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Related papers: Dark Matter Detectors as Dark Photon Helioscopes

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We describe a method for dark matter detection based on the evaporation of helium atoms from a cold surface and their subsequent detection using field ionization. When a dark matter particle scatters off a nucleus of the target material,…

Instrumentation and Methods for Astrophysics · Physics 2017-11-08 Humphrey J. Maris , George M. Seidel , Derek Stein

Dark photons are well motivated hypothetical dark sector particles that could account for observations that cannot be explained by the standard model of particle physics. A search for dark photons that are produced by an electron beam…

High Energy Physics - Phenomenology · Physics 2021-04-16 Seon-Hee Seo , Yeongduk Kim

Semiconductors are by now well-established targets for direct detection of MeV to GeV dark matter via scattering off electrons. We show that semiconductor targets can also detect significantly lighter dark matter via an absorption process.…

High Energy Physics - Phenomenology · Physics 2017-04-17 Yonit Hochberg , Tongyan Lin , Kathryn M. Zurek

Light dark matter with sub-eV masses has a high number density in our galaxy, and its scattering cross section with macroscopic objects can be significantly enhanced by coherence effects. Repeated scattering with a target object can induce…

High Energy Physics - Phenomenology · Physics 2026-03-31 Shigeki Matsumoto , Jie Sheng , Chuan-Yang Xing , Lin Zhu

Existing xenon dark matter (DM) direct detection experiments can probe the DM-nucleon interaction of DM with a sub-GeV mass through a search for photon emission from the recoiling xenon atom. We show that LUX's constraints on sub-GeV DM,…

High Energy Physics - Phenomenology · Physics 2017-08-23 Christopher McCabe

Hidden photons and axion-like particles are candidates for cold dark matter if they were produced non-thermally in the early universe. We conducted a search for both of these bosons using 800 live-days of data from the XMASS detector with…

Astrophysical dark matter particles with masses well below GeV-scale can be difficult to detect using conventional nuclear recoil experiments due to their low velocities in our Milky Way halo. Elastic scattering with high-energy cosmic rays…

High Energy Physics - Phenomenology · Physics 2026-04-21 Xiaoyong Chu , Yue-Lin Sming Tsai , Mei-Wen Yang

In the framework of an nonuniversal $U(1)'$ extension of the standard model, we propose an scalar candidate for cold dark matter which exhibits interactions with ordinary matter through Higgs and gauge bosons. Using limits from low energy…

High Energy Physics - Phenomenology · Physics 2014-11-07 R. Martinez , J. Nisperuza , F. Ochoa , J. P. Rubio

Dark photons, hypothesized to be sufficiently light and/or weakly interacting, offer a compelling candidate for dark matter. Their decay into three photons, referred to as the "dark photon trident" process, becomes the dominant channel when…

High Energy Physics - Phenomenology · Physics 2025-06-17 Thong T. Q. Nguyen

We revisit MSSM scenarios with light neutralino as a dark matter candidate in view of the latest LHC and dark matter direct and indirect detection experiments. We show that scenarios with a very light neutralino (~ 10 GeV) and a scalar…

High Energy Physics - Phenomenology · Physics 2013-11-08 Alexandre Arbey , Marco Battaglia , Farvah Mahmoudi

A number of new balloon or space-based $\gamma$-ray observatories have been proposed to close a "MeV gap" in sensitivity to $\gamma$ rays in the MeV-GeV energy band. One aspect of the science case for these instruments is their ability to…

High Energy Physics - Phenomenology · Physics 2025-04-29 Kayla E. O'Donnell , Tracy R. Slatyer

The last decade has seen unprecedented effort in dark matter model building at all mass scales coupled with the design of numerous new detection strategies. Transformative advances in quantum technologies have led to a plethora of new…

