaki , Savas Dimopoulos , Sergei Dubovsky , Peter W. Graham , Roni Harnik , Surjeet Rajendran

This work analyzes the detection prospects for weakly interacting massive particles (WIMPs) in dark matter (DM) density spikes around nearby supermassive black holes (SMBHs) by observations in very high energy gamma-ray band. Such spikes…

High Energy Astrophysical Phenomena · Physics 2025-12-12 Andrei E. Egorov

An energy threshold of (220$\pm$10) eV was achieved at an efficiency of 50% with a four-channel ultra-low-energy germanium detector each with an active mass of 5 g\cite{wimppaper}. This provides a unique probe to WIMP dark matter with mass…

Astrophysics · Physics 2019-08-13 Shin-Ted Lin , H. T. Wong

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

Dark matter that was once in thermal equilibrium with the Standard Model is generally prohibited from obtaining all of its mass from the electroweak phase transition. This implies a new scale of physics and mediator particles to facilitate…

High Energy Physics - Phenomenology · Physics 2014-12-19 Sonia El Hedri , William Shepherd , Devin G. E. Walker
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