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Dark matter direct and indirect detection signals depend crucially on the dark matter distribution. While the formation of large scale structure is independent of the nature of the cold dark matter (CDM), the fate of inhomogeneities on…

Astrophysics · Physics 2011-05-05 Anne M. Green , Stefan Hofmann , Dominik J. Schwarz

The observed density of dark matter is of the magnitude expected for a thermal relic weakly-interacting massive particle (WIMP). In addition, the observed baryon density is within an order of magnitude of the dark matter density. This…

High Energy Physics - Phenomenology · Physics 2015-03-06 John McDonald

We obtain predictions for the properties of cold dark matter annihilation radiation using high resolution hydrodynamic zoom-in cosmological simulations of Milky Way-like galaxies (APOSTLE project) carried out as part of the "Evolution and…

We derive the effects of DM decays and annihilations on structure formation. We consider moderately massive DM particles (sterile neutrinos and light DM), as they are expected to give the maximum contribution to heating and reionization.…

Astrophysics · Physics 2008-11-26 E. Ripamonti , M. Mapelli , A. Ferrara

The dark matter distribution on small scales may depend on the the properties of the first generation of dark matter halos to form, which is in turn determined by the microphysics of the dark matter particles. We overview the microphysics…

Astrophysics · Physics 2009-11-13 Anne M. Green , Stefan Hofmann , Dominik J. Schwarz

We use six, high-resolution $\Lambda$CDM simulations of galaxy formation to study how emission from dark matter annihilation is affected by baryonic processes. These simulations produce isolated, disc-dominated galaxies with structure,…

Astrophysics of Galaxies · Physics 2021-01-06 Robert J J Grand , Simon D M White

The inability of standard non-interacting cold dark matter (CDM) to account for the small scale structure of individual galaxies has led to the suggestion that the dark matter may undergo elastic and/or inelastic scattering. We simulate the…

Astrophysics · Physics 2009-11-06 Matthew W. Craig , Marc Davis

We revisit the possibility of constraining the properties of dark matter (DM) by studying the epoch of cosmic reionization. Previous studies have shown that DM annihilation was unlikely to have provided a large fraction of the photons that…

Cosmology and Nongalactic Astrophysics · Physics 2016-12-21 Alexander A. Kaurov , Dan Hooper , Nickolay Y. Gnedin

High resolution cosmological N-body simulations of four galaxy-scale dark matter halos are compared to corresponding N-body/hydrodynamical simulations containing dark matter, stars and gas. The simulations without baryons share features…

Astrophysics · Physics 2007-05-23 Michael Gustafsson , Malcolm Fairbairn , Jesper Sommer-Larsen

Context: While stars have often been used as laboratories to study dark matter (DM), red giant branch (RGB) stars and all the rich phenomenology they encompass have frequently been overlooked by such endeavors. Aims: We study the capture,…

Solar and Stellar Astrophysics · Physics 2021-07-30 José Lopes , Ilídio Lopes

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

We include an energy term based on Dark Matter (DM) self-annihilation during the cooling and subsequent collapse of the metal-free gas, in halos hosting the formation of the first stars in the Universe. We have found that the feedback…

Cosmology and Nongalactic Astrophysics · Physics 2015-05-18 E. Ripamonti , F. Iocco , A. Ferrara , R. Schneider , A. Bressan , P. Marigo

WIMP-type dark matter may have additional interactions that break baryon number, leading to induced nucleon decays which are subject to direct experimental constraints from proton decay experiments. In this work, we analyze the possibility…

High Energy Physics - Phenomenology · Physics 2025-01-06 Yohei Ema , Robert McGehee , Maxim Pospelov , Anupam Ray

Weakly interacting massive particles are part of the lepton-photon plasma in the early universe until kinetic decoupling, after which time the particles behave like a collisionless gas with nonzero temperature. The Boltzmann equation for…

Astrophysics · Physics 2009-11-11 Edmund Bertschinger

We have proposed that the first phase of stellar evolution in the history of the Universe may be Dark Stars (DS), powered by dark matter heating rather than by nuclear fusion, and in this paper we examine the history of these DS. The power…

Cosmology and Nongalactic Astrophysics · Physics 2011-02-11 Douglas Spolyar , Peter Bodenheimer , Katherine Freese , Palo Gondolo

We use the NIHAO simulations to investigate the effects of baryonic physics on the time evolution of Dark Matter central density profiles. The sample is made of $\approx 70$ independent high resolution hydrodynamical simulations of galaxy…

The properties of a neutron star are studied in the presence of dark matter. We have considered a relatively light Weakly Interacting Massive Particle (WIMP) as a dark matter candidate with properties suggested by the results of the…

Nuclear Theory · Physics 2020-08-26 Abdul Quddus , Grigorios Panotopoulos , Bharat Kumar , Shakeb Ahmad , S. K. Patra

Primordial black holes (PBHs) can form spike density halos through the accretion of weakly interacting massive particles (WIMPs). In these halos, the enhanced density significantly boosts the annihilation rate of WIMPs. For Majorana dark…

Cosmology and Nongalactic Astrophysics · Physics 2026-01-05 Shibsankar Si , Pravin Kumar Natwariya , Alekha C. Nayak

Although dark matter makes up 80% of the gravitational mass of our Galaxy, its composition is not known. One hypothesis is that dark matter consists of massive particles called WIMPs. WIMPs are expected to accumulate and coannihilate in the…

Astrophysics · Physics 2007-11-16 Benjamin Monreal , Lorne A. Nelson , Joseph A. Formaggio

Simple models of weakly interacting massive particles (WIMPs) predict dark matter annihilations into pairs of electroweak gauge bosons, Higgses or tops, which through their subsequent cascade decays produce a spectrum of gamma rays.…

High Energy Physics - Phenomenology · Physics 2015-05-20 Prateek Agrawal , Brian Batell , Patrick J. Fox , Roni Harnik