High Energy Physics - Experiment · Physics 2022-03-29 D. Antypas , A. Banerjee , C. Bartram , M. Baryakhtar , J. Betz , J. J. Bollinger , C. Boutan , D. Bowring , D. Budker , D. Carney , G. Carosi , S. Chaudhuri , S. Cheong , A. Chou , M. D. Chowdhury , R. T. Co , J. R. Crespo López-Urrutia , M. Demarteau , N. DePorzio , A. V. Derbin , T. Deshpande , M. D. Chowdhury , L. Di Luzio , A. Diaz-Morcillo , J. M. Doyle , A. Drlica-Wagner , A. Droster , N. Du , B. Döbrich , J. Eby , R. Essig , G. S. Farren , N. L. Figueroa , J. T. Fry , S. Gardner , A. A. Geraci , A. Ghalsasi , S. Ghosh , M. Giannotti , B. Gimeno , S. M. Griffin , D. Grin , D. Grin , H. Grote , J. H. Gundlach , M. Guzzetti , D. Hanneke , R. Harnik , R. Henning , V. Irsic , H. Jackson , D. F. Jackson Kimball , J. Jaeckel , M. Kagan , D. Kedar , R. Khatiwada , S. Knirck , S. Kolkowitz , T. Kovachy , S. E. Kuenstner , Z. Lasner , A. F. Leder , R. Lehnert , D. R. Leibrandt , E. Lentz , S. M. Lewis , Z. Liu , J. Manley , R. H. Maruyama , A. J. Millar , V. N. Muratova , N. Musoke , S. Nagaitsev , O. Noroozian , C. A. J. O'Hare , J. L. Ouellet , K. M. W. Pappas , E. Peik , G. Perez , A. Phipps , N. M. Rapidis , J. M. Robinson , V. H. Robles , K. K. Rogers , J. Rudolph , G. Rybka , M. Safdari , M. Safdari , M. S. Safronova , C. P. Salemi , P. O. Schmidt , T. Schumm , A. Schwartzman , J. Shu , M. Simanovskaia , J. Singh , S. Singh , M. S. Smith , W. M. Snow , Y. V. Stadnik , C. Sun , A. O. Sushkov , T. M. P. Tait , V. Takhistov , D. B. Tanner , D. J. Temples , P. G. Thirolf , J. H. Thomas , M. E. Tobar , O. Tretiak , Y. -D. Tsai , J. A. Tyson , M. Vandegar , S. Vermeulen , L. Visinelli , E. Vitagliano , Z. Wang , D. J. Wilson , L. Winslow , S. Withington , M. Wooten , J. Yang , J. Ye , B. A. Young , F. Yu , M. H. Zaheer , T. Zelevinsky , Y. Zhao , K. Zhou

Dark matter candidates arising in models of particle physics incorporating weak scale supersymmetry may produce detectable signals through their annihilation into neutrinos, photons, or positrons. A large number of relevant experiments are…

Astrophysics · Physics 2009-10-09 Jonathan L. Feng , Konstantin T. Matchev , Frank Wilczek

If dark matter consists of hidden-sector photons which kinetically mix with regular photons, a tiny oscillating electric-field component is present wherever we have dark matter. In the surface of conducting materials this induces a small…

Dark matter candidates with electromagnetic dipole moments can arise as dark baryons in gauge-mediated or technicolor models. These dark matter candidates interact with nuclei in direct detection experiments mainly through magnetic and/or…

High Energy Physics - Phenomenology · Physics 2010-08-04 Tom Banks , Jean-François Fortin , Scott Thomas

We consider the use of quantum-limited mechanical force sensors to detect ultralight (sub-meV) dark matter candidates which are weakly coupled to the standard model. We show that mechanical sensors with masses around or below the milligram…

High Energy Physics - Phenomenology · Physics 2021-03-12 Daniel Carney , Anson Hook , Zhen Liu , Jacob M. Taylor , Yue Zhao

The current generation of Dark Matter Direct Detection Experiments has ruled out a large region of parameter space for dark matter, particularly in the ($10 - 1000$) GeV mass range. However, due to very low event rates, searching for dark…

High Energy Physics - Phenomenology · Physics 2024-12-19 Praveen Bharadwaj , Ranjeet Kumar , Hemant Kumar Prajapati , Rahul Srivastava , Sushant Yadav

We calculate the terrestrial, astrophysical and cosmological constraints on a light vector boson that couples to an arbitrary combination of the electromagnetic and $B-L$ currents of the Standard Model. The dark photon and a vector boson…

High Energy Physics - Phenomenology · Physics 2026-02-27 Haidar Esseili , Graham D. Kribs

Direct-detection searches for dark matter are insensitive to dark matter particles that have large interactions with ordinary matter, which are stopped in the atmosphere or the Earth's crust before reaching terrestrial detectors. We use…

Cosmology and Nongalactic Astrophysics · Physics 2024-12-18 Peizhi Du , Rouven Essig , Bernard J. Rauscher , Hailin Xu
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